A process in which pressure remains constant is called an isobaric process. Consider n moles of a gas enclosed in a cylinder fitted with a movable, massless and frictionless piston. We assume that the gas behaves as an ideal gas so that we can use the equation of state PV = nRT.

Consider an isobaric expansion (or compression) of the gas in which the volume of the gas changes from Vi to Vf and the temperature of the gas changes from Ti to Tf when the pressure (P) of the gas is kept constant. The work done by the gas,

Now, PVi = nRTi and PVf = nRTf
∴ PVf – PVi = nRTf – nRTi
∴ P(Vf – Vi) = nR(Tf – Ti)
∴ from Eq. (1), W = nR(Tf – Ti) … (2)
The change in the internal energy of the gas,
∆ U = nC (T – T ) …(3)
where Cv is the molar specific heat of the gas at constant volume.
From Eqs. (2) and (3),
we have, the heat supplied to the gas,
Q = ∆ U + W = nCv (Tf – Ti) + nR(Tf – Ti)
= n(Cv + R)(Tf – Ti)
∴ Q = nCp (Tf – Ti) …(4)
Where Cp ( = Cv + R) is the molar specific heat of the gas at constant pressure.
[Note : P-V curve for an isobaric process is called an isobar.