Conservation of Energy in different inertial frames

Click For Summary

Discussion Overview

The discussion revolves around the conservation of energy as observed from different inertial frames, particularly in the context of a mass sliding down a slope. Participants explore how energy appears to change when viewed from different reference frames, raising questions about the invariance of energy and the implications for conservation laws in classical mechanics and relativity.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • One participant describes a scenario where a mass sliding down a slope appears to violate conservation of energy when viewed from a moving frame.
  • Another participant asserts that energy is conserved across all frames but is not invariant, meaning measurements of energy can differ based on the observer's frame of reference.
  • A different viewpoint suggests that the kinetic energy of the Earth must be accounted for in the moving frame to resolve the apparent discrepancy in energy conservation.
  • Some participants express confusion regarding the definitions of invariant and conserved, questioning whether energy can be both.
  • There are discussions about the vector nature of kinetic energy and the importance of considering direction when analyzing energy in different frames.
  • A participant provides a mathematical proof to demonstrate that energy conservation holds true across different inertial frames, emphasizing that all terms in the energy equations remain constant.
  • Another participant highlights the necessity of considering all forces acting on the mass and the slope to fully understand the energy dynamics in different frames.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the nature of energy invariance versus conservation. While some agree that energy is conserved in all frames, others remain uncertain about the implications of this conservation and the definitions involved.

Contextual Notes

Participants express uncertainty regarding the definitions of invariant and conserved, and the discussion includes various assumptions about the forces acting on the mass and the Earth, as well as the mathematical treatment of kinetic energy.

Who May Find This Useful

This discussion may be useful for students and enthusiasts of physics, particularly those interested in classical mechanics, relativity, and the nuances of energy conservation across different reference frames.

bartieshaw
Messages
50
Reaction score
0
today my dynamics lecturer illustrated a situation to us where energy did not appear to be conserved.

The situation involves observing the motion of a mass sliding down a slope, height 'h' above the ground from rest

initially in the rest frame, we see;

initially,
PE = mgh
KE = 0

as the mass starts from rest (we are assuming the force required to start the motion of the mass is insignificant)

and finally (at the bottom of the slope),
PE = 0
KE = 1/2 mv^2

NB. i cannot work out how to make a diagram and post it, but imagine the mass is sliding down the slope to the right.


using this we can claculate the simple equation to determine the final velocity of the mass (to the right)

v = (2gh)^(1/2)

This was simple to comprehend, but now our lecturer asked us to imagine observing the motion from another inertial frame moving to the right (relative to the rest frame) at velocity, v = (2gh)^(1/2)

when drawing this, we see the mass now appears to initially be be moving to the left with velovity, v = (2gh)^(1/2), and when the mass reaches its maximum velocity (v = (2gh)^(1/2) to the right) at the bottom, the mass appears to be at rest.

thus when observing from this frame we see the following occurring

initially
PE = mgh
KE = 1/2 mv^2 = mgh

hence, initial energy, E=2mgh

and finally (at the bottom of the slope)
PE = 0
KE = 0

this obviously seems to disagree with the conservation of energy and I am sure there is something wrong with what i have described, but i simply do not know

can anyone explain what is really going on here...?
 
Physics news on Phys.org
Actually this is not an issue of the conservation of energy. This is an issue known as invariance. Energy is always conserved, but it is not invariant meaning that depending on your frame of reference you will measure it differently. Any object traveling at the same velocity as you will appear to have no kinetic energy right? But you will find that whatever reference frame you use, the conservation laws will hold. When you step into the realm of relativity you will also find other quantities:

mass: not conserved but invariant
charge: conserved and invariant
velocity: neither conserved nor invariant
 
Your instructor is just pulling your leg.
bartieshaw said:
thus when observing from this frame we see the following occurring

initially
PE = mgh
KE = 1/2 mv^2 = mgh

hence, initial energy, E=2mgh
You must include the KE energy of the Earth, since it's moving in this frame.

and finally (at the bottom of the slope)
PE = 0
KE = 0
Figure out the work done on the Earth during the ball's motion. You'll find that the work done on the Earth will exactly equal the missing energy. Energy is conserved!

(Hint: How far does the Earth move during the time that the ball falls? Realize that the average horizontal speed of the ball is only v/2, so that the Earth moves twice as far as the ball.)
 
i don't understand...
bartieshaw...
do u understand?
 
Yeah, i do now, thank you for answering
 
Still unsure

I sort of understand what you are saying, but can't seem to be prove it...?
 
So which is right? Is the statement that energy is invariant correct, or is it right to say energy is conserved even during changing frames?

Is energy invariant or not?

Also, why is it called invariant? Doesn't that mean in does not vary??
 
leright said:
So which is right? Is the statement that energy is invariant correct, or is it right to say energy is conserved even during changing frames?
Huh? Who said energy was invariant?

Yes, energy is conserved in either frame.
 
