Special relativity momentum and energy conservation

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Homework Help Overview

The discussion revolves around a problem in special relativity involving two identical particles of mass m traveling towards each other at speed v, which combine to form a new particle. Participants are exploring the implications of conservation of momentum and energy in this context.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants express confusion about the need for a frame of reference and whether to treat velocity as a vector. There is a discussion about the implications of momentum being zero before the collision and how that affects the final state post-collision. Some participants suggest considering different reference frames, such as one where a particle is at rest, to clarify the situation.

Discussion Status

There is ongoing exploration of the problem, with participants questioning assumptions about momentum and energy conservation. Some guidance has been offered regarding the use of reference frames and the nature of the collision, but no consensus has been reached on the specifics of the solution.

Contextual Notes

Participants note that the collision is assumed to be head-on and consider the implications of a perfectly inelastic collision in a relativistic context. There is also mention of the need for clarity on the use of LaTeX for mathematical expressions in the forum.

Taylor_1989
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Homework Statement


Two identical particles of mass m travel towards each other at speed v; they combine and form a single new particle. By employing conservation of momentum and conservation of energy, what is the mass of this new particle in

Homework Equations


Relativistic momentum and total energy , possibly lorentz velocity transformation

The Attempt at a Solution



I am completely lost to where to start with this, because of two reasons. I can see if I need to use a frame of reference, I not sure if the v<<c and do I take the velocity as a vector?

I know the momentum and total energy are consevered in relativity but in the question I see that if the final momentum is equal to the sum of the initial surely this 0 because they are moving at the same speed and they are the same mass, so how can they even move at a speed after the collision. My lecture has not explained this very well in his notes and I am very lost could someone please help me.

Also tell me what the latex tags are for the physics forum. Big thanks in advance.
 
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Taylor_1989 said:

Homework Statement


Two identical particles of mass m travel towards each other at speed v; they combine and form a single new particle. By employing conservation of momentum and conservation of energy, what is the mass of this new particle in

Homework Equations


Relativistic momentum and total energy , possibly lorentz velocity transformation

The Attempt at a Solution



I am completely lost to where to start with this, because of two reasons. I can see if I need to use a frame of reference, I not sure if the v<<c and do I take the velocity as a vector?

I know the momentum and total energy are consevered in relativity but in the question I see that if the final momentum is equal to the sum of the initial surely this 0 because they are moving at the same speed and they are the same mass, so how can they even move at a speed after the collision. My lecture has not explained this very well in his notes and I am very lost could someone please help me.

Also tell me what the latex tags are for the physics forum. Big thanks in advance.

I think it's safe to assume that "towards each other" means a head-on collision. So, momentum before the collision is 0, as you suspected.

Latex in line ##E = mc^2## or isolated: $$E = mc^2$$
 
Taylor_1989 said:

Homework Statement


Two identical particles of mass m travel towards each other at speed v; they combine and form a single new particle. By employing conservation of momentum and conservation of energy, what is the mass of this new particle in

Homework Equations


Relativistic momentum and total energy , possibly lorentz velocity transformation

The Attempt at a Solution



I am completely lost to where to start with this, because of two reasons. I can see if I need to use a frame of reference, I not sure if the v<<c and do I take the velocity as a vector?

I know the momentum and total energy are consevered in relativity but in the question I see that if the final momentum is equal to the sum of the initial surely this 0 because they are moving at the same speed and they are the same mass, so how can they even move at a speed after the collision. My lecture has not explained this very well in his notes and I am very lost could someone please help me.

Also tell me what the latex tags are for the physics forum. Big thanks in advance.
Something to think about to clarify your thinking on the velocity and Lorentz transform: would the answer be any different if you were to use a reference frame in which one of the particles is at rest?
 
phinds said:
Something to think about to clarify your thinking on the velocity and Lorentz transform: would the answer be any different if you were to use a reference frame in which one of the particles is at rest?

Personally, I would prefer the centre-of-momentum frame for his one!
 
Thank for the response guy, I just had another look and it dawned on me. I mean momentum would be 0 and then I could total energy of the system is equal to the rest energy hence [math]E=mc^2[\math]
 
Taylor_1989 said:
Thank for the response guy, I just had another look and it dawned on me. I mean momentum would be 0 and then I could total energy of the system is equal to the rest energy hence [math]E=mc^2[\math]

You have to enclose the math in side two # or two $
eg:
#`# e = mc^2 #`#
or $`$ e = mc^2 $`$

just don't put ` in between.It is to stop the rendering of math.
 
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Taylor_1989 said:
Thank for the response guy, I just had another look and it dawned on me. I mean momentum would be 0 and then I could total energy of the system is equal to the rest energy hence [math]E=mc^2[\math]

No. If the collision is perfectly inelastic (all kinetic energy converted to mass) then the mass afterwards would NOT be ##2m## in the relativistic case. (In the classical case we would not have conservation of energy because mass end energy are not equivalent in that regime.)
 

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