Expert Answer
To show that for an ideal gas, the relation Cp = Cv + nR holds using the given equation , we can apply the ideal gas law and the definition of specific heat capacities.Starting with the given equation: We know that for an ideal gas, the specific heat capacities are defined as follows:
(heat capacity at constant pressure)
(heat capacity at constant volume)Using the first law of thermodynamics, we have:
(change in heat energy = change in internal energy + work done)For an ideal gas, the change in internal energy (dU) only depends on the change in temperature (dT). Therefore, we can write:
Substituting this into the equation for heat capacity at constant pressure (Cp), we have:
Cp = (?Q/?T)p = dU/dT + P(dV/dT)pNow, let's consider the ideal gas law:
PV = nRTTaking the partial derivative of this equation with respect to time (t) at constant volume (V), we get:
V(?P/?t)v = nRSubstituting this into the expression for Cp, we have:
Cp = dU/dT + P(dV/dT)p
= Cv + (nR/V)(dV/dT)pSince nR/V = P (using the ideal gas law), we have:
Cp = Cv + P(dV/dT)pTherefore, for an ideal gas, the relation Cp = Cv + nR holds true.Now, to express the relation in terms of the number of moles (n) and the ideal gas constant (R), we can use the ideal gas law:
PV = nRTSolving for P, we have:
P = nRT/VSubstituting this back into the equation for Cp, we get:
Cp = Cv + P(dV/dT)p
= Cv + (nRT/V)(dV/dT)pSince the partial derivative (?V/?T)p represents the change in volume with respect to temperature at constant pressure, it is related to the thermal expansion coefficient (?) of the gas:
(?V/?T)p = V?Therefore, we have:
Cp = Cv + P(dV/dT)p
= Cv + P(V?)
= Cv + nRT?/V
= Cv + nR?So, the relation for an ideal gas can be expressed as:
Cp = Cv + nRThus, we have shown that for an ideal gas, Cp = Cv + nR, which is the well-known relationship between the specific heat capacities.