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相关概念视频

Shock Waves01:16

Shock Waves

While deriving the Doppler formula for the observed frequency of a sound wave, it is assumed that the speed of sound in the medium is greater than the source's speed through it. When this condition is breached, a shock wave occurs.
When the source's speed approaches the speed of sound, constructive interference between successive wavefronts emitted by the source occurs immediately behind it. Initially, scientists believed that this constructive interference would result in such high pressures...
Distribution of Molecular Speeds01:27

Distribution of Molecular Speeds

The motion of molecules in a gas is random in magnitude and direction for individual molecules, but a gas of many molecules has a predictable distribution of molecular speeds. This predictable distribution of molecular speeds is known as the Maxwell-Boltzmann distribution. The distribution of molecular speeds in liquids is comparable to that of gases but not identical and can help to understand the phenomenon of the boiling and vapor pressure of a liquid. Consider that a molecule requires a...
Velocity and Acceleration of a Wave00:51

Velocity and Acceleration of a Wave

A wave propagates through a medium with a constant speed, known as a wave velocity. It is different from the speed of the particles of the medium, which is not constant. In addition, the velocity of the medium is perpendicular to the velocity of the wave. The variable speed of the particles of the medium implies that there must be acceleration associated with it. 
The velocity of the particles can be obtained by taking the partial derivative of the position equation with respect to time. We can...
Molecular Kinetic Energy01:21

Molecular Kinetic Energy

The word "gas" comes from the Flemish word meaning "chaos," first used to describe vapors by the chemist J. B. van Helmont. Consider a container filled with gas, with a continuous and random motion of molecules. During collisions, the velocity component parallel to the wall is unchanged, and the component perpendicular to the wall reverses direction but does not change in magnitude. If the molecule’s velocity changes in the x-direction, then its momentum is changed. During the short time of the...
Maxwell-Boltzmann Distribution: Problem Solving01:20

Maxwell-Boltzmann Distribution: Problem Solving

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
Equations of Wave Motion01:02

Equations of Wave Motion

Mathematically, the motion of a wave can be studied using a wavefunction. Consider a string oscillating up and down in simple harmonic motion, having a period T. The wave on the string is sinusoidal and is translated in the positive x-direction as time progresses. Sine is a function of the angle θ, oscillating between +A and −A and repeating every 2π radians. To construct a wave model, the ratio of the angle θ and the position x is considered.

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相关实验视频

Updated: Jul 11, 2026

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
11:03

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

Published on: December 4, 2017

在高超音速冲击波中的无平衡分子运动.

G Pham-Van-Diep, D Erwin, E P Muntz

    Science (New York, N.Y.)
    |August 11, 1989
    PubMed
    概括

    在高超音速冲击波中测量了分子速度分布,揭示了双模性特征. 这一观察证实了莫特-史密斯的说法.

    科学领域:

    • 流体动力学 流体动力学
    • 空气动力学 航空动力学
    • 物理化学 物理化学

    背景情况:

    • 超音速流动涉及通过冲击波快速改变气体特性.
    • 莫特-史密斯假设在冲击波中存在双模分子速度分布.
    • 缺乏对这种双模分布的直接观察.

    研究的目的:

    • 在超音速冲击波中实验测量分子速度.
    • 为了验证假设的双模态分子速度分布.
    • 为了验证非平衡流分析的计算方法.

    主要方法:

    • 对分子速度的实验测量.
    • 对分子速度分布函数的分析.
    • 直接模拟蒙特卡罗 (DSMC) 技术用于计算建模.

    主要成果:

    • 质量双模分子速度分布的直接观测.
    • 观察到的分布与冲击的两侧分布一致.
    • DSMC精确计算了分子速度分布函数.

    结论:

    • 超音速冲击波中的分子速度分布确实是双模的.

    更多相关视频

    Conducting Elevated Temperature Normal and Combined Pressure-Shear Plate Impact Experiments Via a Breech-end Sabot Heater System
    10:52

    Conducting Elevated Temperature Normal and Combined Pressure-Shear Plate Impact Experiments Via a Breech-end Sabot Heater System

    Published on: August 7, 2018

    Blast Quantification Using Hopkinson Pressure Bars
    09:41

    Blast Quantification Using Hopkinson Pressure Bars

    Published on: July 5, 2016

    相关实验视频

    Last Updated: Jul 11, 2026

    An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
    11:03

    An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

    Published on: December 4, 2017

    Conducting Elevated Temperature Normal and Combined Pressure-Shear Plate Impact Experiments Via a Breech-end Sabot Heater System
    10:52

    Conducting Elevated Temperature Normal and Combined Pressure-Shear Plate Impact Experiments Via a Breech-end Sabot Heater System

    Published on: August 7, 2018

    Blast Quantification Using Hopkinson Pressure Bars
    09:41

    Blast Quantification Using Hopkinson Pressure Bars

    Published on: July 5, 2016

  • 实验数据支持莫特-史密斯的假设.
  • DSMC是模拟高度不平衡流量的可靠方法.