首页> 外文期刊>The Journal of Chemical Physics >The effect of the spatial nonlocality of the Kirkwood g-factor on the determination of the long wavelength dielectric functions in dipolar fluids
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The effect of the spatial nonlocality of the Kirkwood g-factor on the determination of the long wavelength dielectric functions in dipolar fluids

机译:柯克伍德g因子的空间非局部性对偶极流体中长波长介电函数的确定的影响

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摘要

The Kirkwood g-factor that determines the long wavelength dielectric constant of a simple, isotropic, translationally invariant dipolar fluid is given by an integral of a dipole-dipole correlation function over a spherical region of a nonzero radius RK chosen such that any further increase in the radius leads to no change in the value of the integral, thereby defining a Kirkwood correlation length RK. For radii less than the correlation length the integral defines a radius dependent (nonlocal) Kirkwood g-factor, implying a nonlocal dielectric function. The nonlocal nature of these quantities has important consequences for the determination of the long wavelength dielectric function from dipole fluctuations via the Kirkwood-Frhlich connection. The dipole-dipole correlation function (the volume dipole auto-correlation function) commonly used in this determination involves particles residing solely within a sphere of radius R, unlike the correct correlation function which involves either a single particle with those particles in a spherical volume of radius RK or those particles in a spherical volume of radius R with those residing within a spherical volume of radius R+RK. A procedure is suggested for extracting the infinite system dipole-dipole correlation function from results of simulations performed on finite spherical samples. Using some results reported in the recent literature, relative to the accurate correlation function the commonly used correlation function ranges from 27 too small for a sphere having a radius comparable to the Kirkwood correlation length to 4 too small at a radius of seven times that correlation length. As a result, the apparent dielectric constants, as determined by the conventional procedure of using the fluctuations of the sum of dipoles in a finite fixed volume, are also too small. This suggests that a dielectric constant extracted from computer simulations using a total dipole-total dipole correlation function in a given volume with other geometries and/or boundary conditions will result in similar errors.
机译:确定简单,各向同性,平移不变的偶极流体的长波长介电常数的柯克伍德g因子由在非零半径RK的球形区域上的偶极子-偶极子相关函数的积分给出,以使任何进一步增加的半径导致积分值不变,从而定义了柯克伍德相关长度RK。对于半径小于相关长度的积分,积分定义了一个与半径相关的(非局部)柯克伍德g因子,这意味着存在非局部介电函数。这些量的非局部性质对于通过柯克伍德-弗里希连接(Kirkwood-Frhlich connection)通过偶极子波动确定长波长介电函数具有重要意义。该确定中通常使用的偶极子-偶极子相关函数(体积偶极子自相关函数)涉及仅存在于半径为R的球体中的粒子,而正确的相关函数不涉及单个粒子和那些球形粒子的球体体积。半径RK或位于半径为R的球体中的那些粒子以及位于半径为R + RK的球体中的那些粒子。建议从有限球形样本的仿真结果中提取无限系统偶极-偶极相关函数的过程。使用最新文献中报道的一些结果,相对于精确的相关函数,常用的相关函数的范围从半径小于柯克伍德相关长度的球体的27太小到半径为相关长度的七倍的球体的太小4 。结果,通过使用有限的固定体积中的偶极子之和的波动的常规程序所确定的表观介电常数也太小。这表明,在给定体积中使用其他偶极子和总偶极子相关函数从计算机模拟中提取的介电常数将具有类似的误差。

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