A three-dimensional resistive magnetohydrodynamic code has been used t
o model the reconnection process at the m=1, n=1 surface, in periodic
cylindrical geometry. Large current densities are expected at this rec
onnection layer and an enhancement of the transport properties is expe
cted if the local drift speed exceeds a critical velocity, such as som
e multiple of the local sound speed. This effect is modeled in these s
imulations by the local enhancement of the resistivity coefficient whe
re the criterion for micro-turbulence is satisfied. It is found that t
he reconnection times for this type of simulation are comparable to th
e reconnection times for a plasma where the resistivity is enhanced ev
erywhere, implying that the reconnection is dominated by the local res
istivity value and not its gradient. An analytic scaling law of the re
connection rate for the case when the local electron drift velocity is
Limited to a multiple of the sound speed is presented. This model pre
dicts that when this multiple is (m(i)/m(e))(1/2), reconnection times
are close to experimental values in large tokamaks. Under these condit
ions, electron inertia and electron viscosity can be shown to be unimp
ortant. The onset of micro-turbulence acts as a trigger for the reconn
ection process, and partial reconnection can occur if the conditions f
or micro-turbulence cease. (C) 1998 American Institute of Physics. [S1
070-664X(98)02309-X].