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The theoretical study of dielectric properties of water using the modified Onsager-Kirkwood-Fr?hlich theory

机译:用改进的onsager-kirkwood-fr的水介电性质的理论研究 - kirkwood-fr?Hlich理论

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In the work, we present the new method for calculation dielectric properties for Water in the wide temperature range. We use the modified Onsager-Kirkwood-Fr?hlich theory, which makes it possible to calculate the polarization characteristics without using the static permittivity. We assumed that the dielectric is an isotropic medium consisting of molecules that do not interact with each other and are located in molecular electric fields. It allows us to use the average cosine of the angle between local electric field vectors and the dipole moment vectors of molecules in a medium as the average measure of the local orientation of the dipoles. This approach also makes it possible to equate the value of the energy of the interaction of dipoles with molecular fields to the value of the internal interaction energy if the energy of the interaction of the dipoles with external fields used for the experimental determination of the value of static permittivity is much less than the energy of the interaction. The calculated values of the dipole moment agree with the modern quantum mechanical calculations, and the results of calculating the values of permittivity are in practical agreement with experiment in the wide range of123.15K-573.15K. The method allows to calculate the static permittivity of water in various aggregate states: ice Ih in the range from 123K to melting point, supercooled water in the range from 238K to melting point, water at the saturation line from the melting point to the precritical region.
机译:在工作中,我们介绍了宽温度范围内水的计算介电性能的新方法。我们使用修改的onsager-kirkwood-fr?Hlich理论,这使得可以在不使用静态介电常数的情况下计算偏振特性。我们假设电介质是由不彼此相互作并且位于分子电场中的分子组成的各向同性培养基。它允许我们使用局部电场向量和介质中分子的偶极力矩向量之间的平均余弦作为偶极子局部取向的平均测量。这种方法还使得可以将偶极子与分子场的相互作用的能量等同于内部相互作用能量的值,如果偶极子与外部字段的相互作用的能量用于实验确定值的值静态介电常数远小于相互作用的能量。偶极力矩的计算值与现代量子力学计算同意,计算介电常数的值的结果是实际协议,实验在于123.15K-573.15K的范围内。该方法允许计算各种骨料状态中水的静电介电常数:冰Ih在123k至熔点的范围内,从238k到熔点的过冷水,饱和点的水从熔点到预临界区域。 。

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