Steady cool fronts supported by nonsaturated thermal conduction in opticall
y thin plasmas are analyzed. Explicit relations for the pressure (p(2)), nu
mber density (n(2)), temperature (T-2), and flow velocity (v(2)) behind the
front are found as functions of the temperature T-1 and the intake Mach nu
mber M-1 ahead of the cool front. Weak cool fronts may exist only for intak
e velocities less than the isothermal sound speed. Behind these kinds of fr
onts, the flow retards, cools down, and is compressed. Strong cool fronts e
xist for intake Mach numbers greater than a threshold value depending on T-
1. In these fronts, two compression branches appear, a high-compression bra
nch well below the isotherm for which n(1)/n(2) < (gamma - 1)/(gamma + 1) a
nd a weak-compression branch, close to (but below) the isotherm. In particu
lar, in the high-compression branch for low values of M. quasi-isobaric coo
l fronts occur when the ratio n(1)/n(2) close to the maximum value, where t
his branch just emerges, beyond which the pressure of the flow behind the f
ront increases when n(1)/n(2) decreases. The implications of these results
on the formation of cool condensations in the hot interstellar medium gas a
nd in the solar atmosphere are outlined.