Doc Al said:
Huh? Who said energy was invariant?

Yes, energy is conserved in either frame.

n/m. nobody said it was invariant. :p I was lacking sleep when I wrote that.
 
Last edited:
  • #10
bartieshaw said:
when drawing this, we see the mass now appears to initially be be moving to the left with velovity, v = (2gh)^(1/2), and when the mass reaches its maximum velocity (v = (2gh)^(1/2) to the right) at the bottom, the mass appears to be at rest.

thus when observing from this frame we see the following occurring

initially
PE = mgh
KE = 1/2 mv^2 = mgh

hence, initial energy, E=2mgh

and finally (at the bottom of the slope)
PE = 0
KE = 0
There's your mistake. Should be [tex]KE = -1/2 mv^2[/tex]. KE has a vector, and at the start of the experiment, it is opposite to your "moving" reference frame.
 
  • Skeptical
Likes   Reactions: Dale
  • #11
WhyIsItSo said:
There's your mistake. Should be [tex]KE = -1/2 mv^2[/tex]. KE has a vector, and at the start of the experiment, it is opposite to your "moving" reference frame.
KE is a scalar, not a vector!
 
Last edited:
  • Like
Likes   Reactions: Dale
  • #12
How so, given the velocity term?PS: (im not arguing with your statement, i think i know why, i just can't be sure :P)
 
  • #13
Because the velocity term appears in the expression for KE within a scalar product:

[tex]T = \frac{m|\vec{v}|^2}{2} = \frac{m\vec{v}\cdot\vec{v}}{2}[/tex]

i.e. it's the length squared. It's the only way to turn a pair of vectors into a scalar - by the scalar/inner (sometimes known as dot) product. And by definition, the inner product of two vectors is equal to or greater than 0 (the equality holding for the zero vector only).
 
Last edited:
  • #14
So confused?

:confused: Can someone please clarify this? What is actually happening? Thanks
 
  • #15
Look at it this way, change the math the way I suggested and the mystery disappears.

Kinetic Energy is the result of motion which has a vector. You cannot ignore the direction the force is applied in and expect the OP situation to make any mathematical sense.
 
  • Skeptical
Likes   Reactions: Dale
  • #16
WhyIsItSo said:
Look at it this way, change the math the way I suggested and the mystery disappears.
It only appears to. The math as suggested by you is wrong...and it wouldn't work for any other velocity of the reference frame (w.r. to the Earth frame).


Kinetic Energy is the result of motion which has a vector. You cannot ignore the direction the force is applied in and expect the OP situation to make any mathematical sense.
The KE itself is a scalar and the situation makes perfect mathematical sense if you do the math right.

Pete, see post #3.
 
  • Informative
Likes   Reactions: Dale
  • #17
Work Done on the Earth?

Ok I understand the concept now. So with the addition of the work done by the Earth energy is conserved. But how do I find the work done on the Earth so that I can prove that energy has been conserved?...
 
  • #18
To properly account for the KE, you must consider all the forces acting. In particular, the sliding mass and slope exert forces on each other.

In the usual frame of reference, where the slope is stationary, this contact force--the normal force--does no work.

But viewed from a moving frame, the slope moves and thus "work" is being done by those forces on the slope and on the mass. Since they move at different speeds, the work done on each is not the same. But the net change in KE of all objects (earth and sliding mass) will exactly balance the change in gravitational PE.
 
  • #19
Proof that changing the refererence inertial frame doesn't change the truth of energy conservation:

First, we have the "rest frame", the frame where we accept the truths of momentum and energy conservation (for the problem in the OP, this is the Earth frame). In this frame,

[tex]P_0 = \sum m_iv_i = const[/tex]

[tex]E_0 = (1/2)\sum m_iv_i^2 + \sum U_i = const[/tex]

Now consider a frame moving a speed v (v<<c), relative to this frame. In the new frame,

[tex]E_v = (1/2)\sum m_i(v_i-v)^2 + \sum U_i = E_0 - (1/2)\sum m_iv_i^2 + (1/2)\sum m_i(v_i-v)^2 = E_0 - 2vP + (1/2)\sum m_iv^2[/tex]

All the terms in the RHS are constants, and hence, the total energy is conserved in the new frame as well.

Note: All squares and products of velocities (or velocities with momenta) are to be understood as scalar (dot or inner) products.
 
Last edited:
  • #20
Excellent, Gokul. That's the easiest way to convince oneself that energy is conserved in all frames, since it avoids having to consider the details of the forces involved.
 

Similar threads

  • · Replies 3 ·
Replies
3
Views
1K
  • · Replies 6 ·
Replies
6
Views
3K
  • · Replies 30 ·
2
Replies
30
Views
4K
  • · Replies 7 ·
Replies
7
Views
1K
  • · Replies 14 ·
Replies
14
Views
3K
  • · Replies 8 ·
Replies
8
Views
3K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 3 ·
Replies
3
Views
1K