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相关概念视频

Heat Capacities of an Ideal Gas III01:25

Heat Capacities of an Ideal Gas III

2.2K
The number of independent ways a gas molecule can move along straight line, rotate, and vibrate is called its degrees of freedom. Supposing d represents the number of degrees of freedom of an ideal gas, the molar heat capacity at constant volume of an ideal gas in terms of d is
2.2K
Nuclear Binding Energy02:13

Nuclear Binding Energy

12.5K
The difference between the calculated and experimentally measured masses is known as the mass defect of the atom. In the case of helium-4, the mass defect indicates a “loss” in mass of 4.0331 amu – 4.0026 amu = 0.0305 amu. The loss in mass accompanying the formation of an atom from protons, neutrons, and electrons is due to the conversion of that mass into energy that is evolved as the atom forms. The nuclear binding energy is the energy produced when the atoms’ nucleons...
12.5K
Heat Capacities of an Ideal Gas II01:23

Heat Capacities of an Ideal Gas II

2.4K
For a system that undergoes a thermodynamic process at a constant volume condition, the heat absorbed is used only to increase the system's internal energy and not for doing any kind of work. While for a system undergoing a thermodynamic process under a constant pressure condition, the amount of heat absorbed is used not only for increasing the internal energy (as a function of temperature) but also for doing some work. The molar heat capacity is the amount of heat required to increase the...
2.4K
Heat Capacities of an Ideal Gas I01:14

Heat Capacities of an Ideal Gas I

2.7K
Heat capacity is the ratio of heat absorbed by the substance corresponding to its temperature change. It is also called thermal capacity and the SI unit of heat capacity is J/K. Whereas, specific heat capacity is defined as the amount of heat necessary to change the temperature of 1 kg of a substance by 1 K and is also called massic heat capacity. Its SI unit is J/kg⋅K.
Molar heat capacity quantifies the ratio of the amount of heat added (or removed) to increase (or decrease) the...
2.7K
Molecular Comparison of Gases, Liquids, and Solids02:26

Molecular Comparison of Gases, Liquids, and Solids

41.4K
Particles in a solid are tightly packed together (fixed shape) and often arranged in a regular pattern; in a liquid, they are close together with no regular arrangement (no fixed shape); in a gas, they are far apart with no regular arrangement (no fixed shape). Particles in a solid vibrate about fixed positions (cannot flow) and do not generally move in relation to one another; in a liquid, they move past each other (can flow) but remain in essentially constant contact; in a gas, they move...
41.4K

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相关实验视频

Updated: Jul 18, 2025

Simulation of the Planetary Interior Differentiation Processes in the Laboratory
06:04

Simulation of the Planetary Interior Differentiation Processes in the Laboratory

Published on: November 15, 2013

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固态阶段的He: 一个蒙特卡洛模拟研究.

Massimo Boninsegni1

  • 1Department of Physics, University of Alberta, Edmonton, AB T6G 2H5, Canada.

Entropy (Basel, Switzerland)
|August 26, 2023
PubMed
概括

在低温下模拟固体-4 (4He) 晶体的热力学. 关键性质在1克尔文以下保持稳定,量子统计微妙地影响动量分布.

科学领域:

  • 凝聚物质物理学 凝聚物质物理学
  • 量子力学就是量子力学.
  • 热力学是一种热力学.

背景情况:

  • 固体-4 (4He) 呈现出独特的量子行为.
  • 之前的理论研究探讨了它的热力学特性.

研究的目的:

  • 在理论上研究固体 (hcp) 4He的热力学.
  • 用更低的温度和更大的系统尺寸来扩展以前的工作.
  • 为了充分纳入量子统计,并比较不同的对潜力.

主要方法:

  • 在有限温度下进行无偏的蒙特卡洛模拟.
  • 在广泛的密度范围内进行的模拟.
  • 包括量子统计和对对潜力的比较.

主要成果:

  • 热力学特性,包括动能,在1K以下大大独立于温度.
  • 量子力学交换是可以忽略不计的,即使在60mK.
  • 量子统计学效应可以在动量分布中观察到.

结论:

  • 固体4He的热力学在低温下是稳定的.
关键词:
气是气的重要组成部分.量子蒙特卡罗是一个量子的蒙特卡罗.量子固体是一种量子固体.

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Quantification of Hydrogen Concentrations in Surface and Interface Layers and Bulk Materials through Depth Profiling with Nuclear Reaction Analysis
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Fabrication of Uniform Nanoscale Cavities via Silicon Direct Wafer Bonding
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  • 量子统计学扮演了一个微妙但可检测的角色.
  • 模拟结果与实验数据一致.