牛顿冷却定律的新解释:热子的两个特征:弹性体积和角动量

J. Stávek
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引用次数: 0

摘要

牛顿冷却定律为了描述热粒子(热子)的隐藏特征和将热量辐射到温度较低的环境中的机制,至今仍吸引着学者们的关注。定义了该过程的特征冷却常数1/τπ [min-1]作为描述热弹性体积和热角动量贡献的实验参数。该实验参数τπ表示研究对象在起始温度为T0,周围温度为Tenv时达到温度Tπ = Tenv +(T0-Tenv)/π所需的时间。所研究的系统是装在体积为2000、1000、500、250和100 mL的球形烧瓶中的水,起始温度为90°C、80°C和70°C,周围温度为24°C(实验室温度)和(4°±2°)C(2023年3月5日布拉格附近的室外温度)。有一个关键的实验参数:把温度计放在球烧瓶的什么地方。向内到底墙,2。在球形烧瓶的中心,3。在水量的上层,4。从外面到底墙。在所有的实验运行中,我们发现在球形烧瓶内底壁测量的温度Tπ可以解释为“真正的”牛顿温度,而特征冷却常数τπ非常接近这些冷却系统的半对数图上的斜率值。该模型用于解释牛顿(1701)的历史实验数据和格里古尔(1984)的现代实验数据。该模型开辟了卡诺热机的新观点,热子的弹性体积可以达到效率η1 = (THOT - Tπ)/(THOT - TCOLD) = 1-1/π≈0.682。此外,卡诺热机后的“余热”可用于塞贝克发生器,将热子的角动量转化为电能(热电发生器),效率η为2 = (Tπ - TCOLD)/(THOT - TCOLD) = 1/π≈0.318。卡诺(1824年)-塞贝克(1825年)联合热机可以探测热门的所有可用热量,以获得THOT - TCOLD的温差。
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A New Interpretation of the Newton´s Cooling Law: Two Features of Thermons: Their Elastic Volume and Their Angular Momentum
The Newton´s cooling law still attracts the attention of scholars in order to describe hidden features of heat particles (thermons) and the mechanism of the radiating heat into the surroundings with a lower temperature. The characteristic cooling constant of this process 1/τπ [min-1] was defined as the experimental parameter describing the contributions of the thermon elastic volume and thermon angular momentum. This experimental parameter τπwas found as the time needed to achieve the temperature Tπ = Tenv +(T0-Tenv)/π during the cooling of the studied object with the starting temperature T0 and the surrounding with temperature Tenv. The studied system was water in spherical flasks with the volumes 2000, 1000, 500, 250, and 100 mL and the starting temperatures 90° C, 80°C, and 70° C. The temperature of the surrounding was 24° C (laboratory temperature) and (4° ± 2°) C (outdoor temperature on March 5 2023 near Prague). There was one critical experimental parameter: where to place the thermometer in the spherical flask: 1. inside to the bottom wall, 2. in the center of spherical flask, 3. at the upper level of the water volume, 4. outside to the bottom wall. For all experimental runs we have found that the temperature Tπ measured at the inside bottom wall of the spherical flasks might be interpreted as the “true” Newtonian temperature while the characteristic cooling constant τπ is very close to the value of the slope in the semi-log graph of those cooling systems. This model was used to interpret the historical experimental data of Newton (1701) and the modern experimental data of Grigull (1984). This model opens a new view on the Carnot engine where the elastic volume of thermons can achieve the efficiency η1 = (THOT – Tπ)/(THOT – TCOLD) = 1-1/π ≈ 0.682. Moreover, the “waste heat” after the Carnot engine can be used in the Seebeck generator to convert the angular momentum of thermons into the electricity (thermoelectric generator) with the efficiency η2 = (Tπ –TCOLD)/(THOT – TCOLD) = 1/π ≈ 0.318. The combined Carnot (1824) – Seebeck (1825) engine can explore all available heat of the of thermons for the temperature difference THOT – TCOLD.
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