Prove square of four-momentum is relativistic invariant

In summary, the task is to prove that the square of relativistic four-momentum for a massive particle is a relativistic invariant under Lorentz transformations. This means that two observers in different frames should agree on this quantity. You can derive it explicitly by taking the square of the 4-momentum and applying Lorentz transformations, or use an example from class notes to illustrate the concept. Good luck with your assignment!
  • #1
Falken_47
9
0

Homework Statement



Hi everyone,

I have a physics assignment that asks: Prove that the square of relativistic four-momentum for a massive particle is a relativistic invariant under Lorentz transformations.

Can anyone help me to work on the problem? I'm always lost in the class ever since my professor starts teaching modern physics. Any help would be greatly appreciated!

Homework Equations



p = <γmc, γmv>

The Attempt at a Solution



From what I can gather from the question and my understanding, relativistic invariant means that the four-momentum from two different observer should be the same. My best shot on this question is through example from my class notes:

suppose p1 (four-momentum from observer 1) is <γmc, γmv> and p2 four-momentum from observer 2, traveling at speed v) is <mc, 0>. Therefore when we calculate p^2 for both observer we find it to be (mc)^2

Again I'm really grateful for any help you could give me
 
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  • #2
Hi Falken_47. If you want to derive it explicitly, take the square of the 4-momentum [itex]p^i=({\gamma}mc,{\gamma}m{\mathbf{v}})[/itex], apply the Lorentz transformations for a contravariant 4-vector to obtain [itex]p^i{'}[/itex] which moves in a frame at an arbitrary speed V with respect to the original frame. So you should have [itex]p^i{'}[/itex] in terms of non-primes, take the square of this and after some algebra you should arrive at the same solution as you had for the square of [itex]p^i[/itex]. Lorentz Invariant just means that 2 observers in 2 different inertial frames will agree on the quantity which is invariant.
 
  • #3
Falken_47 said:

Homework Statement



Hi everyone,

I have a physics assignment that asks: Prove that the square of relativistic four-momentum for a massive particle is a relativistic invariant under Lorentz transformations.

Can anyone help me to work on the problem? I'm always lost in the class ever since my professor starts teaching modern physics. Any help would be greatly appreciated!

Homework Equations



p = <γmc, γmv>

The Attempt at a Solution



From what I can gather from the question and my understanding, relativistic invariant means that the four-momentum from two different observer should be the same. My best shot on this question is through example from my class notes:

suppose p1 (four-momentum from observer 1) is <γmc, γmv> and p2 four-momentum from observer 2, traveling at speed v) is <mc, 0>. Therefore when we calculate p^2 for both observer we find it to be (mc)^2

Again I'm really grateful for any help you could give me

I think that your method is both elegant and correct.
 

FAQ: Prove square of four-momentum is relativistic invariant

What is the definition of four-momentum?

Four-momentum is a four-dimensional vector that describes the energy and momentum of a particle in special relativity. It is given by the product of the particle's energy and its four-velocity.

Why is it important to prove that the square of four-momentum is relativistic invariant?

This proof is important because it demonstrates that the laws of physics, specifically those related to energy and momentum, are the same for all observers in different reference frames. It is a fundamental principle of special relativity.

How is the square of four-momentum calculated?

The square of four-momentum is calculated by taking the dot product of the four-momentum vector with itself. This results in a scalar quantity that is invariant under Lorentz transformations.

What does it mean for a quantity to be relativistic invariant?

A relativistic invariant quantity is one that has the same value for all observers in different frames of reference, regardless of their relative velocities. This means that the laws of physics, which are described by these quantities, are the same for all observers.

How is the proof of the invariance of four-momentum related to the principle of conservation of energy and momentum?

The proof of the invariance of four-momentum is directly related to the principle of conservation of energy and momentum. This is because the invariance of four-momentum implies that the total energy and momentum of a system is conserved in all reference frames, which is a fundamental principle of physics.

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