Abstract
Porous media containing fluids and subject to the field of an NMR instrument usually have incremental local magnetic fields due to susceptibility differences χd, such as between a fluid and a solid matrix. If ‖χd‖≪1 the effective variation ω of the local precession angular frequency is limited to ±1/2χd ω0, where ω0 is the mean precession angular frequency. Diffusion of fluid molecules through these local fields leads to a τ-dependent increase Rd in the value of 1/T2 obtained from Carr-Purcell-Meiboom-Gill (CPMG) measurements. Many porous media appear likely to have significant ω variation over a substantial range of diffusion time scales, or correlation times. For a sample with a single correlation time τc the logarithm of the additional decay of the nth echo amplitude due to diffusion through regions of different ω is Ω2 τc{2nτf(τ/τc)-τc[(1-x)4/(1+x2 )2] [1-(-)n x2n]}, where f(t)=1-(tanht)/t, Ω2=〈ω2〉, and x=exp(-τ/τc). The term without n causes only a shift in the relaxation curve, and the terms in x2n are small, so RdΩ2 τcf(τ/τc). The function f(t) starts quadratically at small t, has a nearly linear portion, and then approaches 1-1/t at large t. However, the superposition of terms of the form f(τ/τci) tends to give a nearly linear portion of the Rd vs τ curve extending from small values of Rd to about a third of the asymptotic value if there is a significant range of τci.