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相关概念视频

Propagation of Waves01:07

Propagation of Waves

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When a wave propagates from one medium to another, part of it may get reflected in the first medium, and part of it may get transmitted to the second medium. In such a case, the interface of the two mediums can be considered as a boundary that is neither fixed nor free.
Consider a scenario where a wave propagates from a string of low linear mass density to a string of high linear mass density. In such a case, the reflected wave is out of phase with respect to the incident wave, however the...
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Reflection of Waves01:07

Reflection of Waves

3.7K
When a wave travels from one medium to another, it gets reflected at the boundary of the second medium. A common example of this is when a person yells at a distance from a cliff and hears the echo of their voice. The sound waves (longitudinal waves) traveling in the air are reflected from the bounding cliff. Similarly, flipping one end of a string whose other end is tied to a wall causes a pulse (transverse wave) to travel through the string, which gets reflected upon reaching the wall. In...
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Boundary Conditions: Lossless Lines01:21

Boundary Conditions: Lossless Lines

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Consider a single-phase, two-wire, lossless transmission line terminated by an impedance at the receiving end and a source with Thevenin voltage and impedance at the sending end. The line, with length, has a surge impedance and wave velocity determined by the line's inductance and capacitance.
At the receiving end, the boundary condition states that the voltage equals the product of the receiving-end impedance and current. This relationship is expressed as a function of the incident and...
94
Transmission-Line Differential Equations01:26

Transmission-Line Differential Equations

299
Transmission lines are essential components of electrical power systems. They are characterized by the distributed nature of resistance (R), inductance (L), and capacitance (C) per unit length. To analyze these lines, differential equations are employed to model the variations in voltage and current along the line.
Line Section Model
A circuit representing a line section of length Δx helps in understanding the transmission line parameters. The voltage V(x) and current i(x) are measured...
299
Interference: Path Lengths01:10

Interference: Path Lengths

1.3K
Consider two sources of sound, that may or may not be in phase, emitting waves at a single frequency, and consider the frequencies to be the same.
Two special sources may be considered when they are in phase. This can be easily achieved by feeding the two sources from the same source. An example would be synchronizing the two speakers by feeding them with the same source, such as the sound waves produced by a tuning fork. This setup ensures that the two sources have the same frequency and are...
1.3K
Fault Types01:18

Fault Types

89
When analyzing a single line-to-ground fault from phase A to ground at a three-phase bus, it is important to consider the fault impedance. This impedance is zero for a bolted fault, equal to the arc impedance for an arcing fault, and represents the total fault impedance for a transmission-line insulator flashover. To derive sequence and phase currents, fault conditions are translated from the phase domain to the sequence domain.
For line-to-line faults occurring between phases B and C, the...
89

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Detection of Architectural Distortion in Prior Mammograms via Analysis of Oriented Patterns
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    此摘要是机器生成的。

    白光干扰仪实验区分几何和传播阶段. 该研究解决了几何相界限问题,表明其解决方案取决于相规则的选择.

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    科学领域:

    • 光学和光子学 在光学和光子学.
    • 量子力学就是量子力学.

    背景情况:

    • 几何相位,量子力学和光学中的一个基本概念,描述了独立于系统演变的大小的相位移动.
    • "局限性问题"问的是几何相是否局限于特定范围 (例如, -π 到 +π) 或是否可以不受限制.

    研究的目的:

    • 通过白光干涉测量来实验地区分几何和传播相.
    • 研究几何相的"边界性问题"及其对相规范的依赖.
    • 为理解几何阶段提供教学资源.

    主要方法:

    • 使用白光干扰仪实验.
    • 分析实验结果以确定几何和传播阶段之间的差异.
    • 理论和实验检查阶段规范及其对几何阶段的影响.

    主要成果:

    • 清楚的实验证明了几何和传播阶段之间的区别.
    • 证据表明一种方法来解决几何相局限性问题.
    • 突出阶段常规在确定几何阶段的边界性方面的关键作用.

    结论:

    • 实验发现澄清了几何和传播阶段的性质.
    • 几何相界限问题的解决方法被证明是依赖于常规的.
    • 提供的实验视频可以作为几何相概念的宝贵教育工具.