热的机械等效解释为热体的角动量

J. Stávek
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引用次数: 1

摘要

在过去的三百年里,产生了许多形式的热学理论。在它的起源上,热力学是研究热和发动机的,因此,我们应该与这些根源联系起来。在这个模型中,我们把热子看作热从热物体到冷物体的载体。热流被模拟为这些热子的角动量在从高角动量到低角动量方向上的传递。热J的机械当量被定义为热子角动量与周围温度之比。这个模型将热熵S定义为热子角动量与周围温度之比。这个模型可以为微观世界打开一个新的窗口,量子粒子在一个方向上传递它们的热量。然而,这个方向可以通过对这些量子粒子所做的功来改变,并使这些量子粒子的角动量从低角动量流向高角动量。我们将会发现,这些为所有学者所熟知的S公式可能仍然隐藏着一些令人惊讶的性质。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
The Mechanical Equivalent of Heat Interpreted as the Angular Momentum of Thermons
There were derived many forms of theories of heat during the past three hundred years. At its origins, thermodynamics was the study of heat and engines and therefore, we should be connected to these roots. In this model we present thermons as carriers of heat from hot bodies to cold bodies. The flow of heat is modelled as the transfer of angular momentum of these thermons in the direction from the higher angular momentum to the lower angular momentum of thermons. The mechanical equivalent of heat J is defined as the ratio of the angular momentum of thermons to the temperature of the surrounding. This model newly defines the quantity of heat – entropy S – as the ratio of the angular momentum of thermons to the temperature of the surrounding. This model can open a new window to the microworld where quantum particles transfer their heat content in one direction. However, this direction can be changed via the work done on these quantum particles and to reverse the flow of the angular momentum from lower angular momentum to higher angular momentum of those quantum particles. It will be shown that these very well-known formulae of S to all scholars might still keep some hidden surprising properties.
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