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相关概念视频

Thermodynamic Potentials01:26

Thermodynamic Potentials

799
Thermodynamic potentials are state functions that are extremely useful in analyzing a thermodynamic system. They have dimensions of energy. The four important thermodynamic potentials are internal energy, enthalpy, Helmholtz free energy, and Gibbs free energy. These thermodynamic potentials can be expressed using two of the following variables: pressure, volume, temperature, and entropy. These two variables are expressed as the rate of change of the thermodynamic potential with respect to other...
799
Calculating Standard Free Energy Changes02:49

Calculating Standard Free Energy Changes

21.0K
The free energy change for a reaction that occurs under the standard conditions of 1 bar pressure and at 298 K is called the standard free energy change. Since free energy is a state function, its value depends only on the conditions of the initial and final states of the system. A convenient and common approach to the calculation of free energy changes for physical and chemical reactions is by use of widely available compilations of standard state thermodynamic data. One method involves the...
21.0K
Van der Waals Equation01:10

Van der Waals Equation

4.0K
The ideal gas law is an approximation that works well at high temperatures and low pressures. The van der Waals equation of state (named after the Dutch physicist Johannes van der Waals, 1837−1923) improves it by considering two factors.
First, the attractive forces between molecules, which are stronger at higher densities and reduce the pressure, are considered by adding to the pressure a term equal to the square of the molar density multiplied by a positive coefficient a. Second, the volume...
4.0K
Free Energy Changes for Nonstandard States03:25

Free Energy Changes for Nonstandard States

11.2K
The free energy change for a process taking place with reactants and products present under nonstandard conditions (pressures other than 1 bar; concentrations other than 1 M) is related to the standard free energy change according to this equation:
 
where R is the gas constant (8.314 J/K·mol), T is the absolute temperature in kelvin, and Q is the reaction quotient. This equation may be used to predict the spontaneity of a process under any given set of conditions.
Reaction Quotient...
11.2K
The Born-Haber Cycle02:44

The Born-Haber Cycle

21.7K
Lattice Energy 
21.7K
Van der Waals Interactions01:24

Van der Waals Interactions

63.7K
Atoms and molecules interact with each other through intermolecular forces. These electrostatic forces arise from attractive or repulsive interactions between particles with permanent, partial, or temporary charges. The intermolecular forces between neutral atoms and molecules are ion–dipole, dipole–dipole, and dispersion forces, collectively known as van der Waals forces.
63.7K

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相关实验视频

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Author Spotlight: Advancing Cell Membrane Biophysics - Exploring Interactions and Challenges Through Experimental and Computational Approaches
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拉普拉斯级非相互作用的自由能量密度函数的框架.

Valentin V Karasiev1, Joshua Hinz1, R M N Goshadze1

  • 1Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299 United States.

The journal of physical chemistry letters
|August 6, 2024
PubMed
概括

一个新的无轨道元一般化梯度近似 (meta-GGA) 框架提高了热密度函数理论模拟的准确性. 这种先进的方法在较低温度下对温暖的密集物质特别有效.

科学领域:

  • 计算物理 计算物理
  • 量子化学 是一个量子化学.
  • 材料科学 材料科学 材料科学

背景情况:

  • 无轨密度函数理论 (DFT) 方法提供了计算效率,但往往缺乏准确性,特别是对于热性质.
  • 现有的近似方法,如托马斯-费米和通用梯度近似 (GGA),在描述复杂系统方面存在局限性.
  • 开发精确的无轨函数对于在极端条件下模拟系统至关重要,例如热密集物质.

研究的目的:

  • 为无轨道的元一般化梯度近似 (meta-GGA) 函数开发一个新的框架.
  • 构建一个非实证的元GGA函数,适用于非相互作用的自由能量密度函数.
  • 为了提高无轨道DFT模拟热性质的准确性.

主要方法:

  • 基于非相互作用的自由能量第四阶梯度膨胀的理论框架的开发.
  • 构建一个非实证的元-GGA函数,将其缩小到已知的极限.
  • 使用热密的模拟来应用和验证新的功能.

主要成果:

  • 成功开发了一个新的无轨元GGA框架和相应的非实证函数.
  • 开发的函数准确地复制了缓慢变化的密度极限中的第四阶梯度扩张.
  • 与托马斯-费米和GGA方法相比,温密的模拟显示了40 eV以下的精度大幅增加.

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结论:

  • 开发的无轨道元GGA框架为热DFT计算提供了重大进步.
  • 这种新的功能提供了更准确的描述,在较低的温度下温暖的密集物质.
  • 这项研究为未来计算物理和材料科学研究提供了有价值的工具.