As is well known, the requirement that gamma-ray bursts be optically thin t
o high-energy photons yields a lower limit on the Lorentz factor (gamma) of
the expansion. In this paper, we provide a simple derivation of the lower
limit on gamma due to the annihilation of photon pairs and correct the erro
rs in some of the previous calculations of this limit. We also derive a sec
ond limit on gamma due to scattering of photons by pair-created electrons a
nd positrons. For some bursts, this limit is the more stringent. In additio
n, we show that a third limit on gamma, obtained by considering the scatter
ing of photons by electrons that accompany baryons, is nearly always less i
mportant than the second limit. Finally, we evaluate these limits for a num
ber of bursts.