  The quantum-classical limits for quantum tomograms are studied and compared
with the corresponding classical tomograms, using two different definitions for
the limit. One is the Planck limit where $\hbar \to 0$ in all $\hbar
$-dependent physical observables, and the other is the Ehrenfest limit where
$\hbar \to 0$ while keeping constant the mean value of the energy.The Ehrenfest
limit of eigenstate tomograms for a particle in a box and a harmonic
oscillatoris shown to agree with the corresponding classical tomograms of
phase-space distributions, after a time averaging. The Planck limit of
superposition state tomograms of the harmonic oscillator demostrating the
decreasing contribution of interferences terms as $\hbar \to 0$.
