PX155 - I5 - relativistic kinetic energy

EK=∫F.dx=∫dpdtdxdt.dt=∫vdpdt.dt EK=vp−∫pdvdt.dt=vp−∫p.dv EK=m0v2(1−v2c2)12−∫0vm0v(1−v2c2)12.dv ddv(1−v2c2)12=−2vc212(1−v2c2)−12=−vc21(1−v2c2)12 EK=m0v2(1−v2c2)12−−+m0c2[(1−v2c2)12]0vEK=m0v2(1−v2c2)12+m0c2(1−v2c2)12−m0c2EK=γm0c2−m0c2∴EK=(γ−1)m0c2

equivalence of mass and energy

Δm0=2(γ−1)m0=ΔEKc2

- before collision:

EK=2(γ−1)m0c2

- after collision:

EK=0ΔEK=2(γ−1)m0c2=Δm0c2 E0=m0c2 ∴E=mc2