If ε represents the energy of one molecule, then
|
1.16 |
If N is the number of molecules in the system, then the total internal energy is
|
1.17 |
For an ideal gas there are no intermolecular forces of attraction and repulsion, and the internal energy depends only on temperature. Thus, for an ideal gas
U = ƒ(T) |
1.18 |
Other forms of energy which can also be possessed by a system are magnetic energy, electrical energy and surface tension energy. In absence of these forms, the total energy E of a system is given by
E = (EK + EP) + U |
1.19 |
where EK + EP Macro energy and U = Micro energy.
In absence of motion and gravity,
EK = 0, EP = 0 |
1.20 |
Hence,
E = U |
1.21 |
Hence, Eq. (1.4) becomes
Q = ΔU + W |
1.22 |
For open system, the enthalpy H = U + pV is a property. The specific enthalpy h = u + pv is an intensive property.