Is there a relativistic version of the work-energy theorem?

In summary: Yes, they are just different perspectives. So, regardless of the choice of reference frame, the work-energy theorem remains valid and the work done on the object is equal to the change in kinetic energy.In summary, the work-energy theorem states that the work done on an object is equal to the change in its kinetic energy, regardless of the choice of reference frame. This applies to both classical and relativistic versions of the theorem. The Lorentz transformations allow for the relationship between different inertial frames, but the fundamental principle remains unchanged.
  • #1
jaketodd
Gold Member
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The work-energy theorem is stated here on Wikipedia. On the same page it says "regardless of the choice of reference frame, the work energy theorem remains valid and the work done on the object is equal to the change in kinetic energy."

I am wondering if there is a relativistic version of the work-energy theorem.

Thanks,

Jake
 
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  • #2
jaketodd said:
I am wondering if there is a relativistic version of the work-energy theorem.

No. The classical version applies to relativity too. But the result is different.
 
  • #3
[itex]W=\Delta E_k=(\gamma -1)mc^2[/itex]

Just integrate force over some distance, starting from rest:

[tex]W=\int Fdx=\int \frac{dp~dx}{dt}=\int vdp=vp-\int pdv=\gamma mv^2-\int \gamma mvdv[/tex]

What you end up with is:

[itex]W=\gamma mc^2+C[/itex]

with some constant of integration C. If you set v=0, you take W=0 and γ=1, therefore C=-mc2. So what you get is:

[itex]W=\gamma mc^2-mc^2=(\gamma -1)mc^2=E_k[/itex]
 
  • #4
In general, [itex]W=\int F dx[/itex], but the Lorentz transformations tell you the relationship between dx in the two different inertial frames as [itex]dx = {{dx'}\over{\sqrt{1-{{v^2}\over{c^2}}}}}[/itex].
 
  • #5
Pengwuino said:
In general, [itex]W=\int F dx[/itex], but the Lorentz transformations tell you the relationship between dx in the two different inertial frames as [itex]dx = {{dx'}\over{\sqrt{1-{{v^2}\over{c^2}}}}}[/itex].

Two different inertial frames?
 

1. What is the work-energy theorem?

The work-energy theorem is a fundamental principle in classical mechanics that states that the net work done on an object equals the change in its kinetic energy. In other words, if an external force is applied to an object, it will either increase or decrease its speed, resulting in a change in its kinetic energy.

2. Is the work-energy theorem applicable to relativistic systems?

No, the work-energy theorem only applies to classical mechanics, which describes the motion of objects at speeds much lower than the speed of light. For systems moving at relativistic speeds, the equations of special relativity must be used.

3. What is the relativistic version of the work-energy theorem?

The relativistic version of the work-energy theorem is known as the relativistic energy-momentum relation. It states that the net work done on an object equals the change in its total energy, which includes both its rest energy and its kinetic energy. This is derived from the principle of conservation of energy in special relativity.

4. How is the relativistic version of the work-energy theorem different from the classical version?

The major difference between the two versions is that the classical version only considers the change in an object's kinetic energy, while the relativistic version takes into account the change in its total energy, which includes its rest energy. Additionally, the equations used in the relativistic version are different, as they are based on the principles of special relativity.

5. What are some examples of relativistic systems where the work-energy theorem is applicable?

The relativistic version of the work-energy theorem is applicable in a variety of situations, including the motion of particles at high speeds in particle accelerators, the motion of charged particles in electric and magnetic fields, and the motion of objects in the presence of strong gravitational fields, such as black holes.

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