Following the restricted model in the preceding part, its electronic factor for independent magnetic molecules is . Its field-dependent Helmholtz free energy is therefore
where denotes terms independent of the field. Equivalently, the change from zero field is . Retaining the excited-state offset simply adds to the restricted free energy.
If instead counts all molecules in thermal equilibrium, the correct electronic expression is
The ordinary translational indistinguishability factor is field independent and does not alter either magnetic derivative.

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