Physics Book - User contributions [en]

Potential Energy of a Multiparticle System

2016-11-28T04:45:12Z

Pepper: /* References */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.
<div style="text-align: center;">
[[File:Balldropping.gif]]
</div>

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
<div style="text-align: center;">
[[File:Sun_earth_orbit.png]]
</div>

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.
<div style="text-align: center;">
[[File:Electricz.jpg]]
</div>

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
<div style="text-align: center;">
[[File:Spring.jpg]]
</div>

===A Computational Model===
The following is a code segment to compute the spring potential energy, gravitational energy, and the total energy of a spring-ball multiparticle system in which one end of the spring is attached to the ceiling and the other end is attached to a ball.
<code>
L=ball.pos-ceiling.pos
s=mag(L)-L0
unitL=L/mag(L)
Fspring=-ks*s*unitL
Fgrav=mball*g*vector(0,-1,0)

## calculate net force on ball (note: has two contributions)
Fnet = Fspring + Fgrav

## apply momentum principle
ball.p=ball.p+Fnet*deltat
## update position
ball.pos=ball.pos+ball.p/mball * deltat
## update axis of spring
spring.axis=ball.pos-ceiling.pos

# kinetic energy of the ball
ball.v = ball.p / mball
K_ball = 0.5 * mball * (mag(ball.v))**2

# potential energy of spring
U_ball = 0.5 * ks * s**2

# potential energy of gravity
U_gravity = mball*g*ball.pos.y

# total energy
E_tot = K_ball + U_ball + U_gravity

# plot energy graphs
U_graph.plot(pos=(t,U_ball + U_gravity)) #Potential energy as a function of time
K_graph.plot(pos=(t,K_ball)) #Kinetic energy as a function of time
Energy_graph.plot(pos=(t,E_tot)) #Total energy as a function of time
</code>

==Examples==
Refer to the above section for detailed examples to compute potential energies for a multiparticle system in different contexts.

==Connectedness==
Potential energy is an important form of energy but overlooked sometimes. Understanding the significant of the potential energy gives me a clear understanding of real-world systems such as the ball-Earth system. Also, another important application is the spring potential energy which is prevalent in any systems that involves the use of spring.

== See also ==

If you haven't read this wiki page, you should check it [https://en.wikipedia.org/wiki/Potential_energy] out. Also, this is another related article [http://hyperphysics.phy-astr.gsu.edu/hbase/pegrav.html] that has detailed examples and explanations on how to compute the potential energies in different systems.

===Further reading===
The book '''Matter & Interactions''' by Ruth W. Chabay and Bruce A. Sherwood provides a nice reading on this topic [https://www.amazon.com/Matter-Interactions-Ruth-W-Chabay/dp/1118875869/ref=sr_1_1?ie=UTF8&qid=1480308086&sr=8-1&keywords=matters+and+interactions].

===External links===
Related discussion topics from University of Oregon [http://jersey.uoregon.edu/vlab/PotentialEnergy/].

A very nice video from Khan academic [https://www.khanacademy.org/science/physics/work-and-energy/hookes-law/v/potential-energy-stored-in-a-spring].

Another short video by Bozeman Science [https://www.youtube.com/watch?v=8a4D2xqHBF4].

==References==
http://shaikhshahin.blogspot.com/2015_09_01_archive.html

https://goo.gl/5kfLn8

https://www.youtube.com/watch?v=8a4D2xqHBF4

http://shaikhshahin.blogspot.com/2015_09_01_archive.html

https://www.khanacademy.org/science/physics/work-and-energy/hookes-law/v/potential-energy-stored-in-a-spring

Potential Energy of a Multiparticle System

2016-11-28T04:44:03Z

Pepper: /* References */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.
<div style="text-align: center;">
[[File:Balldropping.gif]]
</div>

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
<div style="text-align: center;">
[[File:Sun_earth_orbit.png]]
</div>

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.
<div style="text-align: center;">
[[File:Electricz.jpg]]
</div>

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
<div style="text-align: center;">
[[File:Spring.jpg]]
</div>

===A Computational Model===
The following is a code segment to compute the spring potential energy, gravitational energy, and the total energy of a spring-ball multiparticle system in which one end of the spring is attached to the ceiling and the other end is attached to a ball.
<code>
L=ball.pos-ceiling.pos
s=mag(L)-L0
unitL=L/mag(L)
Fspring=-ks*s*unitL
Fgrav=mball*g*vector(0,-1,0)

## calculate net force on ball (note: has two contributions)
Fnet = Fspring + Fgrav

## apply momentum principle
ball.p=ball.p+Fnet*deltat
## update position
ball.pos=ball.pos+ball.p/mball * deltat
## update axis of spring
spring.axis=ball.pos-ceiling.pos

# kinetic energy of the ball
ball.v = ball.p / mball
K_ball = 0.5 * mball * (mag(ball.v))**2

# potential energy of spring
U_ball = 0.5 * ks * s**2

# potential energy of gravity
U_gravity = mball*g*ball.pos.y

# total energy
E_tot = K_ball + U_ball + U_gravity

# plot energy graphs
U_graph.plot(pos=(t,U_ball + U_gravity)) #Potential energy as a function of time
K_graph.plot(pos=(t,K_ball)) #Kinetic energy as a function of time
Energy_graph.plot(pos=(t,E_tot)) #Total energy as a function of time
</code>

==Examples==
Refer to the above section for detailed examples to compute potential energies for a multiparticle system in different contexts.

==Connectedness==
Potential energy is an important form of energy but overlooked sometimes. Understanding the significant of the potential energy gives me a clear understanding of real-world systems such as the ball-Earth system. Also, another important application is the spring potential energy which is prevalent in any systems that involves the use of spring.

== See also ==

If you haven't read this wiki page, you should check it [https://en.wikipedia.org/wiki/Potential_energy] out. Also, this is another related article [http://hyperphysics.phy-astr.gsu.edu/hbase/pegrav.html] that has detailed examples and explanations on how to compute the potential energies in different systems.

===Further reading===
The book '''Matter & Interactions''' by Ruth W. Chabay and Bruce A. Sherwood provides a nice reading on this topic [https://www.amazon.com/Matter-Interactions-Ruth-W-Chabay/dp/1118875869/ref=sr_1_1?ie=UTF8&qid=1480308086&sr=8-1&keywords=matters+and+interactions].

===External links===
Related discussion topics from University of Oregon [http://jersey.uoregon.edu/vlab/PotentialEnergy/].

A very nice video from Khan academic [https://www.khanacademy.org/science/physics/work-and-energy/hookes-law/v/potential-energy-stored-in-a-spring].

Another short video by Bozeman Science [https://www.youtube.com/watch?v=8a4D2xqHBF4].

