In the Schutz book, "A First Course in General Relativity" (bottom of p.42 if you have it), it states the following:
For small v, the energy is:
E = po = m(1-v2)-(1/2) =(approx) m + (1/2)mv2
I can't figure out why this is! For small v, the LHS will tend to m, and the RHS will tend to m, so...