What is the rest mass of the composite particle after a relativistic collision?

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SUMMARY

The discussion centers on calculating the rest mass of a composite particle resulting from a relativistic collision involving a stationary particle with rest mass 2m0 and another particle with rest mass m0 and kinetic energy 2m0c2. The key equations utilized include conservation of momentum and energy, specifically m0γ(u)u = M0qγ(q) and m0γ(u) + 2m0 = M0γ(q). The challenge lies in determining the ratio M0/m0, which is critical for solving the problem.

PREREQUISITES
  • Understanding of relativistic mechanics
  • Familiarity with the concepts of rest mass and kinetic energy
  • Knowledge of conservation laws in physics
  • Ability to manipulate Lorentz factors (γ)
NEXT STEPS
  • Study the derivation of the Lorentz factor (γ) in relativistic physics
  • Learn about the conservation of momentum and energy in relativistic collisions
  • Explore examples of composite particle mass calculations in relativistic contexts
  • Investigate the implications of relativistic mass versus rest mass
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Students of physics, particularly those studying relativistic mechanics, and educators looking for clear explanations of composite particle behavior in collisions.

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Homework Statement



A stationary particle of rest mass [tex]2m_{0}[/tex] is hit by a particle of rest mass [tex]m_{0}[/tex] and kinetic energy [tex]2m_{0} c^{2}[/tex]. I must find the rest mass of the composite particle afterward.

Homework Equations



Conservation of momentum and energy.

The Attempt at a Solution



I worked problems with identical mass and velocity, but I don't exactly know what to do with this particular problem. I'm still having trouble understanding the explanation my book provided, so I was hoping someone can give me a more lucid elaboration of this whole phenomenon.
 
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This is what I have so far.

[tex]m_{0} \gamma (u) u = M_{0} q \gamma(q)[/tex]

[tex]m_{0} \gamma (u) + 2m_{0} = M_{0} \gamma (q)[/tex]

[tex]M_{0}[/tex] is the rest mass of the composite particle, [tex]q[/tex] its velocity, and [tex]u[/tex] the velocity of the inertial particle before it strikes the stationary one.

The problem is the ratio [tex]\frac{M_{0}}{m_{0}}[/tex], which is what I need, is eliminated.

I don't know where to proceed from here.
 

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