==References==
http://shaikhshahin.blogspot.com/2015_09_01_archive.html

https://www.amazon.com/Matter-Interactions-Ruth-W-Chabay/dp/1118875869/ref=sr_1_1?ie=UTF8&qid=1480308086&sr=8-1&keywords=matters+and+interactions

https://www.youtube.com/watch?v=8a4D2xqHBF4

http://shaikhshahin.blogspot.com/2015_09_01_archive.html

https://www.khanacademy.org/science/physics/work-and-energy/hookes-law/v/potential-energy-stored-in-a-spring

Potential Energy of a Multiparticle System

2016-11-28T04:43:49Z

Pepper: /* References */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.
<div style="text-align: center;">
[[File:Balldropping.gif]]
</div>

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
<div style="text-align: center;">
[[File:Sun_earth_orbit.png]]
</div>

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.
<div style="text-align: center;">
[[File:Electricz.jpg]]
</div>

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
<div style="text-align: center;">
[[File:Spring.jpg]]
</div>

===A Computational Model===
The following is a code segment to compute the spring potential energy, gravitational energy, and the total energy of a spring-ball multiparticle system in which one end of the spring is attached to the ceiling and the other end is attached to a ball.
<code>
L=ball.pos-ceiling.pos
s=mag(L)-L0
unitL=L/mag(L)
Fspring=-ks*s*unitL
Fgrav=mball*g*vector(0,-1,0)

## calculate net force on ball (note: has two contributions)
Fnet = Fspring + Fgrav

## apply momentum principle
ball.p=ball.p+Fnet*deltat
## update position
ball.pos=ball.pos+ball.p/mball * deltat
## update axis of spring
spring.axis=ball.pos-ceiling.pos

# kinetic energy of the ball
ball.v = ball.p / mball
K_ball = 0.5 * mball * (mag(ball.v))**2

# potential energy of spring
U_ball = 0.5 * ks * s**2

# potential energy of gravity
U_gravity = mball*g*ball.pos.y

# total energy
E_tot = K_ball + U_ball + U_gravity

# plot energy graphs
U_graph.plot(pos=(t,U_ball + U_gravity)) #Potential energy as a function of time
K_graph.plot(pos=(t,K_ball)) #Kinetic energy as a function of time
Energy_graph.plot(pos=(t,E_tot)) #Total energy as a function of time
</code>

==Examples==
Refer to the above section for detailed examples to compute potential energies for a multiparticle system in different contexts.

==Connectedness==
Potential energy is an important form of energy but overlooked sometimes. Understanding the significant of the potential energy gives me a clear understanding of real-world systems such as the ball-Earth system. Also, another important application is the spring potential energy which is prevalent in any systems that involves the use of spring.

== See also ==

If you haven't read this wiki page, you should check it [https://en.wikipedia.org/wiki/Potential_energy] out. Also, this is another related article [http://hyperphysics.phy-astr.gsu.edu/hbase/pegrav.html] that has detailed examples and explanations on how to compute the potential energies in different systems.

===Further reading===
The book '''Matter & Interactions''' by Ruth W. Chabay and Bruce A. Sherwood provides a nice reading on this topic [https://www.amazon.com/Matter-Interactions-Ruth-W-Chabay/dp/1118875869/ref=sr_1_1?ie=UTF8&qid=1480308086&sr=8-1&keywords=matters+and+interactions].

===External links===
Related discussion topics from University of Oregon [http://jersey.uoregon.edu/vlab/PotentialEnergy/].

A very nice video from Khan academic [https://www.khanacademy.org/science/physics/work-and-energy/hookes-law/v/potential-energy-stored-in-a-spring].

Another short video by Bozeman Science [https://www.youtube.com/watch?v=8a4D2xqHBF4].

==References==
http://shaikhshahin.blogspot.com/2015_09_01_archive.html
https://www.amazon.com/Matter-Interactions-Ruth-W-Chabay/dp/1118875869/ref=sr_1_1?ie=UTF8&qid=1480308086&sr=8-1&keywords=matters+and+interactions
https://www.youtube.com/watch?v=8a4D2xqHBF4
http://shaikhshahin.blogspot.com/2015_09_01_archive.html
https://www.khanacademy.org/science/physics/work-and-energy/hookes-law/v/potential-energy-stored-in-a-spring

[[Category:Which Category did you place this in?]]

Potential Energy of a Multiparticle System

2016-11-28T04:42:23Z

Pepper: /* Further reading */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.
<div style="text-align: center;">
[[File:Balldropping.gif]]
</div>

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
<div style="text-align: center;">
[[File:Sun_earth_orbit.png]]
</div>

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.
<div style="text-align: center;">
[[File:Electricz.jpg]]
</div>

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
<div style="text-align: center;">
[[File:Spring.jpg]]
</div>

===A Computational Model===
The following is a code segment to compute the spring potential energy, gravitational energy, and the total energy of a spring-ball multiparticle system in which one end of the spring is attached to the ceiling and the other end is attached to a ball.
<code>
L=ball.pos-ceiling.pos
s=mag(L)-L0
unitL=L/mag(L)
Fspring=-ks*s*unitL
Fgrav=mball*g*vector(0,-1,0)

## calculate net force on ball (note: has two contributions)
Fnet = Fspring + Fgrav

## apply momentum principle
ball.p=ball.p+Fnet*deltat
## update position
ball.pos=ball.pos+ball.p/mball * deltat
## update axis of spring
spring.axis=ball.pos-ceiling.pos

# kinetic energy of the ball
ball.v = ball.p / mball
K_ball = 0.5 * mball * (mag(ball.v))**2

# potential energy of spring
U_ball = 0.5 * ks * s**2

# potential energy of gravity
U_gravity = mball*g*ball.pos.y

# total energy
E_tot = K_ball + U_ball + U_gravity

# plot energy graphs
U_graph.plot(pos=(t,U_ball + U_gravity)) #Potential energy as a function of time
K_graph.plot(pos=(t,K_ball)) #Kinetic energy as a function of time
Energy_graph.plot(pos=(t,E_tot)) #Total energy as a function of time
</code>

==Examples==
Refer to the above section for detailed examples to compute potential energies for a multiparticle system in different contexts.

==Connectedness==
Potential energy is an important form of energy but overlooked sometimes. Understanding the significant of the potential energy gives me a clear understanding of real-world systems such as the ball-Earth system. Also, another important application is the spring potential energy which is prevalent in any systems that involves the use of spring.

== See also ==

If you haven't read this wiki page, you should check it [https://en.wikipedia.org/wiki/Potential_energy] out. Also, this is another related article [http://hyperphysics.phy-astr.gsu.edu/hbase/pegrav.html] that has detailed examples and explanations on how to compute the potential energies in different systems.

===Further reading===
The book '''Matter & Interactions''' by Ruth W. Chabay and Bruce A. Sherwood provides a nice reading on this topic [https://www.amazon.com/Matter-Interactions-Ruth-W-Chabay/dp/1118875869/ref=sr_1_1?ie=UTF8&qid=1480308086&sr=8-1&keywords=matters+and+interactions].

===External links===
Related discussion topics from University of Oregon [http://jersey.uoregon.edu/vlab/PotentialEnergy/].

A very nice video from Khan academic [https://www.khanacademy.org/science/physics/work-and-energy/hookes-law/v/potential-energy-stored-in-a-spring].

Another short video by Bozeman Science [https://www.youtube.com/watch?v=8a4D2xqHBF4].

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

Potential Energy of a Multiparticle System

2016-11-28T04:42:10Z

Pepper: /* Further reading */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.
<div style="text-align: center;">
[[File:Balldropping.gif]]
</div>

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
<div style="text-align: center;">
[[File:Sun_earth_orbit.png]]
</div>

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.
<div style="text-align: center;">
[[File:Electricz.jpg]]
</div>

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
<div style="text-align: center;">
[[File:Spring.jpg]]
</div>

===A Computational Model===
The following is a code segment to compute the spring potential energy, gravitational energy, and the total energy of a spring-ball multiparticle system in which one end of the spring is attached to the ceiling and the other end is attached to a ball.
<code>
L=ball.pos-ceiling.pos
s=mag(L)-L0
unitL=L/mag(L)
Fspring=-ks*s*unitL
Fgrav=mball*g*vector(0,-1,0)

## calculate net force on ball (note: has two contributions)
Fnet = Fspring + Fgrav

## apply momentum principle
ball.p=ball.p+Fnet*deltat
## update position
ball.pos=ball.pos+ball.p/mball * deltat
## update axis of spring
spring.axis=ball.pos-ceiling.pos

# kinetic energy of the ball
ball.v = ball.p / mball
K_ball = 0.5 * mball * (mag(ball.v))**2

# potential energy of spring
U_ball = 0.5 * ks * s**2

# potential energy of gravity
U_gravity = mball*g*ball.pos.y

# total energy
E_tot = K_ball + U_ball + U_gravity

# plot energy graphs
U_graph.plot(pos=(t,U_ball + U_gravity)) #Potential energy as a function of time
K_graph.plot(pos=(t,K_ball)) #Kinetic energy as a function of time
Energy_graph.plot(pos=(t,E_tot)) #Total energy as a function of time
</code>

==Examples==
Refer to the above section for detailed examples to compute potential energies for a multiparticle system in different contexts.

