FRACTAL-DIMENSION CROSSOVERS IN TURBULENT PASSIVE SCALAR SIGNALS

The fractal dimension delta(g)(1) of turbulent passive scalar signals is calculated from the fluid dynamical equation delta(g)(1) depends on the scale. For small Prandtl (or Schmidt) number Pr < 10(-2) one gets two ranges, delta(g)(1)= 1 for small-scale r and delta(g)(1)= 5/3 for large r, both as expected. But for large Pr > 1 one gets a third, int ermediate range in which the signal is extremely wrinkled and has delt a(g)(1) = 2. In that range the passive scalar structure function D(the ta)(r) has a plateau. We calculate the Pr-dependence of the crossovers . The plateau regime can be observed in a numerical solution of the fl uid dynamical equation, employing a reduced wave vector set approximat ion introduced by us recently.