The spectrum of a passive temperature field, G(k), has been determined by a numerical
simulation using three kinds of isotropic turbulent velocity fields. For a time independent and
Gaussian velocity field, the resulting G(k) has the form ,
with G0 ~ 0.33 Ko , confirming the prediction of Batchelor, Howells
and Townsend [J. Fluid Mech. 5, 134 (1959)]. For a velocity field developed through the
Navier-Stokes equations and then frozen in time, G(k) has the same form as above, but with
G0~ 0.39 Ko. Finally, for a velocity field developed concurrently with
the temperature field, G(k) collapses onto the spectrum obtained using a frozen, developed
velocity field only for high enough values of the conductivity.
For lower values of the conductivity, the power law behavior of G(k) is less clear.