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Force and Potential Energy in Three Dimensions01:04

Force and Potential Energy in Three Dimensions

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Consider a particle moving under the action of a conservative force that has components along each coordinate axis. Each component of force is a function of the coordinates. The potential energy function U is also a function of all three spatial coordinates. Force in one dimension can be written as the negative ratio of potential energy change to the displacement along that coordinate. For minimal displacement, the ratios become derivatives. If a function has many variables, the derivative only...
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Van der Waals Interactions01:24

Van der Waals Interactions

70.3K
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.
70.3K
Potential Due to a Magnetized Object01:24

Potential Due to a Magnetized Object

766
Magnetic dipoles in magnetic materials are aligned when placed under an external magnetic field. For paramagnets and ferromagnets, dipole alignment occurs in the direction of the magnetic field. However, the dipoles align opposite to the field in the case of diamagnets. This state of magnetic polarization due to the external field is called magnetization. Magnetization is defined as the dipole moment per unit volume. It plays a similar role to polarization in electrostatics.
The vector...
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Differential Form of Maxwell's Equations01:17

Differential Form of Maxwell's Equations

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James Clerk Maxwell (1831–1879) was one of the significant contributors to physics in the nineteenth century. He is probably best known for having combined existing knowledge of the laws of electricity and the laws of magnetism with his insights to form a complete overarching electromagnetic theory, represented by Maxwell's equations. The four basic laws of electricity and magnetism were discovered experimentally through the work of physicists such as Oersted, Coulomb, Gauss, and...
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Magnetic Vector Potential01:15

Magnetic Vector Potential

1.5K
In electrostatics, the electric field can be written as the negative gradient of the potential. In magnetostatics, the zero divergence of the magnetic field ensures that the magnetic field can be expressed as the curl of a vector potential. This potential is known as the magnetic vector potential.
Consider an ideal solenoid with n turns per unit length and radius R. If I is the current through the solenoid, the magnetic field inside the solenoid is expressed as the product of vacuum...
1.5K
Symmetry in Maxwell's Equations01:28

Symmetry in Maxwell's Equations

4.1K
Once the fields have been calculated using Maxwell's four equations, the Lorentz force equation gives the force that the fields exert on a charged particle moving with a certain velocity. The Lorentz force equation combines the force of the electric field and of the magnetic field on the moving charge. Maxwell's equations and the Lorentz force law together encompass all the laws of electricity and magnetism. The symmetry that Maxwell introduced into his mathematical framework may not be...
4.1K

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相关实验视频

Updated: Jan 16, 2026

Excitonic Hamiltonians for Calculating Optical Absorption Spectra and Optoelectronic Properties of Molecular Aggregates and Solids
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Excitonic Hamiltonians for Calculating Optical Absorption Spectra and Optoelectronic Properties of Molecular Aggregates and Solids

Published on: May 27, 2020

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时刻张量潜力和等价张量网络潜力,具有明确的分散相互作用.

Olga Chalykh1, Dmitry Korogod1,2, Ivan S Novikov1,2,3,4

  • 1Skolkovo Institute of Science and Technology, Skolkovo Innovation Center, Bolshoy Boulevard 30, Moscow 143026, Russian Federation.

The Journal of chemical physics
|October 2, 2025
PubMed
概括

显式分散相互作用 (D2 / D3 校正) 显著增强机器学习液体建模的原子间潜力 (MLIP). D2校正提供了与D3相似的准确性,而计算成本较低.

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Generation and Coherent Control of Pulsed Quantum Frequency Combs
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Vibrational Spectra of a N719-Chromophore/Titania Interface from Empirical-Potential Molecular-Dynamics Simulation, Solvated by a Room Temperature Ionic Liquid
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相关实验视频

Last Updated: Jan 16, 2026

Excitonic Hamiltonians for Calculating Optical Absorption Spectra and Optoelectronic Properties of Molecular Aggregates and Solids
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Excitonic Hamiltonians for Calculating Optical Absorption Spectra and Optoelectronic Properties of Molecular Aggregates and Solids

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Generation and Coherent Control of Pulsed Quantum Frequency Combs
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Generation and Coherent Control of Pulsed Quantum Frequency Combs

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科学领域:

  • 计算化学的计算化学
  • 材料科学 材料科学 材料科学
  • 机器学习 机器学习

背景情况:

  • 机器学习原子间潜力 (MLIP) 对于模拟分子系统至关重要.
  • 准确的建模需要捕捉各种原子间力,包括分散相互作用.

研究的目的:

  • 评估显式分散校正 (D2,D3) 对MLIP精度的影响.
  • 评估液态四化碳,甲和的MLIP性能.
  • 为了比较D2和D3校正和不同切断半径的有效性.

主要方法:

  • 将D2和D3分散校正纳入动量张量潜力和等价张量网络潜力.
  • 基准测量MLIP准确度与初始二元结合曲线的比较.
  • 使用实验密度和辐射分布函数进行验证.

主要成果:

  • 显式分散校正显著提高了MLIP的准确性,特别是在标准切断半径 (5-6 Å) 上.
  • 将切断半径延长到7.5 Å进一步提高了四化碳和甲的准确性.
  • D2 校正提供了与 D3 校正相当的准确性,但计算成本降低.
  • 准确的托鲁建模需要明确的分散合并.

结论:

  • 明确的分散相互作用对于精确的分子液体MLIP至关重要.
  • D2校正为D3提供了一个计算效率高的替代方案,以实现高精度.
  • 带有分散校正的MLIP显示出与理论和实验数据的良好一致.