Conservation of Energy

Kyle Barber (kbarber8) claimed 03/26/2017

This page was originally created by ksubramanian33, as can be seen by the edit history.

Main Ideas

Conceptual Model

• Conservation of energy means that the total energy of a system will be the same before and after an event.
• This only applies to isolated systems (no outside forces acting on the system).
  • Not Isolated: An object sliding across a rough floor (system = the object). There is work being done by the floor on the object because of the frictional force.
  • Isolated: An object sliding across a rough floor (system = the object AND the floor). There is no work done on the system because all the forces are contained in the system.

see reference 1

Mathematical Model

• Single Particle
  • Particle Energy: E_particle = γmc²
  • Rest Energy: E_rest = mc²
  • Kinetic (particle): K = γmc² + mc²
• General Objects
  • Kinetic: (1/2)mv²
  • Gravitational Potential: (-Gm₁m₂)/(R²) (large distances), mgh (near the surface of the Earth)
  • Spring (Elastic) Potential: (1/2)k_ss²
  • Thermal Energy: mCΔT

General Formulas

• E = W + Q (if no heat transfer indicated, Q = 0; if no external forces acting on system, W = 0)
• E = K + U (The total energy is the sum of the kinetic and potential energies. From this, you can infer that for an isolated system, any change in kinetic energy will correspond in an equal but opposite change in the potential energy and vice versa.)

These formulas can be interchanged. For example, is you know work and heat transfer are zero, energy equals zero, so K + U will equal zero

See Reference 2

Basic Explanation of Conservation of Energy
Skater Visualization of Transfers of Energy

Examples

Particle

An electron is accelerated to a speed of 2.95 × 108 

(a) What is the energy of the electron? 

(b) What is the rest energy of the electron? 

(c) What is the kinetic energy of the moving proton? 

(a)
E = γmc²
E = (5.50)(9.11 × 10^-31)(3 × 10⁸)
E = 1.50 × 10^-21 J
(b)
E_rest = mc²
E_rest = (9.11 × 10^-31)(3 × 10⁸)²
E_rest = 2.73 × 10^-22 J
(c)
K = E - E_rest K = 1.50 × 10^-21 - 2.73 × 10^-22
K = 1.23 × 10^-21 J

Simple

A ball is at rest on a table with 50 J of potential energy. 
It then rolls of the table, and at one point in time as it falls, the ball has 30 J of kinetic energy. 

What is the potential energy of the ball at that instant?

See Reference 3

E_initial = E_final
K_initial + U_initial = K_final + U_final
0 J + 50 J = 30 J + U_final
U_final = 20 J

Middling

A ball is at rest 50 m above the ground. You then drop the ball.
What is its speed before hitting the ground? 

See Reference 4

v = √2gh 
v = √2(9.8)(50) 
v = 31.3 m/s

Difficult

The driver of an SUV (m = 1700 kg) isn’t paying attention and rear ends a car (m = 950 kg) on level ground at a red light.
On impact, both drivers lock their brakes. The SUV and car stick together and travel a distance of 8.2 m before they
come to a stop. How fast was the SUV traveling just before the collision? The coefficient of friction between the tires and
the road is 0.72.

See Reference 5

Notice how the mass is canceled.

Connectedness

Computer Science
1. How is this topic connected to something that you are interested in?
This concept is clearly connected to physics and helps explain and sometimes predict how our world works. Knowing why and how things move and interact is very powerful.
2. How is it connected to your major?
This topic is connected to computer science in the field of modeling and simulation. When you use computers to more efficiently model grand scale scenarios, it is important to take all fundamental concepts of physics, including the conservation of energy, into account.
3. Is there an interesting industrial application?
The law of conservation of energy is prevalent in nearly every industrial application of physics. More specifically, it is relevant today as finding renewable and sustainable forms of energy is becoming a more prevalent social and economic issue. It will be interesting to see how this concept will be applied as we try to get more energy for less.

History

Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.
Who: Julius Robert Mayer
What: Most formally discovered the law of conservation of energy
When: 1842
Where: Germany
Why: To explain what happens to energy in an isolated system
See Reference 6

See also

Kinetic Energy
Potential Energy
Work

Further reading

Goldstein, Martin, and Inge F., (1993). The Refrigerator and the Universe. Harvard Univ. Press. A gentle introduction.
Kroemer, Herbert; Kittel, Charles (1980). Thermal Physics (2nd ed.). W. H. Freeman Company. ISBN 0-7167-1088-9.
Nolan, Peter J. (1996). Fundamentals of College Physics, 2nd ed. William C. Brown Publishers.

External links

The First Law of Thermodynamics
Khan Academy [1]
Practice Questions [2]
More Practice [3]
Basic Examples [4]

References

1."Conservation of Energy." Hmolpedia. Web. 1 Dec. 2015. <http://www.eoht.info/page/Conservation+of+energy>.
2. "University of Wisconsin Green Bay." Speed & Stopping Distance of a Roller-Coaster. Web. 1 Dec. 2015. <http://www.uwgb.edu/fenclh/problems/energy/2/>.
3. "Motion." G9 to Engineering. Web. 1 Dec. 2015. <http://www.g9toengineering.com/resources/translational.htm>.
4. "Energy of Falling Object." HyperPhysics. Web. 1 Dec. 2015. <http://hyperphysics.phy-astr.gsu.edu/hbase/flobj.html>.
5. "Conservation of Energy & Momentum Problem: Collision of Two Cars at a Stoplight." University of Wisconsin- Green Bay Physics. Web. 2 Dec. 2015. <http://www.uwgb.edu/fenclh/problems/energy/6/>.
6. "Law of Conservation of Mass Energy." Law of Conservation of Mass Energy. Web. 3 Dec. 2015. <http://www.chemteam.info/Thermochem/Law-Cons-Mass-Energy.html>.