CHAP. 3: FUNDAMENTALS OF THERMODYNAMICS [CONTENTS] 68
3.2 Definition of fundamental thermodynamic quantities
T,p,V,n,U,Sas defined in the preceding sections represent basic thermodynamic functions.
In this section we will define further basic thermodynamic functions: enthalpy, Helmholtz
energy, Gibbs energy, heat capacities and fugacity.
3.2.1 Enthalpy.
EnthalpyHis a function of state defined by the relation
H=U+pV. (3.9)
U Main unit:J.
Note:Similarly as internal energy, enthalpy is defined up to the additive constant.
If a system exchanges only heat and reversible volume work with its surroundings during a
thermodynamic process [see4.1.1], we have
dH= ̄dQ+Vdp. (3.10)
If this process is isobaric (dp= 0), the change in the enthalpy of a system is equal to the heat
supplied to the system
∆H=Q , [p]. (3.11)
Example
A system containing 5 moles of an ideal gas was heated from temperatureT 1 = 300 K to
temperatureT 2 = 400 K. The internal energy of the gas increased by∆U= 800 J. How did the
enthalpy of the system change?