==Connectedness==
Potential energy is an important form of energy but overlooked sometimes. Understanding the significant of the potential energy gives me a clear understanding of real-world systems such as the ball-Earth system. Also, another important application is the spring potential energy which is prevalent in any systems that involves the use of spring.

== See also ==

If you haven't read this wiki page, you should check it [https://en.wikipedia.org/wiki/Potential_energy] out. Also, this is another related article [http://hyperphysics.phy-astr.gsu.edu/hbase/pegrav.html] that has detailed examples and explanations on how to compute the potential energies in different systems.

===Further reading===
The book '''Matter & Interactions''' by by Ruth W. Chabay and Bruce A. Sherwood provides a nice reading on this topic [https://www.amazon.com/Matter-Interactions-Ruth-W-Chabay/dp/1118875869/ref=sr_1_1?ie=UTF8&qid=1480308086&sr=8-1&keywords=matters+and+interactions].

===External links===
Related discussion topics from University of Oregon [http://jersey.uoregon.edu/vlab/PotentialEnergy/].

A very nice video from Khan academic [https://www.khanacademy.org/science/physics/work-and-energy/hookes-law/v/potential-energy-stored-in-a-spring].

Another short video by Bozeman Science [https://www.youtube.com/watch?v=8a4D2xqHBF4].

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

Potential Energy of a Multiparticle System

2016-11-28T04:40:11Z

Pepper: /* External links */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.
<div style="text-align: center;">
[[File:Balldropping.gif]]
</div>

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
<div style="text-align: center;">
[[File:Sun_earth_orbit.png]]
</div>

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.
<div style="text-align: center;">
[[File:Electricz.jpg]]
</div>

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
<div style="text-align: center;">
[[File:Spring.jpg]]
</div>

===A Computational Model===
The following is a code segment to compute the spring potential energy, gravitational energy, and the total energy of a spring-ball multiparticle system in which one end of the spring is attached to the ceiling and the other end is attached to a ball.
<code>
L=ball.pos-ceiling.pos
s=mag(L)-L0
unitL=L/mag(L)
Fspring=-ks*s*unitL
Fgrav=mball*g*vector(0,-1,0)

## calculate net force on ball (note: has two contributions)
Fnet = Fspring + Fgrav

## apply momentum principle
ball.p=ball.p+Fnet*deltat
## update position
ball.pos=ball.pos+ball.p/mball * deltat
## update axis of spring
spring.axis=ball.pos-ceiling.pos

# kinetic energy of the ball
ball.v = ball.p / mball
K_ball = 0.5 * mball * (mag(ball.v))**2

# potential energy of spring
U_ball = 0.5 * ks * s**2

# potential energy of gravity
U_gravity = mball*g*ball.pos.y

# total energy
E_tot = K_ball + U_ball + U_gravity

# plot energy graphs
U_graph.plot(pos=(t,U_ball + U_gravity)) #Potential energy as a function of time
K_graph.plot(pos=(t,K_ball)) #Kinetic energy as a function of time
Energy_graph.plot(pos=(t,E_tot)) #Total energy as a function of time
</code>

==Examples==
Refer to the above section for detailed examples to compute potential energies for a multiparticle system in different contexts.

==Connectedness==
Potential energy is an important form of energy but overlooked sometimes. Understanding the significant of the potential energy gives me a clear understanding of real-world systems such as the ball-Earth system. Also, another important application is the spring potential energy which is prevalent in any systems that involves the use of spring.

== See also ==

If you haven't read this wiki page, you should check it [https://en.wikipedia.org/wiki/Potential_energy] out. Also, this is another related article [http://hyperphysics.phy-astr.gsu.edu/hbase/pegrav.html] that has detailed examples and explanations on how to compute the potential energies in different systems.

===Further reading===
[http://jersey.uoregon.edu/vlab/PotentialEnergy/]

===External links===
Related discussion topics from University of Oregon [http://jersey.uoregon.edu/vlab/PotentialEnergy/].

A very nice video from Khan academic [https://www.khanacademy.org/science/physics/work-and-energy/hookes-law/v/potential-energy-stored-in-a-spring].

Another short video by Bozeman Science [https://www.youtube.com/watch?v=8a4D2xqHBF4].

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

Potential Energy of a Multiparticle System

2016-11-28T04:39:57Z

Pepper: /* External links */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.
<div style="text-align: center;">
[[File:Balldropping.gif]]
</div>

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
<div style="text-align: center;">
[[File:Sun_earth_orbit.png]]
</div>

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.
<div style="text-align: center;">
[[File:Electricz.jpg]]
</div>

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
<div style="text-align: center;">
[[File:Spring.jpg]]
</div>

===A Computational Model===
The following is a code segment to compute the spring potential energy, gravitational energy, and the total energy of a spring-ball multiparticle system in which one end of the spring is attached to the ceiling and the other end is attached to a ball.
<code>
L=ball.pos-ceiling.pos
s=mag(L)-L0
unitL=L/mag(L)
Fspring=-ks*s*unitL
Fgrav=mball*g*vector(0,-1,0)

## calculate net force on ball (note: has two contributions)
Fnet = Fspring + Fgrav

## apply momentum principle
ball.p=ball.p+Fnet*deltat
## update position
ball.pos=ball.pos+ball.p/mball * deltat
## update axis of spring
spring.axis=ball.pos-ceiling.pos

# kinetic energy of the ball
ball.v = ball.p / mball
K_ball = 0.5 * mball * (mag(ball.v))**2

# potential energy of spring
U_ball = 0.5 * ks * s**2

# potential energy of gravity
U_gravity = mball*g*ball.pos.y

# total energy
E_tot = K_ball + U_ball + U_gravity

# plot energy graphs
U_graph.plot(pos=(t,U_ball + U_gravity)) #Potential energy as a function of time
K_graph.plot(pos=(t,K_ball)) #Kinetic energy as a function of time
Energy_graph.plot(pos=(t,E_tot)) #Total energy as a function of time
</code>

==Examples==
Refer to the above section for detailed examples to compute potential energies for a multiparticle system in different contexts.

==Connectedness==
Potential energy is an important form of energy but overlooked sometimes. Understanding the significant of the potential energy gives me a clear understanding of real-world systems such as the ball-Earth system. Also, another important application is the spring potential energy which is prevalent in any systems that involves the use of spring.

== See also ==

If you haven't read this wiki page, you should check it [https://en.wikipedia.org/wiki/Potential_energy] out. Also, this is another related article [http://hyperphysics.phy-astr.gsu.edu/hbase/pegrav.html] that has detailed examples and explanations on how to compute the potential energies in different systems.

===Further reading===
[http://jersey.uoregon.edu/vlab/PotentialEnergy/]

===External links===
Related discussion topics from University of Oregon [http://jersey.uoregon.edu/vlab/PotentialEnergy/].
A very nice video from Khan academic [https://www.khanacademy.org/science/physics/work-and-energy/hookes-law/v/potential-energy-stored-in-a-spring].
Another short video by Bozeman Science [https://www.youtube.com/watch?v=8a4D2xqHBF4].

