
Arturo O. answered 08/12/17
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A good approach is to begin with the calculation of work, which gives kinetic energy. Use relativistic mass.
K = W = ∫Fdx
F = d(mv)/dt = mdv/dt + vdm/dt
K = ∫(mdv/dt + vdm/dt)dx
m = m0/√(1 - v2/c2)
m2(1 - v2/c2) = m02
m2c2 - m2v2 = m02c2
Take d/dt of the above.
2c2mdm/dt - 2mv2dm/dt - 2m2vdv/dt = 0
Divide through by 2mv.
c2(1/v)dm/dt - vdm/dt - mdv/dt = 0
Rearrange.
mdv/dt + vdm/dt = c2(1/v)dm/dt
v = dx/dt ⇒ 1/v = dt/dx
mdv/dt + vdm/dt = c2(dt/dx)(dm/dt) = c2dm/dx
mdv/dt + vdm/dt = c2dm/dx
Now put this in the K integral.
K = ∫(mdv/dt + vdm/dt)dx = ∫(c2dm/dx)dx = c2∫dm = c2(mf - mi)
If the particle starts from rest, mi = m0. But when it reaches speed v,
mf = m0/√(1 - v2/c2)
Therefore,
K = c2[m0/√(1 - v2/c2) - m0] = m0c2/√(1 - v2/c2) - m0c2
Rearrange.
K + m0c2 = m0c2/√(1 - v2/c2)
The left hand side is some kind of total energy E.
E = K + m0c2
Since K = kinetic energy, K ≠ 0 if the particle is moving, and K = 0 if the particle is at rest. Then when the particle is at rest,
E = m0c2