Special Relativity: Collision of a Particle and Antiparticle

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Homework Help Overview

The discussion revolves around a problem in special relativity involving a particle and its antiparticle colliding to create a new particle. The original poster outlines the rest energies and total energy involved in the collision, seeking to determine the required speeds of the particles before the collision.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to apply conservation of energy and momentum principles, laying out equations related to total energy and relativistic momentum. They express uncertainty about the next steps after deriving equations for momentum and energy.
  • Some participants question the approach of setting one of the velocities to zero and suggest alternative methods for solving the problem.

Discussion Status

The discussion includes attempts to clarify the problem and explore different methods for finding the velocities of the particles. One participant indicates they have resolved their confusion, while another expresses a desire for further clarification on the original poster's solution.

Contextual Notes

Participants are navigating the complexities of relativistic equations and the implications of conservation laws in the context of high-energy particle collisions. There is a focus on ensuring the correct application of principles without reaching a definitive conclusion.

szimmy
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Homework Statement


A particle and its anti-particle are directed toward each other, each with rest energy 1,000 MeV. We want to create a new particle with rest energy 10,000 MeV and total energy 100,000 MeV. What must the speed of the particle and antiparticle be before the collision.

ERest0 = m0c2 = 1,000 MeV
ERestFinal = 10,000 MeV
ETotal = 100,000 MeV

Homework Equations


γx = 1 / √[1 - (vx2 / c2)]

Conservation of Energy:
EInitial = EFinal
Conservation of Momentum:
PInitial = PFinal

Total energy:
ETotal = √[(pc)2 + (ERest)2]
ETotal = ERestγ

Relativistic Momentum for the particles:
PInitial = m0 / c2 * [v1γ1 + v2γ2]

Solving for momentum in terms of the total and rest energies:
PFinal = 1 / c * √[(ET)2 - (ERestFinal)2]

The Attempt at a Solution


First I laid out conservation of energy.
EInitial = EFinal
ERest01 + γ2] = 100,000 MeV
100 = γ1 + γ2

Then I solved for the final momentum using the expression above which is derived from the total energy formula.
PFinal = 1 / c * √[(100,000)2 + (10,000)2]
PFinal = 1 / c * 99,498 MeV

The I setup conservation of momentum.
PFinal = PInitial
1 / c * 99,498 MeV = m0 / c2 * [v1γ1 + v2γ2]

1 / c * 99,498 MeV / [1,000 MeV / c2] = [v1γ1 + v2γ2]

99.498c = [v1γ1 + v2γ2]

This is where I get stuck. I don't know whether I should attempt to solve for one of the velocities or just in general which step to take next. I tried solving by setting one of the velocities to zero but I'm not sure if this is the correct way to do it.

If I substitute v2 = 0:
γ2 = 1

100 = γ1 + 1
99 = γ1
√[1-(v12 / c2)] = 1 / 99
v12 / c2 = 1 - (1 / 99)2
v1 = √[1 - (1 / 99)2] c
v1 = .99995c

Is this answer right? v1 = .99995c and v2 = 0c

Can someone please either verify my answer or give me a step in the right direction? Thank you.
 
Last edited:
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I actually figured it out, no need to reply
 
Wait what did you do? I'm stuck.
 
It's generally better to work in terms of energy and momentum and then find velocities using ##v = E/p##. It simplifies the algebra.
 

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