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The Average Energy and Molar Specific Heat at Constant Volume of an Einstein Solid Measured by an Observer with Fluctuating Frame of Reference

机译:爱因斯坦固体在恒定体积下的平均能量和摩尔比热

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We report an observer effect in an Einstein solid, a quantum-mechanical system, induced by fluctuations of an observer's frame of reference; which has been studied so far under the assumption that the observer's frame of reference remains constant throughout the performance of a measurement, thus, what is actually measured throughout the performance of a measurement is an unresolved problem during which the observer's frame of reference is assumed to fluctuate. We investigate the average energy and molar specific heat at constant volume of an Einstein solid measured by an observer with fluctuating frame of reference. The Einstein solid consists of N identical non-interacting simple harmonic oscillators per mole, where N is the Avogadro's number at temperature T. The average energy and molar specific heat at constant volume of the Einstein solid are formulated for two types of fluctuations of the observer's frame of reference in order to consider pedagogical and experimental demonstrations. The average energy of the Einstein solid is formulated from the definition of canonical ensemble average and the molar specific heat at constant volume of it is calculated by differentiating the average energy with T. The molar specific heat at constant volume of the Einstein solid exhibits novel features at low temperatures according to the distribution of fluctuations of the observer's frame of reference: 0 and 3R at T = 0 K for square-wave and sawtooth-wave fluctuations, respectively, where R is the gas constant.
机译:我们报告了由观察者参考系的波动引起的爱因斯坦固体(一种量子力学系统)中的观察者效应;到目前为止,在假设观察者的参考框架在整个测量过程中保持恒定的前提下进行了研究,因此,在整个测量过程中实际测量的结果是一个未解决的问题,在该问题中,观察者的参考框架被认为是波动。我们研究了由观察者在波动参考框架下测得的爱因斯坦固体在恒定体积下的平均能量和摩尔比热。爱因斯坦固体由每摩尔N个相同的非相互作用的简单谐振子组成,其中N是温度T时的阿伏加德罗数。爱因斯坦固体在恒定体积下的平均能量和摩尔比热是针对观察者的两种类型的涨落制定的为了考虑教学和实验示范的参考框架。爱因斯坦固体的平均能量由典范集合平均的定义来确定,并且通过将平均能量与T相除来计算其恒定体积的摩尔比热。爱因斯坦固体的恒定体积的摩尔比热表现出新的特征在低温下,根据观察者参考系的涨落分布:对于方波和锯齿波涨落,T = 0 K时分别为0和3R,其中R为气体常数。

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