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Actually, no, but you're on the right track. The molar enthalpy of a pure single phase substance can be expressed uniquely as a function of temperature T and pressure P: h = h(T,P). The molar heat capacity Cp is, by definition, the partial derivative of h with respect to T at constant P:Tomdickjerry said:alright thanks! for the left side do i just use cv(t2-t1) i figured since the it isn't constant pressure process
$$C_p\equiv \left(\frac{\partial h}{\partial T}\right)_P$$For an ideal gas, molar enthalpy is a function only of temperature T. So the partial derivative becomes a total derivative: $$\frac{dh}{dT }=C_p$$For an ideal gas, this equation applies even if the pressure is not constant. The quantity ##C_p## is called the heat capacity at constant pressure only because, in measuring ##C_p## experimentally, not only is the change in enthalpy dh at constant pressure equal to ##C_pdT##, but so also is the amount of heat added dQ. So, under constant pressure conditions, ##C_p## can be measured experimentally by directly determining the amount of heat added. If the pressure is not constant, then dQ is not equal to ##C_pdT## but dh (for an ideal gas) is still equal to CpdT.
So, since for an ideal gas, dh is always equal to ##C_pdT##, irrespective of whether the pressure is constant, we have:
$$(h-h_{in})=C_p(T-T_{in})$$where h is the final molar enthalpy of the air in the cylinder, ##h_{in}## is the molar enthalpy of the air in the tank, T is the final temperature of the air in the cylinder, and ##T_{in}## is the temperature of the air in the tank (27 C = 300 K).
Now m is the final number of moles of air in the cylinder. From the ideal gas law, please (algebraically) express m as a function of PV, R, and T, where R is the universal gas constant.
Air is a diatomic gas. In the ideal gas region, how is the molar heat capacity ##C_p## of a diatomic ideal gas related to the ideal gas constant R?
Chet