Spin Echo Analysis of Restricted Diffusion under Generalized Gradient Waveforms: Planar, Cylindrical, and Spherical Pores with Wall Relaxivity.

A simple matrix formalism presented by Callaghan [J. Magn. Reson. 129, 74-84 (1997)], and based on the multiple propagator approach of Caprihan et al. [J. Magn. Reson. A 118, 94-102 (1996)], allows for the calculation of the echo attenuation, E(q), in spin echo diffusion experiments, for practically all gradient waveforms. We have extended the method to the treatment of restricted diffusion in parallel plate, cylindrical, and spherical geometries, including the effects of fluid-surface interactions. In particular, the q-space coherence curves are presented for the finite-width gradient pulse PGSE experiment and the results of the matrix calculations compare precisely with published computer simulations. It is shown that the use of long gradient pulses (delta approximately a2/D) create the illusion of smaller pores if a narrow pulse approximation is assumed, while ignoring the presence of significant wall relaxation can lead to both an underestimation of the pore dimensions and a misidentification of the pore geometry. Copyright 1999 Academic Press.

[1]  J. Jehng,et al.  Surface magnetic relaxation in cement pastes. , 1994, Magnetic resonance imaging.

[2]  P. Callaghan Principles of Nuclear Magnetic Resonance Microscopy , 1991 .

[3]  Schwartz,et al.  Short-time behavior of the diffusion coefficient as a geometrical probe of porous media. , 1993, Physical review. B, Condensed matter.

[4]  Fernando Zelaya,et al.  Diffusion in porous systems and the influence of pore morphology in pulsed gradient spin-echo nuclear magnetic resonance studies , 1992 .

[5]  Sen,et al.  Effects of microgeometry and surface relaxation on NMR pulsed-field-gradient experiments: Simple pore geometries. , 1992, Physical review. B, Condensed matter.

[6]  E. Fukushima,et al.  Spatially Resolved Magnetic Resonance , 1998 .

[7]  Callaghan,et al.  A simple matrix formalism for spin echo analysis of restricted diffusion under generalized gradient waveforms , 1997, Journal of magnetic resonance.

[8]  G. Arfken Mathematical Methods for Physicists , 1967 .

[9]  Klaus Schulten,et al.  Edge enhancement by diffusion in microscopic magnetic resonance imaging , 1992 .

[10]  J. E. Tanner,et al.  Spin diffusion measurements : spin echoes in the presence of a time-dependent field gradient , 1965 .

[11]  E. Stejskal Use of Spin Echoes in a Pulsed Magnetic‐Field Gradient to Study Anisotropic, Restricted Diffusion and Flow , 1965 .

[12]  P. Callaghan,et al.  Diffraction-like effects in NMR diffusion studies of fluids in porous solids , 1991, Nature.

[13]  Dunn,et al.  Self-diffusion in a periodic porous medium with interface absorption. , 1995, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[14]  R. Kleinberg Utility of NMR T2 distributions, connection with capillary pressure, clay effect, and determination of the surface relaxivity parameter rho 2. , 1996, Magnetic resonance imaging.

[15]  K. Brownstein,et al.  Importance of classical diffusion in NMR studies of water in biological cells , 1979 .

[16]  Paul C. Lauterbur,et al.  Effects of restricted diffusion on microscopic NMR imaging , 1991 .