Put
Δr=r2−r1. Expanding the
quotient S/T consistently to
first order gives
veff=1+r2M−ΔrMlogr1r2.
Thus
veff=1+r2M−r2−r1Mlogr1r2.
Because
log(r2/r1)/(r2−r1)→1/r2 as r1→r2,
This local limit is the expected
speed of
a massless particle measured in
a freely falling
local inertial frame; the finite-interval effective
velocity combines nonlocal
length and
clock comparisons.