SPECIFIC HEAT OF A GAS AT CONSTSNT VOLUME (CV)

SPECIFIC HEAT OF A GAS AT CONSTSNT PRESSURE (CP)

Heat (q) || Sign Convention || Unit Calculation OF Heat || total/Molar/Specific Heat Capacity || Process Dependent Heat Capacity (Cp,Cv) || Cp and Cv OF Ideal Gas || Degree OF Freedom

C_p and C_v are specific heats at constant pressure and constant volume respectively. It is observed that C_p - C_v = a for hydrogen gas C_p = C_V = b for nitrogen gas The correct relation between a and b is:

C_p and C_v are specific heats at constant pressure and constant volume respectively. It is observed that C_p - C_v = a for hydrogen gas C_p = C_V = b for nitrogen gas The correct relation between a and b is:

C_P and C_V are specific heats at constant pressure and constant volume respectively. it is observed that C_P - C_V=p for helium gas and C_P - C_V=q for Oxygen gas. The correct relation between p and q is

The molar specific heats of an ideal gas at constant pressure and volume arc denoted by C_P and C_V respectively. If gamma = (C_P)/(C_V) and R is the universal gas constant, then C_V is equal to

For hydrogen gas C_p-C_v=a and for oxygen gas C_p-C_v=b , C_p and C_v being molar specific heats. The relation between a and b is

For hydrogen gas C_p-C_v=a and for oxygen gas C_p-C_v=b , C_p and C_v being molar specific heats. The relation between a and b is

An ideal gas (C_p // C_V = (gamma) is taken through a process in which the pressure and the volume vary as P = aV^b . Find the values of (b) for which the specific heat capacity of the gas for the process is zero.

Show that for an ideal gas C_p - C_v = R where C_p and C_v are the heat capacity at constant pressure and constant volume respectively.