首页> 外文会议>Transactions of the SPWLA >PARAMAGNETIC RELAXATION IN SANDSTONES: DISTINGUISHING T1 AND T2 DEPENDENCE ON SURFACE RELAXATION, INTERNAL GRADIENTS AND DEPENDENCE ON ECHO SPACING
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PARAMAGNETIC RELAXATION IN SANDSTONES: DISTINGUISHING T1 AND T2 DEPENDENCE ON SURFACE RELAXATION, INTERNAL GRADIENTS AND DEPENDENCE ON ECHO SPACING

机译:沙岩中的顺磁弛豫:区分T1和T2与表面弛豫,内部梯度和回声间距的相关性

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Sandstones have T1/T2 ratio of 1.6, on the average. Clean silica has a T1/T2 ratio of about 1.3. If T2 changes with echo spacing in a homogeneous applied magnetic field, the change is interpreted to be due to diffusion in internal gradients. We demonstrate that when the paramagnetic materia material is iron, the increase in the l T1/T2 ratio above that of clean silica is due to diffusion in internal gradient. Furthermore, when the paramagnetic sites are small enough, no dependence on echo spacing is observed with conventional low low-field NMR spectromet spectrometers. Echo spacing dependence is observed ers. When the paramagnetic materials become large enough or form a ‘shell’ around each silica grain such that the length scale of the region of induced magnetic gradients is large compared to the diffusion length durin during the g time of the echo spacing. The basis for these assertions is a series of experiments and calculations described below. Silica sand coated with 0.12 nm Fe Fe3+ 3+ ion has a T1/T2 ratio close to that of clean sand sand. No echo spacing dependence of T2 relaxatio relaxation is observed. Larger ( n 25 nm and 110 nm nm) magnetite particles coated on silica sand have no echo spacing dependence for lower concentration of particles but show echo spacing dependence for larger concentrations. Largest (2, 2,400 nm) magnetite particles 00 mixe mixed with fine sand have echo spacing dependence d and T1/T2 greater than 2.These experimental observations are being interpreted by theoretical calculations. The magnetite particles are modeled as paramagnetic spheres. Paramagnetic particles on the surfa surface of silica grains ce are modeled as individual particles at low concentrations. At high surface concentrations, they are modeled as a thin, spherical shell of paramagnetic material. Calculations show that the system transitions from the motionally averagin averaging to g the localization regime at high surface concentration of paramagnetic particles.
机译:平均而言,砂岩的T1 / T2比为1.6。清洁二氧化硅的T1 / T2比约为1.3。如果在均匀施加的磁场中T2随回波间隔而变化,则该变化被认为是由于内部梯度的扩散所致。我们证明,当顺磁性材料是铁时,I T1 / T2比率高于干净二氧化硅的比率的增加是由于内部梯度的扩散所致。此外,当顺磁性位点足够小时,使用常规的低场NMR光谱仪无法观察到对回波间隔的依赖性。回声间距的依赖性被观察到。当顺磁性材料变得足够大或在每个二氧化硅晶粒周围形成一个“壳”时,与在回波间隔g时间内的扩散长度durin相比,感应磁梯度区域的长度尺度会更大。这些断言的基础是下面描述的一系列实验和计算。涂有0.12 nm Fe Fe3 + 3+离子的硅砂的T1 / T2比值接近清洁砂的比值。没有观察到T2弛豫弛豫的回波间距依赖性。硅砂上涂覆的较大的磁铁矿颗粒(n 25 nm和110 nm nm)对较低浓度的颗粒没有回声间距依赖性,但对于较大浓度的颗粒显示出回声间距依赖性。与细砂混合的最大(2,2,400 nm)磁铁矿颗粒00具有回波间距依赖性d和T1 / T2大于2。这些实验观察结果正在通过理论计算来解释。磁铁矿颗粒被建模为顺磁球。二氧化硅颗粒表面上的顺磁性颗粒被建模为低浓度的单个颗粒。在高表面浓度下,它们被建模为顺磁性材料的薄球形外壳。计算表明,在顺磁粒子的高表面浓度下,系统从平均运动过渡到局部定位。

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