In this paper a non-equilibrium statistical-mechanical theory of dielectric
relaxation is developed. This approach differs from previous work in that
a generalized nonlocal evolution equation for the polarization is construct
ed. General equations of motion are presented for the polarization, interna
l energy, and entropy which include effects of memory. These equations can
be expressed in terms of reduced-correlation functions, and are valid for n
on-equilibrium and arbitrary field strengths. Expressions for an effective
local field also are developed. The Fourier transform of the evolution equa
tion yields a general compact expression for the Fourier transform of the m
emory function and a specific form for the susceptibility. The kernel, Four
ier transform of the memory function are developed, and relaxation-time fun
ctions for special cases. In the limit of a single relaxation time, a Debye
response is obtained. In the subsequent special cases exponential and Gaus
sian forms for the memory functions are assumed. The final special case rel
ates a power-law circuit transfer function to the theory of Dissado and Hil
l. In this case the memory kernel and relaxation times are derived from the
Dissado-Hill response function.