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

Potential Energy of a Multiparticle System

2016-11-28T04:37:50Z

Pepper: /* Further reading */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.
<div style="text-align: center;">
[[File:Balldropping.gif]]
</div>

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
<div style="text-align: center;">
[[File:Sun_earth_orbit.png]]
</div>

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.
<div style="text-align: center;">
[[File:Electricz.jpg]]
</div>

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
<div style="text-align: center;">
[[File:Spring.jpg]]
</div>

===A Computational Model===
The following is a code segment to compute the spring potential energy, gravitational energy, and the total energy of a spring-ball multiparticle system in which one end of the spring is attached to the ceiling and the other end is attached to a ball.
<code>
L=ball.pos-ceiling.pos
s=mag(L)-L0
unitL=L/mag(L)
Fspring=-ks*s*unitL
Fgrav=mball*g*vector(0,-1,0)

## calculate net force on ball (note: has two contributions)
Fnet = Fspring + Fgrav

## apply momentum principle
ball.p=ball.p+Fnet*deltat
## update position
ball.pos=ball.pos+ball.p/mball * deltat
## update axis of spring
spring.axis=ball.pos-ceiling.pos

# kinetic energy of the ball
ball.v = ball.p / mball
K_ball = 0.5 * mball * (mag(ball.v))**2

# potential energy of spring
U_ball = 0.5 * ks * s**2

# potential energy of gravity
U_gravity = mball*g*ball.pos.y

# total energy
E_tot = K_ball + U_ball + U_gravity

# plot energy graphs
U_graph.plot(pos=(t,U_ball + U_gravity)) #Potential energy as a function of time
K_graph.plot(pos=(t,K_ball)) #Kinetic energy as a function of time
Energy_graph.plot(pos=(t,E_tot)) #Total energy as a function of time
</code>

==Examples==
Refer to the above section for detailed examples to compute potential energies for a multiparticle system in different contexts.

==Connectedness==
Potential energy is an important form of energy but overlooked sometimes. Understanding the significant of the potential energy gives me a clear understanding of real-world systems such as the ball-Earth system. Also, another important application is the spring potential energy which is prevalent in any systems that involves the use of spring.

== See also ==

If you haven't read this wiki page, you should check it [https://en.wikipedia.org/wiki/Potential_energy] out. Also, this is another related article [http://hyperphysics.phy-astr.gsu.edu/hbase/pegrav.html] that has detailed examples and explanations on how to compute the potential energies in different systems.

===Further reading===
[http://jersey.uoregon.edu/vlab/PotentialEnergy/]

===External links===

Internet resources on this topic

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

Potential Energy of a Multiparticle System

2016-11-28T04:36:57Z

Pepper: /* Connectedness */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.
<div style="text-align: center;">
[[File:Balldropping.gif]]
</div>

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
<div style="text-align: center;">
[[File:Sun_earth_orbit.png]]
</div>

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.
<div style="text-align: center;">
[[File:Electricz.jpg]]
</div>

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
<div style="text-align: center;">
[[File:Spring.jpg]]
</div>

===A Computational Model===
The following is a code segment to compute the spring potential energy, gravitational energy, and the total energy of a spring-ball multiparticle system in which one end of the spring is attached to the ceiling and the other end is attached to a ball.
<code>
L=ball.pos-ceiling.pos
s=mag(L)-L0
unitL=L/mag(L)
Fspring=-ks*s*unitL
Fgrav=mball*g*vector(0,-1,0)

## calculate net force on ball (note: has two contributions)
Fnet = Fspring + Fgrav

## apply momentum principle
ball.p=ball.p+Fnet*deltat
## update position
ball.pos=ball.pos+ball.p/mball * deltat
## update axis of spring
spring.axis=ball.pos-ceiling.pos

# kinetic energy of the ball
ball.v = ball.p / mball
K_ball = 0.5 * mball * (mag(ball.v))**2

# potential energy of spring
U_ball = 0.5 * ks * s**2

# potential energy of gravity
U_gravity = mball*g*ball.pos.y

# total energy
E_tot = K_ball + U_ball + U_gravity

# plot energy graphs
U_graph.plot(pos=(t,U_ball + U_gravity)) #Potential energy as a function of time
K_graph.plot(pos=(t,K_ball)) #Kinetic energy as a function of time
Energy_graph.plot(pos=(t,E_tot)) #Total energy as a function of time
</code>

==Examples==
Refer to the above section for detailed examples to compute potential energies for a multiparticle system in different contexts.

==Connectedness==
Potential energy is an important form of energy but overlooked sometimes. Understanding the significant of the potential energy gives me a clear understanding of real-world systems such as the ball-Earth system. Also, another important application is the spring potential energy which is prevalent in any systems that involves the use of spring.

== See also ==

If you haven't read this wiki page, you should check it [https://en.wikipedia.org/wiki/Potential_energy] out. Also, this is another related article [http://hyperphysics.phy-astr.gsu.edu/hbase/pegrav.html] that has detailed examples and explanations on how to compute the potential energies in different systems.

===Further reading===

Books, Articles or other print media on this topic

===External links===

Internet resources on this topic

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

Potential Energy of a Multiparticle System

2016-11-28T04:36:36Z

Pepper: /* History */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.
<div style="text-align: center;">
[[File:Balldropping.gif]]
</div>

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
<div style="text-align: center;">
[[File:Sun_earth_orbit.png]]
</div>

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.
<div style="text-align: center;">
[[File:Electricz.jpg]]
</div>

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
<div style="text-align: center;">
[[File:Spring.jpg]]
</div>

===A Computational Model===
The following is a code segment to compute the spring potential energy, gravitational energy, and the total energy of a spring-ball multiparticle system in which one end of the spring is attached to the ceiling and the other end is attached to a ball.
<code>
L=ball.pos-ceiling.pos
s=mag(L)-L0
unitL=L/mag(L)
Fspring=-ks*s*unitL
Fgrav=mball*g*vector(0,-1,0)

## calculate net force on ball (note: has two contributions)
Fnet = Fspring + Fgrav

## apply momentum principle
ball.p=ball.p+Fnet*deltat
## update position
ball.pos=ball.pos+ball.p/mball * deltat
## update axis of spring
spring.axis=ball.pos-ceiling.pos

# kinetic energy of the ball
ball.v = ball.p / mball
K_ball = 0.5 * mball * (mag(ball.v))**2

# potential energy of spring
U_ball = 0.5 * ks * s**2

# potential energy of gravity
U_gravity = mball*g*ball.pos.y

# total energy
E_tot = K_ball + U_ball + U_gravity

# plot energy graphs
U_graph.plot(pos=(t,U_ball + U_gravity)) #Potential energy as a function of time
K_graph.plot(pos=(t,K_ball)) #Kinetic energy as a function of time
Energy_graph.plot(pos=(t,E_tot)) #Total energy as a function of time
</code>

==Examples==
Refer to the above section for detailed examples to compute potential energies for a multiparticle system in different contexts.

==Connectedness==
Potential energy is an important form of energy but overlooked sometimes. Understanding the significant of the potential energy gives me a clear understanding of real-world systems such as the ball-Earth system. Also, another important application is the spring potential energy which is prevalent in any systems that involves the use of spring.

#==History==

#Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.

== See also ==

If you haven't read this wiki page, you should check it [https://en.wikipedia.org/wiki/Potential_energy] out. Also, this is another related article [http://hyperphysics.phy-astr.gsu.edu/hbase/pegrav.html] that has detailed examples and explanations on how to compute the potential energies in different systems.

