Conservation of Energy

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

Main Ideas

Conceptual Model

• The law of conservation of energy states that the total amount of energy of a system before and after an interaction between objects in conserved.
• 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. Energy lost to heat due to friction is an example of mechanical energy being converted into thermal energy.
  • 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 7

Mathematical Model

Here are some helpful formulas to remember that were mentioned in previous sections!

• • Kinetic: [math]\displaystyle{ {1 \over 2} }[/math]mv²
    
  • Gravitational Potential:[math]\displaystyle{ {-Gm1m2 \over r^2} }[/math], mgh (near the surface of the Earth)
    
    
  • Spring (Elastic) Potential: [math]\displaystyle{ {1 \over 2} }[/math]kx²
    
  • Thermal Energy:mCΔT

General Formulas

• ΔE = W + Q (if no heat transfer indicated, Q = 0; if no external forces acting on system, W = 0)
• ΔE = 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, if 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

Computational Model

Below is a link to a segment of Vpython code that models the motion of a spring and graphs its kinetic and potential energy. It also shows how the total amount of energy of the system does not change.

"https://trinket.io/embed/glowscript/49c1365501?showInstructions=true"

Examples

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

KE₂ + PE₂ = KE₃ + PE₃ - W_nc
(1/2)m_totalv₂² + m_totalgh₂ = (1/2)m_totalv₃² + m_totalgh₃ - W_nc
(1/2)m_totalv₂² + 0 = 0 + 0 - (μm_totalg)dcos(180°)
(1/2)v₂² = -(0.72)(9.8 m/s²)(8.2 m)(-1)
v₂² = 116 m²/s²
v₂ = 10.8 m/s

• Notice how the mass is canceled.
  

p₁ = p₂
p_1x = p_2x
m_suvv_suv + m_carv_car = m_totalv₂
(1700 kg)v_suv + 0 = (2650 kg)(10.8 m/s)
(1700 kg)v_suv = 28600 kgm/s
v_suv = 17 m/s

Connectedness

ADD INFO ABOUT CONNECTEDNESS

History

Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.
Who: Many physicists contributed to the knowledge of energy, however it is most notably atributed to 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

Khan Academy
Practice Questions
More Practice
Basic Examples
The First Law of Thermodynamics

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>. 7. "Law of Conservation of Energy" New York University. Web. 18 Apr. 2018. <http://www.nyu.edu/classes/tuckerman/adv.chem/lectures/lecture_2/node4.html> 8. "Law of Conversation of Energy" ME Mechanical. Web. 18 Apr. 2018. <https://me-mechanicalengineering.com/law-of-conservation-of-energy/>