Galilean invariance verification (kinetic energy and momentum)

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SUMMARY

The discussion centers on verifying the Galilean invariance of the relationship between kinetic energy and momentum, specifically the equation E = p²/2m. The participant successfully demonstrates that this relationship holds true in both reference frames S and S' by substituting the momentum expression into the kinetic energy equation. The calculations confirm that the kinetic energy transformation aligns with the Galilean transformation, thereby establishing the invariance of the equation under transformation between frames. The source referenced is McComb's "Dynamics and Relativity" (1999).

PREREQUISITES
  • Understanding of Newton's second law and Galilean invariance
  • Familiarity with kinetic energy and momentum equations
  • Basic knowledge of frame transformations in classical mechanics
  • Ability to manipulate algebraic expressions involving physical quantities
NEXT STEPS
  • Study the implications of Galilean invariance in classical mechanics
  • Explore the derivation of kinetic energy and momentum relationships
  • Learn about transformations between inertial frames in physics
  • Investigate the differences between Galilean and Lorentz transformations
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Students preparing for physics exams, educators teaching classical mechanics, and anyone interested in the foundational principles of motion and energy in physics.

Tiddo
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Hi all,

First of all, sorry for not using the template, but I think in this situation it's better to explain my problem right away:
I'm studying for a physics test, but I think I don't really understand Galilean invariance. In my textbook there is an example in which they proof that if you consider 2 frames S and S' in standard configuration that the second law of Newton is Galilean invariant by proofing that if [itex]x' = x - Vt[/itex] than [itex]F_x = F'_x[/itex], so this law holds in both frames. So far I understand this.

However, in the book there is one assignment in which they ask me to verify that the relationship between kinetic energy and momentum, [itex]E = p^2/2m[/itex], is Galilean invariant. I couldn't really figure it out by myself so I looked at the answers. The answer is as followed:
In S:

[itex]E = \frac{1}{2}m\dot{x}^2;[/itex] [itex]p=m\dot{x}.[/itex]

Substitute [itex]\dot{x} = p/m[/itex] in the equation for the energy:

[itex]E = \frac{1}{2}m(\frac{p}{m})^2=p^2/2m[/itex]

In S':

[itex]E'=\frac{1}{2}m\dot{x}'^2-\frac{1}{2}m(\dot{x}-V)^2=\frac{1}{2}m\dot{x}^2-m\dot{x}V^2[/itex]

[itex]p'=m\dot{x}'[/itex]

Assume the relationship holds: i.e.,

[itex]E'=\frac{p'^2}{2m}=\frac{1}{2m}(m\dot{x}-mV)^2=\frac{1}{2}(\dot{x}^2-2\dot{x}V+V^2)=\frac{1}{2}m\dot{x}-m\dot{x}V+\frac{1}{2}mV^2,[/itex]

in agreement with the Galilean transformation of the kinetic energy
Source: McComb, W. D., 1999. Dynamics and Relativity. New York: Oxford University Press Inc.

I understand all of the equations, however I just don't understand why this verifies that this relationship is Galilean invariant.

Can someone explain this to me?

Thanks!
 
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There is a problem with the computation of E' in the solutions. It should read:

[tex]E^\prime = \frac{1}{2}m(\dot{x}^{\prime})^2 =\frac{1}{2}m(\dot{x}-V)^2 = \frac{1}{2}m(\dot{x}^2 - 2\dot{x}V + V^2)[/tex]

[tex]= \frac{1}{2}m\dot{x}^2 - m\dot{x}V + \frac{1}{2}mV^2[/tex]

You can see that this expression for E' is the same as what is obtained if you assume that E' = (p')2/2m, showing that this relation between kinetic energy and momentum does indeed hold in S' as well.
 
thank you sp much! I completely missed that. now it'd all clear to me:)
 

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