===Further reading===

Books, Articles or other print media on this topic

===External links===

Internet resources on this topic

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

Potential Energy of a Multiparticle System

2016-11-28T04:36:19Z

Pepper: /* See also */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.
<div style="text-align: center;">
[[File:Balldropping.gif]]
</div>

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
<div style="text-align: center;">
[[File:Sun_earth_orbit.png]]
</div>

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.
<div style="text-align: center;">
[[File:Electricz.jpg]]
</div>

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
<div style="text-align: center;">
[[File:Spring.jpg]]
</div>

===A Computational Model===
The following is a code segment to compute the spring potential energy, gravitational energy, and the total energy of a spring-ball multiparticle system in which one end of the spring is attached to the ceiling and the other end is attached to a ball.
<code>
L=ball.pos-ceiling.pos
s=mag(L)-L0
unitL=L/mag(L)
Fspring=-ks*s*unitL
Fgrav=mball*g*vector(0,-1,0)

## calculate net force on ball (note: has two contributions)
Fnet = Fspring + Fgrav

## apply momentum principle
ball.p=ball.p+Fnet*deltat
## update position
ball.pos=ball.pos+ball.p/mball * deltat
## update axis of spring
spring.axis=ball.pos-ceiling.pos

# kinetic energy of the ball
ball.v = ball.p / mball
K_ball = 0.5 * mball * (mag(ball.v))**2

# potential energy of spring
U_ball = 0.5 * ks * s**2

# potential energy of gravity
U_gravity = mball*g*ball.pos.y

# total energy
E_tot = K_ball + U_ball + U_gravity

# plot energy graphs
U_graph.plot(pos=(t,U_ball + U_gravity)) #Potential energy as a function of time
K_graph.plot(pos=(t,K_ball)) #Kinetic energy as a function of time
Energy_graph.plot(pos=(t,E_tot)) #Total energy as a function of time
</code>

==Examples==
Refer to the above section for detailed examples to compute potential energies for a multiparticle system in different contexts.

==Connectedness==
Potential energy is an important form of energy but overlooked sometimes. Understanding the significant of the potential energy gives me a clear understanding of real-world systems such as the ball-Earth system. Also, another important application is the spring potential energy which is prevalent in any systems that involves the use of spring.

==History==

Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.

== See also ==

If you haven't read this wiki page, you should check it [https://en.wikipedia.org/wiki/Potential_energy] out. Also, this is another related article [http://hyperphysics.phy-astr.gsu.edu/hbase/pegrav.html] that has detailed examples and explanations on how to compute the potential energies in different systems.

===Further reading===

Books, Articles or other print media on this topic

===External links===

Internet resources on this topic

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

Potential Energy of a Multiparticle System

2016-11-28T04:34:40Z

Pepper: /* See also */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.
<div style="text-align: center;">
[[File:Balldropping.gif]]
</div>

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
<div style="text-align: center;">
[[File:Sun_earth_orbit.png]]
</div>

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.
<div style="text-align: center;">
[[File:Electricz.jpg]]
</div>

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
<div style="text-align: center;">
[[File:Spring.jpg]]
</div>

===A Computational Model===
The following is a code segment to compute the spring potential energy, gravitational energy, and the total energy of a spring-ball multiparticle system in which one end of the spring is attached to the ceiling and the other end is attached to a ball.
<code>
L=ball.pos-ceiling.pos
s=mag(L)-L0
unitL=L/mag(L)
Fspring=-ks*s*unitL
Fgrav=mball*g*vector(0,-1,0)

## calculate net force on ball (note: has two contributions)
Fnet = Fspring + Fgrav

## apply momentum principle
ball.p=ball.p+Fnet*deltat
## update position
ball.pos=ball.pos+ball.p/mball * deltat
## update axis of spring
spring.axis=ball.pos-ceiling.pos

# kinetic energy of the ball
ball.v = ball.p / mball
K_ball = 0.5 * mball * (mag(ball.v))**2

# potential energy of spring
U_ball = 0.5 * ks * s**2

# potential energy of gravity
U_gravity = mball*g*ball.pos.y

# total energy
E_tot = K_ball + U_ball + U_gravity

# plot energy graphs
U_graph.plot(pos=(t,U_ball + U_gravity)) #Potential energy as a function of time
K_graph.plot(pos=(t,K_ball)) #Kinetic energy as a function of time
Energy_graph.plot(pos=(t,E_tot)) #Total energy as a function of time
</code>

==Examples==
Refer to the above section for detailed examples to compute potential energies for a multiparticle system in different contexts.

==Connectedness==
Potential energy is an important form of energy but overlooked sometimes. Understanding the significant of the potential energy gives me a clear understanding of real-world systems such as the ball-Earth system. Also, another important application is the spring potential energy which is prevalent in any systems that involves the use of spring.

==History==

Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.

== See also ==

If you haven't read this wiki page, you should check it [https://en.wikipedia.org/wiki/Potential_energy] out.

===Further reading===

Books, Articles or other print media on this topic

===External links===

Internet resources on this topic

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

Potential Energy of a Multiparticle System

2016-11-28T04:32:26Z

Pepper: /* Connectedness */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.
<div style="text-align: center;">
[[File:Balldropping.gif]]
</div>

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
<div style="text-align: center;">
[[File:Sun_earth_orbit.png]]
</div>

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.
<div style="text-align: center;">
[[File:Electricz.jpg]]
</div>

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
<div style="text-align: center;">
[[File:Spring.jpg]]
</div>

===A Computational Model===
The following is a code segment to compute the spring potential energy, gravitational energy, and the total energy of a spring-ball multiparticle system in which one end of the spring is attached to the ceiling and the other end is attached to a ball.
<code>
L=ball.pos-ceiling.pos
s=mag(L)-L0
unitL=L/mag(L)
Fspring=-ks*s*unitL
Fgrav=mball*g*vector(0,-1,0)

## calculate net force on ball (note: has two contributions)
Fnet = Fspring + Fgrav

## apply momentum principle
ball.p=ball.p+Fnet*deltat
## update position
ball.pos=ball.pos+ball.p/mball * deltat
## update axis of spring
spring.axis=ball.pos-ceiling.pos

# kinetic energy of the ball
ball.v = ball.p / mball
K_ball = 0.5 * mball * (mag(ball.v))**2

# potential energy of spring
U_ball = 0.5 * ks * s**2

# potential energy of gravity
U_gravity = mball*g*ball.pos.y

# total energy
E_tot = K_ball + U_ball + U_gravity

# plot energy graphs
U_graph.plot(pos=(t,U_ball + U_gravity)) #Potential energy as a function of time
K_graph.plot(pos=(t,K_ball)) #Kinetic energy as a function of time
Energy_graph.plot(pos=(t,E_tot)) #Total energy as a function of time
</code>

==Examples==
Refer to the above section for detailed examples to compute potential energies for a multiparticle system in different contexts.

==Connectedness==
Potential energy is an important form of energy but overlooked sometimes. Understanding the significant of the potential energy gives me a clear understanding of real-world systems such as the ball-Earth system. Also, another important application is the spring potential energy which is prevalent in any systems that involves the use of spring.

==History==

Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.

== See also ==

Are there related topics or categories in this wiki resource for the curious reader to explore? How does this topic fit into that context?

===Further reading===

Books, Articles or other print media on this topic

===External links===

Internet resources on this topic

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

Potential Energy of a Multiparticle System

2016-11-28T04:31:12Z

Pepper: /* Connectedness */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.
<div style="text-align: center;">
[[File:Balldropping.gif]]
</div>

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
<div style="text-align: center;">
[[File:Sun_earth_orbit.png]]
</div>

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.
<div style="text-align: center;">
[[File:Electricz.jpg]]
</div>

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
<div style="text-align: center;">
[[File:Spring.jpg]]
</div>

===A Computational Model===
The following is a code segment to compute the spring potential energy, gravitational energy, and the total energy of a spring-ball multiparticle system in which one end of the spring is attached to the ceiling and the other end is attached to a ball.
<code>
L=ball.pos-ceiling.pos
s=mag(L)-L0
unitL=L/mag(L)
Fspring=-ks*s*unitL
Fgrav=mball*g*vector(0,-1,0)

## calculate net force on ball (note: has two contributions)
Fnet = Fspring + Fgrav

## apply momentum principle
ball.p=ball.p+Fnet*deltat
## update position
ball.pos=ball.pos+ball.p/mball * deltat
## update axis of spring
spring.axis=ball.pos-ceiling.pos

# kinetic energy of the ball
ball.v = ball.p / mball
K_ball = 0.5 * mball * (mag(ball.v))**2

# potential energy of spring
U_ball = 0.5 * ks * s**2

# potential energy of gravity
U_gravity = mball*g*ball.pos.y

# total energy
E_tot = K_ball + U_ball + U_gravity

# plot energy graphs
U_graph.plot(pos=(t,U_ball + U_gravity)) #Potential energy as a function of time
K_graph.plot(pos=(t,K_ball)) #Kinetic energy as a function of time
Energy_graph.plot(pos=(t,E_tot)) #Total energy as a function of time
</code>

==Examples==
Refer to the above section for detailed examples to compute potential energies for a multiparticle system in different contexts.

