The specific heat at constant pressure is denoted by CP, and the specific heat at constant volume by CV.
The work done on a gas when it is heated at a constant volume raises the system’s internal energy. When a gas is heated at constant pressure, work is done to overcome the pressure, and the system’s internal energy increases as the volume expands. Consequently, it can be concluded that Cp exceeds Cv.
Regarding an ideal gas,
Cp – Cv = R.
Therefore, it is also mathematically possible to demonstrate that Cp exceeds Cv.
The specific heat at constant pressure is denoted by CP, and the specific heat at constant volume by CV.
The work done on a gas when it is heated at a constant volume raises the system’s internal energy. When a gas is heated at constant pressure, work is done to overcome the pressure, and the system’s internal energy increases as the volume expands. Consequently, it can be concluded that Cp exceeds Cv.
Regarding an ideal gas,
Cp – Cv = R.
Therefore, it is also mathematically possible to demonstrate that Cp exceeds Cv.