  The thermodynamics of ideal gas on the noncommutative geometry in the
coherent state formalism is investigated. We first evaluate the statistical
interparticle potential and see that there are residual "attraction (repulsion)
potential" between boson (fermion) in the high temperature limit. The
characters could be traced to the fact that, the particle with mass $m$ in
noncommutative thermal geometry with noncommutativity $\theta$ and temperature
$T$ will correspond to that in the commutative background with temperature
$T(1+kTm\theta)^{-1}$. Such a correspondence implies that the ideal gas energy
will asymptotically approach to a finite limiting value as that on commutative
geometry at $T_\theta= (km\theta)^{-1}$. We also investigate the squeezed
coherent states and see that they could have arbitrary mean energy. The thermal
properties of those systems are calculated and compared to each other. We find
that the heat capacity of the squeezed coherent states of boson and fermion on
the noncommutative geometry have different values, contrast to that on the
commutative geometry.
