Relation Between Enthalpy (H) and Internal Energy (U)
Let H1, U1, V1 be the enthalpy, internal energy and volume of the system in the initial state and H2, U2, V2 be the corresponding values in the final state.
We know that, Enthalpy
H = U + PV
in the initial state
H1 = U1 + PV1 --- Equation:1
in the final stete
H2 = U2 + PV2 --- Equation:2
Subtracting equation:1 from equation:2 we get
H2 − H1 = (U2 + PV2) − (U1 + PV1)
ΔH = (U2 − U1) + P(V2 − V1)
ΔH = ΔU + PΔV
where, ΔH is change in enthalpy, ∆U is change in internal energy, and P∆V is change in work energy.
Thus, the change in enthalpy at constant pressure is equal to the increase in internal energy plus pressure-volume work done (work energy).
For, ideal gas, we know that PV = nRT
Putting the value of PV in the above equation we get
ΔH = ΔU + Δn.RT
This equation shows that the change in enthalpy is equal to the change in internal energy plus changes in moles at constant temperature and pressure.