- #1
kent davidge
- 933
- 56
Let ##u^\alpha## and ##p^\alpha## denote a massive particle's four velocity and four momentum, respectively. Also, let ##\xi^\alpha = (1,0,0,0)## be a time like Killing vector. Since ##g_{00} \xi^0 u^0 = g_{00} p^0 / m = -(1 - 2m / r) E / m## is conserved, if we let ##r \longrightarrow \infty## we have that ##E / m## is conserved. This is the particle's energy per mass. But how to think about that term when ##r## is finite? What's the quantity that's being conserved there?