We present calculations of frictional heating by ion-neutral drift in three
-dimensional simulations of turbulent, magnetized molecular clouds. We show
that ambipolar drift heating is a strong function of position in a turbule
nt cloud, and its average value can be significantly larger than the averag
e cosmic-ray heating rate. The heating rate per unit volume due to ambipola
r drift, H-AD = \J x B\(2)/rho(t)nu(ln) similar to B-4/(16 pi(2)L(B)(2)rho(
i)nu(in)), is found to depend on the rms Alfvenic Mach number, M-A,, and on
the average field strength, as H-AD proportional to M-2(A)<\ B \>(4) This
implies that the typical scale of variation of the magnetic field, L-B, is
inversely proportional to M-A, which we also demonstrate.