We examine the target mass number (A) dependence of the nuclear transp
arency calculated for (e, e' p) reactions. Generally, the transparency
is proportional to A(-1/3) for large A's and has weaker A-dependence
as A decreases. The conventional nuclear physics calculation yields a
transparency whose A(-1/3) dependence is reached in rather light nucle
i (around A = 20). If either the proton mean-free path in nuclei becom
es substantially longer, or the internal structure of the proton is ex
plicitly incorporated in the calculation, however, the A(-1/3) depende
nce is reached only in extremely heavy nuclei. The A-dependence should
thus serve as a signature of the so-called color-transparency phenome
non.