==Connectedness==
Potential energy is an important form of energy but overlooked sometimes. Understanding the significant of the potential energy gives me a clear understanding of real-world systems such as the ball-Earth system. Another important application is the spring potential energy which is prevalent in any systems that involves the use of spring.

==History==

Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.

== See also ==

Are there related topics or categories in this wiki resource for the curious reader to explore? How does this topic fit into that context?

===Further reading===

Books, Articles or other print media on this topic

===External links===

Internet resources on this topic

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

Potential Energy of a Multiparticle System

2016-11-28T04:26:43Z

Pepper: /* Examples */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.
<div style="text-align: center;">
[[File:Balldropping.gif]]
</div>

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
<div style="text-align: center;">
[[File:Sun_earth_orbit.png]]
</div>

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.
<div style="text-align: center;">
[[File:Electricz.jpg]]
</div>

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
<div style="text-align: center;">
[[File:Spring.jpg]]
</div>

===A Computational Model===
The following is a code segment to compute the spring potential energy, gravitational energy, and the total energy of a spring-ball multiparticle system in which one end of the spring is attached to the ceiling and the other end is attached to a ball.
<code>
L=ball.pos-ceiling.pos
s=mag(L)-L0
unitL=L/mag(L)
Fspring=-ks*s*unitL
Fgrav=mball*g*vector(0,-1,0)

## calculate net force on ball (note: has two contributions)
Fnet = Fspring + Fgrav

## apply momentum principle
ball.p=ball.p+Fnet*deltat
## update position
ball.pos=ball.pos+ball.p/mball * deltat
## update axis of spring
spring.axis=ball.pos-ceiling.pos

# kinetic energy of the ball
ball.v = ball.p / mball
K_ball = 0.5 * mball * (mag(ball.v))**2

# potential energy of spring
U_ball = 0.5 * ks * s**2

# potential energy of gravity
U_gravity = mball*g*ball.pos.y

# total energy
E_tot = K_ball + U_ball + U_gravity

# plot energy graphs
U_graph.plot(pos=(t,U_ball + U_gravity)) #Potential energy as a function of time
K_graph.plot(pos=(t,K_ball)) #Kinetic energy as a function of time
Energy_graph.plot(pos=(t,E_tot)) #Total energy as a function of time
</code>

==Examples==
Refer to the above section for detailed examples to compute potential energies for a multiparticle system in different contexts.

==Connectedness==
#How is this topic connected to something that you are interested in?
#How is it connected to your major?
#Is there an interesting industrial application?

==History==

Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.

== See also ==

Are there related topics or categories in this wiki resource for the curious reader to explore? How does this topic fit into that context?

===Further reading===

Books, Articles or other print media on this topic

===External links===

Internet resources on this topic

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

Potential Energy of a Multiparticle System

2016-11-28T04:25:17Z

Pepper: /* A Computational Model */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.
<div style="text-align: center;">
[[File:Balldropping.gif]]
</div>

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
<div style="text-align: center;">
[[File:Sun_earth_orbit.png]]
</div>

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.
<div style="text-align: center;">
[[File:Electricz.jpg]]
</div>

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
<div style="text-align: center;">
[[File:Spring.jpg]]
</div>

===A Computational Model===
The following is a code segment to compute the spring potential energy, gravitational energy, and the total energy of a spring-ball multiparticle system in which one end of the spring is attached to the ceiling and the other end is attached to a ball.
<code>
L=ball.pos-ceiling.pos
s=mag(L)-L0
unitL=L/mag(L)
Fspring=-ks*s*unitL
Fgrav=mball*g*vector(0,-1,0)

## calculate net force on ball (note: has two contributions)
Fnet = Fspring + Fgrav

## apply momentum principle
ball.p=ball.p+Fnet*deltat
## update position
ball.pos=ball.pos+ball.p/mball * deltat
## update axis of spring
spring.axis=ball.pos-ceiling.pos

# kinetic energy of the ball
ball.v = ball.p / mball
K_ball = 0.5 * mball * (mag(ball.v))**2

# potential energy of spring
U_ball = 0.5 * ks * s**2

# potential energy of gravity
U_gravity = mball*g*ball.pos.y

# total energy
E_tot = K_ball + U_ball + U_gravity

# plot energy graphs
U_graph.plot(pos=(t,U_ball + U_gravity)) #Potential energy as a function of time
K_graph.plot(pos=(t,K_ball)) #Kinetic energy as a function of time
Energy_graph.plot(pos=(t,E_tot)) #Total energy as a function of time
</code>

==Examples==

Be sure to show all steps in your solution and include diagrams whenever possible

===Simple===
===Middling===
===Difficult===

==Connectedness==
#How is this topic connected to something that you are interested in?
#How is it connected to your major?
#Is there an interesting industrial application?

==History==

Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.

== See also ==

Are there related topics or categories in this wiki resource for the curious reader to explore? How does this topic fit into that context?

===Further reading===

Books, Articles or other print media on this topic

===External links===

Internet resources on this topic

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

Potential Energy of a Multiparticle System

2016-11-28T04:24:05Z

Pepper: /* A Computational Model */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.
<div style="text-align: center;">
[[File:Balldropping.gif]]
</div>

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
<div style="text-align: center;">
[[File:Sun_earth_orbit.png]]
</div>

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.
<div style="text-align: center;">
[[File:Electricz.jpg]]
</div>

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
<div style="text-align: center;">
[[File:Spring.jpg]]
</div>

===A Computational Model===
The following is a code segment to compute the spring potential energy, gravitational energy, and the total energy of a spring-ball multiparticle system in which one end of the spring is attached to the ceiling and the other end is attached to a ball.
<code>
L=ball.pos-ceiling.pos
s=mag(L)-L0
unitL=L/mag(L)
Fspring=-ks*s*unitL
## calculate net force on ball (note: has two contributions)
Fgrav=mball*g*vector(0,-1,0)

# viscous drag
b = 6 * pi * bn * ball.radius
#b = 0
Fviscous = -1*b*ball.v
#Fnet=Fspring+Fgrav
Fnet = Fspring + Fgrav + Fviscous

## apply momentum principle
ball.p=ball.p+Fnet*deltat
## update position
ball.pos=ball.pos+ball.p/mball * deltat
## update axis of spring
spring.axis=ball.pos-ceiling.pos

# kinetic energy of the ball
ball.v = ball.p / mball
K_ball = 0.5 * mball * (mag(ball.v))**2

# potential energy of spring
U_ball = 0.5 * ks * s**2

# potential energy of gravity
U_gravity = mball*g*ball.pos.y

# total energy
E_tot = K_ball + U_ball + U_gravity

# plot energy graphs
U_graph.plot(pos=(t,U_ball + U_gravity)) #Potential energy as a function of time
K_graph.plot(pos=(t,K_ball)) #Kinetic energy as a function of time
Energy_graph.plot(pos=(t,E_tot)) #Total energy as a function of time
</code>

==Examples==

Be sure to show all steps in your solution and include diagrams whenever possible

===Simple===
===Middling===
===Difficult===

==Connectedness==
#How is this topic connected to something that you are interested in?
#How is it connected to your major?
#Is there an interesting industrial application?

==History==

Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.

== See also ==

Are there related topics or categories in this wiki resource for the curious reader to explore? How does this topic fit into that context?

