Conservation of Energy: Kinetic & Reference Frames

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SUMMARY

The discussion centers on the relationship between kinetic energy and reference frames, emphasizing that while kinetic energy is reference frame dependent, it does not violate the conservation of energy principle. Participants clarify that energy conservation is frame-specific but remains constant within each frame. The example of two 1 kg masses connected by a spring illustrates that energy conservation holds true across different frames, with varying kinetic and potential energy values but consistent total energy. Thus, energy conservation is maintained even when observed from different reference frames.

PREREQUISITES
  • Understanding of kinetic energy and its formula (KE = ½ mv²)
  • Familiarity with reference frames in physics
  • Basic knowledge of potential energy concepts
  • Concept of energy conservation in isolated systems
NEXT STEPS
  • Study the implications of reference frame transformations in classical mechanics
  • Learn about the concept of invariance versus conservation in physics
  • Explore examples of energy conservation in non-isolated systems
  • Investigate the role of momentum in different reference frames
USEFUL FOR

This discussion is beneficial for physics students, educators, and anyone interested in the principles of energy conservation and reference frames in classical mechanics.

Zubair Ahmad
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If velocity is reference frame dependent then kinetic energy should also be.
Considering this we will have different energies in different frames.
Doesn't it violate conservation of energy?
 
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No it doesn't. Being frame dependent and conserved are different things. Conserved means it is constant in time, but it can be different constants in different frames.
 
So it means conservation of energy is limited to a single frame
 
No, it means that energy is constant in every frame, but in principle this constant may have different (but constant in time) values in different frames.
 
So we can have a zero energy frame also?
 
Zubair Ahmad said:
So we can have a zero energy frame also?

When a mass m is at rest in your reference frame, what is its kinetic energy?

Zz.
 
Zero!
 
Zubair Ahmad said:
Zero!

Haven't you just answered your question?

Zz.
 
That I know but what about the original question..
How to explain conservation?
 
  • #10
Zubair Ahmad said:
So we can have a zero energy frame also?
For a system of particles there is no zero kinetic energy frame as there is a zero momentum frame. That should be obvious, as kinetic energy is non negative.
 
  • #11
Zubair Ahmad said:
That I know but what about the original question..
How to explain conservation?

Again, as has been stated by other responses, there is no issue with energy conservation.

If you are in one reference frame, and the object is moving at speed v, the object has KE = ½ mv2.

On the other hand, an observer moving with the object will measure zero KE.

There is no issue with conservation of energy here. Each observer is in a different frame, as has already been mentioned.

If you are in one reference frame and wish to go to another reference frame, you have to BOOST yourself to that frame, and thus, require external energy input. This is now no longer an isolated system and energy should not be conserved for the original system.

Zz.
 
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  • #12
Zubair Ahmad said:
If velocity is reference frame dependent then kinetic energy should also be.
Considering this we will have different energies in different frames.
Doesn't it violate conservation of energy?
The fact a quantity doesn't vary changing the frame of reference is not called "conservation" in physics, it's (usually) called "invariance". They are both important, but completely different concepts.

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  • #13
Zubair Ahmad said:
If velocity is reference frame dependent then kinetic energy should also be.
Considering this we will have different energies in different frames.
Yes, this is correct.

Zubair Ahmad said:
Doesn't it violate conservation of energy?
No, it does not. Let’s consider a specific toy example. Suppose we have two 1 kg masses joined by a compressed spring containing 1 J of elastic energy.

In the frame where they are initially at rest the initial KE is 0 J and the initial PE is 1 J. If the spring is released then one mass will move at 1 m/s and the other mass will at -1 m/s. So the final KE is 1 J (evenly divided between the masses) and the final PE is 0 J. Energy is conserved.

In the frame where they are initially moving at 2 m/s the initial PE is 1 J and the initial KE is 4 J. After release one mass will move at 3 m/s and the other will move at 1 m/s. So the final KE is 5 J (4.5 J in one mass and 0.5 J in the other) and the final PE is 0 J. Energy is also conserved.
 

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