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相关概念视频

Behavior of Gas Molecules: Molecular Diffusion, Mean Free Path, and Effusion03:48

Behavior of Gas Molecules: Molecular Diffusion, Mean Free Path, and Effusion

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Although gaseous molecules travel at tremendous speeds (hundreds of meters per second), they collide with other gaseous molecules and travel in many different directions before reaching the desired target. At room temperature, a gaseous molecule will experience billions of collisions per second. The mean free path is the average distance a molecule travels between collisions. The mean free path increases with decreasing pressure; in general, the mean free path for a gaseous molecule will be...
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Diffusion01:21

Diffusion

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Diffusion is a type of passive transport. In passive transport, a substance tends to move from an area of high concentration to an area of low concentration until the concentration is equal across the space. For example, take the diffusion of substances through the air. When someone opens a perfume bottle in a room filled with people, the perfume is at its highest concentration in the bottle and is at its lowest at the edges of the room. The perfume vapor will diffuse, or spread away, from the...
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Mean free path and Mean free time01:22

Mean free path and Mean free time

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Consider the gas molecules in a cylinder. They move in a random motion as they collide with each other and change speed and direction. The average of all the path lengths between collisions is known as the "mean free path."
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Passive Diffusion: Overview and Kinetics01:17

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Passive diffusion is a critical process that allows small lipophilic drugs to cross the cell membrane along a concentration gradient. This mechanism's efficiency depends on four primary factors: the membrane's surface area, the drug's lipid-water partition coefficient, the concentration gradient, and the membrane's thickness.
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Maxwell-Boltzmann Distribution: Problem Solving01:20

Maxwell-Boltzmann Distribution: Problem Solving

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Individual molecules in a gas move in random directions, but a gas containing numerous molecules has a predictable distribution of molecular speeds, which is known as the Maxwell-Boltzmann distribution, f(v).
This distribution function f(v) is defined by saying that the expected number N (v1,v2) of particles with speeds between v1 and v2 is given by
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Van der Waals Interactions01:24

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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.
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相关实验视频

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In Situ Monitoring of Diffusion of Guest Molecules in Porous Media Using Electron Paramagnetic Resonance Imaging
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在自由分子模式下,气溶颗粒的扩散性.

Katerina S Karadima1,2,3, Dimitris G Tsalikis3, Vlasis G Mavrantzas1,2,3

  • 1Department of Chemical Engineering, University of Patras, Patras GR-26504, Greece.

The journal of physical chemistry. A
|June 3, 2025
PubMed
概括

分子动力学模拟显示了在关键交叉模式中的纳米粒子扩散性. 3纳米以下的微小纳米粒子偏离了经典模型,凸显了原子相互作用的重要性.

科学领域:

  • 气溶科学是一门气溶科学.
  • 纳米技术纳米技术
  • 计算物理学的计算物理.

背景情况:

  • 气溶纳米颗粒 (NPs) 在交叉模式 (分子到<5 nm NPs) 的扩散性对于纳米技术和气溶过程,如核和运输至关重要.
  • 以前使用低压的大颗粒的实验没有捕捉到在纳米尺度上占主导地位的原子级相互作用.
  • 了解NP扩散性是准确模拟自由分子状态下的气溶行为的关键.

研究的目的:

  • 用分子动力学 (MD) 模拟来确定空气中微小的富勒和纳米粒子 (0.47 nm) 的扩散系数.
  • 在关键纳米尺度交叉系统中研究现有扩散性方程 (Epstein,SCM) 的有效性.
  • 为了将模拟结果与实验数据和其他文献模型对NP扩散性进行比较.

主要方法:

  • 采用了原子分子动力学 (MD) 模拟,考虑了NP和气体分子及其全部力场和形状.
  • 对于直径从0.4nm到大约7nm的NP计算了扩散系数.
  • 系统地与已建立的理论模型和实验发现进行了MD衍生的扩散性比较.

主要成果:

  • 在3nm以下,MD衍生的扩散率与实验性气体扩散率方程非常相匹配,但与爱斯坦和SCM方程有显著的偏差.
  • 这些偏差是最明显的,因为NP大小接近气体分子大小,强调原子相互作用效应.

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Last Updated: Jun 13, 2025

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  • 在5nm以上,MD衍生的扩散度与经典爱斯坦和SCM方程的预测趋同.
  • 结论:

    • 经典的扩散性方程 (Epstein,SCM) 对于3nm以下的NP是不够的,因为原子级相互作用占主导地位.
    • 分子动力学模拟在关键的纳米尺度交叉模式中提供准确的NP扩散率数据.
    • 这些发现需要修订NP运输和在分子到纳米级接口上的行为模型.