“…However, if diffusion takes place, the diffusing nucleus will feel a change in the magnetic field and in the resulting phase it experiences, and the signal will be reduced. This change in phase results in attenuation of the magnetization M. In the case of free Gaussian diffusion, the theoretical expression of echo attenuation, for a selected NMR peak integral intensity, is given by the Stejskal-Tanner equation [17,22]: where D is the self-diffusion coefficient, g is the gradient strength (Gauss/cm or Tesla/m), and d and D are the time duration of the applied gradient pulse and the interval between gradient pulses, respectively. I(g) is the signal intensity at t ¼ 2t in the presence of gradient pulses of strength g, while I(0) is the intensity in the absence of any gradient pulses.…”