===Further reading===

Books, Articles or other print media on this topic

===External links===

Internet resources on this topic

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

Potential Energy of a Multiparticle System

2016-11-28T04:18:16Z

Pepper: /* The Main Idea */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.
<div style="text-align: center;">
[[File:Balldropping.gif]]
</div>

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
<div style="text-align: center;">
[[File:Sun_earth_orbit.png]]
</div>

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.
<div style="text-align: center;">
[[File:Electricz.jpg]]
</div>

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
<div style="text-align: center;">
[[File:Spring.jpg]]
</div>

===A Computational Model===

How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]

==Examples==

Be sure to show all steps in your solution and include diagrams whenever possible

===Simple===
===Middling===
===Difficult===

==Connectedness==
#How is this topic connected to something that you are interested in?
#How is it connected to your major?
#Is there an interesting industrial application?

==History==

Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.

== See also ==

Are there related topics or categories in this wiki resource for the curious reader to explore? How does this topic fit into that context?

===Further reading===

Books, Articles or other print media on this topic

===External links===

Internet resources on this topic

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

File:Balldropping.gif

2016-11-28T04:17:34Z

Pepper: http://shaikhshahin.blogspot.com/2015_09_01_archive.html

http://shaikhshahin.blogspot.com/2015_09_01_archive.html

Potential Energy of a Multiparticle System

2016-11-28T04:14:01Z

Pepper: /* A Mathematical Model */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
<div style="text-align: center;">
[[File:Sun_earth_orbit.png]]
</div>

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.
<div style="text-align: center;">
[[File:Electricz.jpg]]
</div>

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
<div style="text-align: center;">
[[File:Spring.jpg]]
</div>

===A Computational Model===

How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]

==Examples==

Be sure to show all steps in your solution and include diagrams whenever possible

===Simple===
===Middling===
===Difficult===

==Connectedness==
#How is this topic connected to something that you are interested in?
#How is it connected to your major?
#Is there an interesting industrial application?

==History==

Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.

== See also ==

Are there related topics or categories in this wiki resource for the curious reader to explore? How does this topic fit into that context?

===Further reading===

Books, Articles or other print media on this topic

===External links===

Internet resources on this topic

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

Potential Energy of a Multiparticle System

2016-11-28T04:13:13Z

Pepper: /* A Mathematical Model */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
<div style="text-align: center;">
[[File:Sun_earth_orbit.png]]
</div>

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.
<div style="text-align: center;">
[[File:Electricz.jpg]]
</div>

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
<div style="text-align: center;">
[[File:Spring.jpg]]
</div>

What are the mathematical equations that allow us to model this topic. For example <math>{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}</math> where '''p''' is the momentum of the system and '''F''' is the net force from the surroundings.

===A Computational Model===

How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]

==Examples==

Be sure to show all steps in your solution and include diagrams whenever possible

===Simple===
===Middling===
===Difficult===

==Connectedness==
#How is this topic connected to something that you are interested in?
#How is it connected to your major?
#Is there an interesting industrial application?

==History==

Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.

== See also ==

Are there related topics or categories in this wiki resource for the curious reader to explore? How does this topic fit into that context?

===Further reading===

Books, Articles or other print media on this topic

===External links===

Internet resources on this topic

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

File:Electricz.jpg

2016-11-28T04:12:32Z

Pepper: http://www.free-ed.net/free-ed/Resources/TechnologyHub/Electricity/Matter.asp?iNum=1

http://www.free-ed.net/free-ed/Resources/TechnologyHub/Electricity/Matter.asp?iNum=1

Potential Energy of a Multiparticle System

2016-11-28T04:09:16Z

Pepper: /* A Mathematical Model */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
<div style="text-align: center;">
[[File:Sun_earth_orbit.png]]
</div>

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
<div style="text-align: center;">
[[File:Spring.jpg]]
</div>

What are the mathematical equations that allow us to model this topic. For example <math>{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}</math> where '''p''' is the momentum of the system and '''F''' is the net force from the surroundings.

===A Computational Model===

How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]

==Examples==

Be sure to show all steps in your solution and include diagrams whenever possible

===Simple===
===Middling===
===Difficult===

==Connectedness==
#How is this topic connected to something that you are interested in?
#How is it connected to your major?
#Is there an interesting industrial application?

==History==

Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.

== See also ==

Are there related topics or categories in this wiki resource for the curious reader to explore? How does this topic fit into that context?

===Further reading===

Books, Articles or other print media on this topic

===External links===

Internet resources on this topic

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

Potential Energy of a Multiparticle System

2016-11-28T04:08:38Z

Pepper: /* A Mathematical Model */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth as in the following figure, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.
[[File:Sun_earth_orbit.png]]

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
[[File:Spring.jpg]]

What are the mathematical equations that allow us to model this topic. For example <math>{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}</math> where '''p''' is the momentum of the system and '''F''' is the net force from the surroundings.

===A Computational Model===

How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]

==Examples==

Be sure to show all steps in your solution and include diagrams whenever possible

===Simple===
===Middling===
===Difficult===

==Connectedness==
#How is this topic connected to something that you are interested in?
#How is it connected to your major?
#Is there an interesting industrial application?

==History==

Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.

== See also ==

Are there related topics or categories in this wiki resource for the curious reader to explore? How does this topic fit into that context?

===Further reading===

Books, Articles or other print media on this topic

===External links===

Internet resources on this topic

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

File:Sun earth orbit.png

2016-11-28T04:08:10Z

Pepper: http://imagine.gsfc.nasa.gov/features/yba/CygX1_mass/gravity/sun_mass.html

http://imagine.gsfc.nasa.gov/features/yba/CygX1_mass/gravity/sun_mass.html

Potential Energy of a Multiparticle System

2016-11-28T04:05:50Z

Pepper: /* A Mathematical Model */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.

'''Spring Potential Energy''': In a multiparticle system as shown in the following figure in which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_sh^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>h</math> is the stretch of the spring.
[[File:Spring.jpg]]

What are the mathematical equations that allow us to model this topic. For example <math>{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}</math> where '''p''' is the momentum of the system and '''F''' is the net force from the surroundings.

===A Computational Model===

How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]

==Examples==

Be sure to show all steps in your solution and include diagrams whenever possible

===Simple===
===Middling===
===Difficult===

==Connectedness==
#How is this topic connected to something that you are interested in?
#How is it connected to your major?
#Is there an interesting industrial application?

==History==

Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.

== See also ==

Are there related topics or categories in this wiki resource for the curious reader to explore? How does this topic fit into that context?

===Further reading===

Books, Articles or other print media on this topic

===External links===

Internet resources on this topic

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

File:Spring.jpg

2016-11-28T04:04:50Z

Pepper: Pepper uploaded a new version of "File:Spring.jpg"

File:Spring.jpg

2016-11-28T04:04:17Z

Pepper: Pepper uploaded a new version of "File:Spring.jpg"

Potential Energy of a Multiparticle System

2016-11-28T03:54:59Z

Pepper: /* A Mathematical Model */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^{−11} N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.

'''Spring Potential Energy''': In a multiparticle system which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_ss^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>s</math> is the stretch of the spring.

What are the mathematical equations that allow us to model this topic. For example <math>{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}</math> where '''p''' is the momentum of the system and '''F''' is the net force from the surroundings.

===A Computational Model===

How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]

==Examples==

Be sure to show all steps in your solution and include diagrams whenever possible

===Simple===
===Middling===
===Difficult===

==Connectedness==
#How is this topic connected to something that you are interested in?
#How is it connected to your major?
#Is there an interesting industrial application?

==History==

Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.

== See also ==

Are there related topics or categories in this wiki resource for the curious reader to explore? How does this topic fit into that context?

