We employ the Monte Carlo method for the calculation of anomalous tran
sport developed by Punjabi and Boozer to calculate the particle diffus
ion coefficient for electrons in the stochastic magnetic fields of the
reversed-field pinch (RFP), In the Monte Carlo calculations represent
ed here, the transport mechanism is the loss of magnetic surfaces due
to resistive perturbations. The equilibrium magnetic fields are repres
ented by the Bessel function model for the RFP. The diffusion coeffici
ent D is calculated as a function of a, the amplitude of the perturbat
ion. We see three regimes as the amplitude of the tearing modes is inc
reased: the Rechester-Rosenbluth regime where D scales as a(2); the an
omalous regime where D scales more rapidly than a(2); and the Mynick-K
rommes regime where D scales more slowly than a(2). Inclusion of the e
ffects of loop voltage on the particle drift orbits in the RFP does no
t affect the intervals in the amplitude a where these regimes operate.