We calculate the electrostatic persistence length l(e) both for flexib
le and for stiff polyelectrolytes using a self-consistent variational
theory. For the case of intrinsically rigid polyelectrolytes we recove
r the classical results due to Odijk, Skolnick, and Fixman (OSF), name
ly, l(e) proportional to kappa(-2) where kappa(-1) is the Debye screen
ing length. In contrast, l(e) for intrinsically flexible polyelectroly
tes is found to be proportional to kappa(-1) in the limit of large scr
eening. This is in accord with simulations, experiments, and numerical
estimates. We also provide a criterion for the crossover from the OSF
result to the behavior observed for intrinsically flexible polyelectr
olytes.