===Further reading===

Books, Articles or other print media on this topic

===External links===

Internet resources on this topic

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

Potential Energy of a Multiparticle System

2016-11-28T03:54:13Z

Pepper: /* A Mathematical Model */

Claimed By yzhang637 - 2016 Fall

This wikipage discusses the definition and significance of the potential energy in a multiparticle system, and exemplifies it in different contexts.

==The Main Idea==

Imagine you drop a ball with a mass of <math>m</math> near the surface of the earth at the height of <math>h</math>. If the ball alone is considered to be the system, i.e., the Earth is the surrounding, it is straightforward to find that the kinetic energy of the system (ball) increases, due to the positive work done on the ball by the Earth. In other words, as the gravitational force acts in the same direction as the displacement of the ball, the work done by the surroundings (the Earth) is equal to <math>mgh</math>.

What if you choose the system to contain both the ball and the Earth? In this case, nothing is significant in the surroundings to exert any work on the system. As a result,
<div style="text-align: center;">
<math>\Delta K_{sys} = W_{surr}</math> =>
<math>\Delta K_{ball} + \Delta K_{earth} = 0 </math>
</div>
However, it is quite apparent from the experimental observation that the kinetic energy of the ball increased since it acquired speed when dropping, and that the kinetic energy of the Earth also increased in a small amount since the gravitational force between the ball and the Earth drew the Earth towards the ball. In other words, the experimental observation indicates that <math>\Delta K_{ball} > 0</math> and <math>\Delta K_{earth} > 0</math>. This seems to introduce a conflict between a real-world experiment and a fundamental principle in Physics, where the experiment indicates that the kinetic energy of the two-body system (ball + Earth) increased, while the energy principle states that the energy change of the system be zero since no significant work is done by the surroundings on the system. '''This can't be correct!''' One may decide that the fundamental Energy Principle has been violated. But wait! Is it possible that some energy component is overlooked during this process?

In fact, some energy component is missing from the energy principle for systems that contain more than one interacting object: the potential energy, commonly designated as <math>U</math>. In particular, any system that consists of more than one particle (multiparticle systems) such as the ball-Earth system, compressed/stretched springs, or atoms in which protons and electrons interact electrically, have a type of energy that is associated with the interactions between pairs of particles inside the system. In the ball-Earth system, it is associated with the interaction between the ball and the Earth, and it is different from the rest energies of the ball or the Earth, and different from the kinetic energies of the two individual particles. This specific type of pairwise interaction energy is referred to as ''potential energy'' for multiparticle systems. For this ball-Earth system consisting of the ball and the Earth interacting with each other, the total energy change is in fact:
<div style="text-align: center;">
<math>\Delta m_{ball}c^2 + \Delta m_{Earth}c^2 + \Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>
As the identities of the two particles do not change, <math>\Delta m_{ball}c^2 = 0</math> and <math>\Delta m_{Earth}c^2 </math>. As a result,
<div style="text-align: center;">
<math>\Delta K_{ball} + \Delta K_{earth} + \Delta U_{ball-Earth} = 0 </math>
</div>

===A Mathematical Model===
How do we calculate the potential energy in a multiparticle system? There are three major types of potential energies that are commonly discussed in real-world multiparticle systems.

'''Gravitational Potential Energy''': In general, in a system containing more than one particles constantly interacting with each other pairwise via gravitational force such as the Sun and the Earth, the potential energy at any moment between any two interacting particles with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = -G\frac{mM}{r}</math>
</div>
where <math>m</math> and <math>M</math> are the masses of the two particles, respectively, and <math>G</math> is the gravitational constant, <math>6.7 × 10^−11 N · m^2/kg^2</math>. In the ball-Earth system, where the ball with a mass of <math>m</math> is falling near the surface of the Earth of the height of <math>h</math>, the gravitational potential energy can be simplified as <math>mgh</math>.

'''Electric Potential Energy''': In a system containing more than one charged particles interacting with each other pairwise electrically such as the protons and the electrons in an atom, the potential energy at any moment between any two charged particle interacting with each other with a distance <math>r</math> can be calculated as:
<div style="text-align: center;">
<math>U = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r}</math>
</div>
where <math>\frac{1}{4\pi\epsilon_0}</math> is the electric constant, <math>9 × 10^9 N · m^2/C^2</math>, and <math>q_1</math>, <math>q_2</math> represent the amount of charges on the two interacting particles (measured in <math>C</math>). Note that unlike the gravitational potential energy, the electric potential energy can have either negative or positive value. If the two charges have opposite signs, the potential energy between the two interactive charged particles is negative. Otherwise, the potential energy is positive.

'''Spring Potential Energy''': In a multiparticle system which consists of a spring and other particles such as a ball detached to one end of the spring, the potential energy of the system can be calculated as
<div style="text-align: center;">
<math>U = \frac{1}{2}k_ss^2</math>
</div>
where <math>k_s</math> represents the spring constant and <math>s</math> is the stretch of the spring.

What are the mathematical equations that allow us to model this topic. For example <math>{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}</math> where '''p''' is the momentum of the system and '''F''' is the net force from the surroundings.

===A Computational Model===

How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]

==Examples==

Be sure to show all steps in your solution and include diagrams whenever possible

===Simple===
===Middling===
===Difficult===

==Connectedness==
#How is this topic connected to something that you are interested in?
#How is it connected to your major?
#Is there an interesting industrial application?

==History==

Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.

== See also ==

Are there related topics or categories in this wiki resource for the curious reader to explore? How does this topic fit into that context?

===Further reading===

Books, Articles or other print media on this topic

===External links===

Internet resources on this topic

==References==

This section contains the the references you used while writing this page

[[Category:Which Category did you place this in?]]

Potential Energy of a Multiparticle System

2016-11-28T03:45:55Z

Pepper: /* A Mathematical Model */

Potential Energy of a Multiparticle System

2016-11-28T03:43:29Z

Pepper: /* A Mathematical Model */

Potential Energy of a Multiparticle System

2016-11-28T03:40:17Z

Pepper: /* A Mathematical Model */

Potential Energy of a Multiparticle System

2016-11-28T03:40:00Z

Pepper: /* A Mathematical Model */

Potential Energy of a Multiparticle System

2016-11-28T03:39:30Z

Pepper: /* The Main Idea */

Potential Energy of a Multiparticle System

2016-11-28T03:31:07Z

Pepper: /* The Main Idea */

Potential Energy of a Multiparticle System

2016-11-28T03:30:40Z

Pepper: /* A Mathematical Model */

Potential Energy of a Multiparticle System

2016-11-28T03:19:29Z

Pepper: /* The Main Idea */

Potential Energy of a Multiparticle System

2016-11-28T03:05:54Z

Pepper: /* The Main Idea */

Potential Energy of a Multiparticle System

2016-11-28T03:05:35Z

Pepper: /* The Main Idea */

Potential Energy of a Multiparticle System

2016-11-28T03:04:23Z

Pepper: /* The Main Idea */

Potential Energy of a Multiparticle System

2016-11-28T03:03:21Z

Pepper: /* The Main Idea */

Potential Energy of a Multiparticle System

2016-11-28T03:03:02Z

Pepper: /* The Main Idea */

Potential Energy of a Multiparticle System

2016-11-28T02:59:41Z

Pepper: /* The Main Idea */

Potential Energy of a Multiparticle System

2016-11-28T02:59:06Z

Pepper: /* The Main Idea */

Potential Energy of a Multiparticle System

2016-11-28T02:49:47Z

Pepper: /* The Main Idea */

Potential Energy of a Multiparticle System

2016-11-28T02:47:25Z

Pepper: /* The Main Idea */

Potential Energy of a Multiparticle System

2016-11-28T02:46:53Z

Pepper: /* The Main Idea */

Potential Energy of a Multiparticle System

2016-11-28T02:03:33Z

Pepper: /* The Main Idea */

Potential Energy of a Multiparticle System

2016-11-28T02:02:18Z

Pepper: /* The Main Idea */