We present a theory to calculate, first, the correlation function of the physical quantity (angular momentum for spin-rotation interaction, second order spherical harmonics for the dipolar interaction), involved in magnetic spin-lattice relaxation and then the relaxation times. The time behaviour of the physical quantity h(t) is described by a generalized Langevin equation whose memory function, K(t), is assumed to be proportional to the density fluctuation correlation function, N(t). The time-independent proportionality function, ~, is obtained by assuming that the relaxation time Tn (for h(t) to reach local equilibrium) is equal to the correlation time, ~'n, of the density fluctuations. The density fluctuation correlation function is calculated by using the classical hydrodynamics form of the structure factor S(q, to) [1,2]. The definition chosen for N(t) forces us to consider only temperatures above the critical temperature, since we do not know the particle density of the liquid below the critical temperature.The ~-dependence of the memory function, the total effect correlation function and the normalized power spectrum is presented. Once the choice of ~ is made (~ is temperature dependent), the main result of the theory is to give a minimum, above the critical temperature, for the spinlattice relaxation times. The variation law (ATocto 1/*) of the shift, AT, in the temperature of the minimum from the critical temperature with respect to the frequency, found experimentally by Krynicki et al. [2], is verified. But while this result is consistent with experimental T1 measurements for CHC13, it is not with those for HCI (and H2S) : for dipolar and spin-rotation interaction we found a similar temperature dependence.