Transients of dielectric relaxation for an assembly of noninteracting
rigid molecules acted on by a pure alternating stimulus of the form E(
t)=E(O) cos omega t are calculated up to the third order in the electr
ic field strength. Both permanent and induced dipole moments are consi
dered which leads to a nonlinear response characterized by a mixture o
f harmonics in omega, 2 omega, and 3 omega, and of exponential terms s
uch that exp(-2Dt) and exp(-6Dt), where D represents the rotational di
ffusion constant. The time-dependent behavior of the electric polariza
tion which is given by the expected value of the first Legendre polyno
mial < P-1(u)>(t) is obtained from solving the Smoluchowski equation.
When one restricts up to terms in E(3), it is shown that the nonlinear
dielectric response depends on the ensemble average of the second Leg
endre polynomial (appropriate to Kerr effect relaxation) whose only te
rms proportional to E(2) are retained. The evolution of < P-1(u)>(t) i
s presented in some figures for different values of omega and the para
meter P which reflects the balance between permanent and induced dipol
ar moments. All these curves are compared with the corresponding linea
r responses in order to emphasize their differences in the establishme
nt of the phenomenon and in the stationary regime.