For a perfect gas, the internal energy (\(U\)) and enthalpy (\(H\)) are functions of temperature only. Their changes are given by \(\Delta U = m c_v \Delta T\) and \(\Delta H = m c_p \Delta T\), where \(c_v\) and \(c_p\) are the specific heats at constant volume and pressure, respectively, and are assumed to be constant.
