Relativistic kinetic energy - particle decay

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Homework Help Overview

The discussion revolves around the decay of a pion at rest into a muon and an antineutrino, focusing on calculating the kinetic energy of the muon and the energy of the antineutrino. The subject area includes concepts from relativistic physics, particularly relating to energy and momentum conservation in particle decay processes.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • The original poster attempts to calculate the kinetic energy of the muon based on the mass difference between the pion and muon, while questioning the assumption that the antineutrino's energy is negligible. Participants raise concerns about this assumption and discuss the implications of conservation laws in two-body decays.

Discussion Status

Participants are actively engaging with the original poster's reasoning, providing guidance on the necessity of considering conservation laws. There is a recognition that the lighter decay product, the muon, is expected to carry most of the kinetic energy, prompting further exploration of momentum and energy relations.

Contextual Notes

There is an ongoing discussion about the implications of the antineutrino's near-zero mass and how this affects the calculations. The original poster's approach may be constrained by assumptions about the energy distribution in the decay process.

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Homework Statement



A pion at rest (mπ = 273me) decays into a muon (mμ = 207me) and an antineutrino (mn ≈ 0).

Find (a) the kinetic energy of the muon and (b) the energy of the antineutrino in electron volts.

Homework Equations



K = (γ-1)mc2

E = γmc2

ER = mc2

E2 = p2c2 + (mc2)2

I didn't use all of these, but I'm assuming a solution requires one or more of them.

The Attempt at a Solution



Not really sure how to go about this when the mass of the neutrino is so close to zero. If I assume the total energy after the reaction of the neutrino is essentially zero, then the missing energy goes into the motion of the muon.

Kμ ≈ E - E
= c2 (mπ - mμ)
= c2 (0.511*106eV/c2)(273-207)
= 3.37*107 eV
= 33.7 MeV

The answer in the book is 4.08MeV so either my assumption that Kn ≈ 0 is a bad one, or I've made a mistake somewhere here.
 
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Yes, your assumption is bad. In fact, in a two body decay, the lighter decay product will carry most of the kinetic energy.

You need to fulfill the conservation laws involved, which are they?
 
Orodruin said:
Yes, your assumption is bad. In fact, in a two body decay, the lighter decay product will carry most of the kinetic energy.

You need to fulfill the conservation laws involved, which are they?

So momentum needs to be conserved, however the momentum is proportional to mass just like kinetic energy, which is what lead me to conclude the kinetic energy must be close to zero. How do I go about calculating the momentum of something for which I do not know the mass?
 
Momentum is only proportional to mass for fixed velocity < c. You can only draw the conclusion that a light particle has smaller energy or momentum than a heavy if they have the same speed.

You already have a relation between the momentum and total energy of a particle. This relation is true also for massless particles.
 

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