When molecules are subjected to an external electric held, static or r
adiative, the interaction with either permanent or induced dipole mome
nts creates pendular eigenstates, directional superpositions or hybrid
s of the field-free rotational states. These hybrids reflect the aniso
tropy of the interaction; for a linear molecule this is proportional t
o cos theta for a permanent dipole and to cos(2) theta for an induced
dipole, with theta the angle between the molecular axis and the held d
irection. In the weak-field regime, the molecular axis tumbles through
360 degrees, but in the strong-field limit it is confined to harmonic
librations about the held direction. Here we treat the statistical me
chanics of pendular states of linear molecules, either polar (with a p
ermanent dipole moment mu) or nonpolar but polarizable (with a polariz
ability anisotropy Delta alpha contributing to an induced dipole momen
t). The partition function and the thermodynamic properties and other
ensemble averages can be specified by two reduced variables involving
mu or Delta alpha, the held strength, rotational constant, and tempera
ture. A simple approximation due to Fitter enables the partition funct
ion to be cast in terms of the classical result with quantum correctio
ns derived from the harmonic librator limit. This provides explicit an
alytic formulas which permit thermodynamic properties to be evaluated
to good accuracy without computing energy levels and state sums. We al
so evaluate the average orientation or alignment of the molecular dipo
les and examine held-induced shifts of chemical equilibria.