Davis L A, Martínez G A, Hassoun T H, Vrubel N K
Magnetic Resonance Imaging Petrophysical Applications Center, Petroleum Engineering Department, Box 43111, Texas Tech University, Lubbock, TX 79409, USA.
Magn Reson Imaging. 2001 Apr-May;19(3-4):369-73. doi: 10.1016/s0730-725x(01)00250-8.
This work investigates the effects of modulation of the transverse and longitudinal relaxation of the surface-fluid/pore-fluid spin system in porous media. Important new NMR well logging applications identify pore fluids by varying the CPMG T(2) pulse spacing to discriminate on the basis of fluid diffusivities in applied and local static magnetic field gradients. However, anomalous laboratory CPMG T(2) results have been reported repeatedly over 25 years for various porous media filled with a single fluid. In relatively large pores, at near bulk conditions, the transverse relaxation of diffusing molecular spins should be proportional to the square of the CPMG pulse spacing tau, the susceptibility contrast at the pore wall and the applied gradient. Observed is a markedly linear tau dependence that saturates at a plateau for large tau. The effect is not quadratic in applied gradient or susceptibility. For large pores, the tau dependence and the saturation value are proportional to the surface-to-volume ratio of the pores. This is in distinct contrast to the behavior observed by Borgia, Brown and Fantazzini for systems with much smaller pores at higher magnetic fields. The large-pore anomalous behaviors can be explained as a modulation of the exchange between surface-fluid and pore-fluid spins, such as observed by Luz and Meiboom in 1963 for water enriched with quadrupolar 17O. Scalar coupling of the solid-surface spins to the fluid-surface spins was postulated by Kleinberg, Kenyon and Mitra as a dominant relaxation mechanism for the surface fluid. The CPMG tau effect can be described as the modulation of the exchange coupling by the CPMG pi pulses, which mix the magnetizations between the exchanging, strongly coupled spin systems of the pore-fluid and the surface-fluid, which is, in turn, weakly coupled by scalar or pseudo-scalar interactions to the fast-relaxing solid surface.
本研究探讨了多孔介质中表面流体/孔隙流体自旋系统横向和纵向弛豫调制的影响。重要的新型核磁共振测井应用通过改变CPMG T(2)脉冲间隔来识别孔隙流体,以便根据外加和局部静磁场梯度中的流体扩散率进行区分。然而,在过去25年里,针对各种充满单一流体的多孔介质,实验室中反复报道了异常的CPMG T(2)结果。在相对较大的孔隙中,在接近体相条件下,扩散分子自旋的横向弛豫应与CPMG脉冲间隔tau的平方、孔隙壁处的磁化率对比度以及外加梯度成正比。观察到的是明显的线性tau依赖性,对于大tau值,其在一个平台上达到饱和。该效应在外加梯度或磁化率方面并非二次方关系。对于大孔隙,tau依赖性和饱和值与孔隙的表面积与体积之比成正比。这与Borgia、Brown和Fantazzini在更高磁场下对孔隙小得多的系统所观察到的行为形成鲜明对比。大孔隙的异常行为可以解释为表面流体和孔隙流体自旋之间交换的调制,就像1963年Luz和Meiboom在富含四极17O的水中所观察到的那样。Kleinberg、Kenyon和Mitra假定固体表面自旋与流体表面自旋的标量耦合是表面流体的主要弛豫机制。CPMG tau效应可以描述为CPMG π脉冲对交换耦合的调制,该脉冲混合了孔隙流体和表面流体的交换的、强耦合自旋系统之间的磁化强度,而这两个自旋系统又通过标量或伪标量相互作用与快速弛豫的固体表面弱耦合。