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Suppose a relativistic particle A with speed v relative to frame S decays into 2 particles B and C. One of these particles is

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Answer #1

Total energy of a relativistic particle

E2 = p2c2 + m2c4

pc is the KE energy and mc2 is the rest mass energy

particle A has a relativistic speed v ;

\gamma _a = 1/(1-v2/c2)1/2

(a) KE of the particle A = \gamma _amAc2 - mAc2 =  mAc2 /(1-v2/c2)1/2 -  mAc2

relativistic momentum pA = \gamma _amAv

after split particle B is at rest so, it total energy = mBc2  

In a relativistic momentum is conserved

pB =0

pc = pA = \gamma _amAv = \gamma _c

EA = mBc2 + Ec  

Total energy of the particle C

Ec = EA - mBc2 = sqrt( pA2c2 + mA2c4 ) - mBc2

KE of the particle C = Ec - mc2 = sqrt( m2Av2c2 /(1-v2/c2) + mA2c4 ) - mBc2 - mAc2  

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