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相关概念视频

Torsional Pendulum01:09

Torsional Pendulum

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A torsional pendulum involves the oscillation of a rigid body in which the restoring force is provided by the torsion in the string from which the rigid body is suspended. Ideally, the string should be massless; practically, its mass is much smaller than the rigid body's mass and is neglected.
As long as the rigid body's angular displacement is small, its oscillation can be modeled as a linear angular oscillation. The amplitude of the oscillation is an angle. The role of mass is played...
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Physical Pendulum01:06

Physical Pendulum

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When a rigid body is hanging freely from a fixed pivot point and is displaced, it oscillates similar to a simple pendulum and is known as a physical pendulum. The period and angular frequency of a physical pendulum are obtained by using the small-angle approximation and drawing parallels with a spring-mass system. The small-angle approximation (sinθ=θ) is valid up to about 14°.
When dealing with complicated systems, the mass moment of inertia is an important parameter, as it...
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Simple Pendulum01:10

Simple Pendulum

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A simple pendulum consists of a small diameter ball suspended from a string, which has negligible mass but is strong enough to not stretch. In our daily life, pendulums have many uses, such as in clocks, on a swing set, and on a sinker on a fishing line. 
The period of a simple pendulum depends on two factors: its length and the acceleration due to gravity. The period is completely independent of any other factors, such as mass or maximum displacement. For small displacements, a pendulum...
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Non-uniform Circular Motion01:22

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In uniform circular motion, the particle executing circular motion has a constant speed, and the circle is at a fixed radius. However, not all circular motion occurs at a constant speed. A particle can travel in a circle and speed up or slow down, showing an acceleration in the direction of motion. In that case, the motion is called non-uniform circular motion, and an additional acceleration is introduced, which is in the direction tangential to the circle. 
For example, such...
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Dynamics of Circular Motion01:30

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An object undergoing circular motion, like a race car, is accelerating because it is changing the direction of its velocity. This centrally directed acceleration is called centripetal acceleration. This acceleration acts along the radius of the curved path (thus is also referred to as radial acceleration).
Any acceleration must be produced by some force. Therefore, any force or combination of forces can cause centripetal acceleration. A few examples include the tension in the rope on a...
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Dynamics Of Circular Motion: Applications01:17

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Suppose a car moves on flat ground and turns to the left. The centripetal force causing the car to turn in a circular path is due to friction between the tires and the road. For this, a minimum coefficient of friction is needed, or the car will move in a larger-radius curve and leave the roadway. Let's now consider banked curves, where the slope of the road helps in negotiating the curve. The greater the angle of the curve, the faster one can take the curve. It is common for race tracks for...
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在一个曲的表面上的时空光学旋摆.

Weifeng Ding, Zhaoying Wang

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    此摘要是机器生成的。

    研究人员研究了曲表面上的时空光学 (STOVs). 他们发现STOVs表现出独特的摆形般的强度波动和可预测的轨道角动量交换在恒定的高斯曲率表面.

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    科学领域:

    • 光学和光子学 在光学和光子学.
    • 数学物理 数学物理

    背景情况:

    • 时空光学 (STOV) 是一种新的结构光场.
    • 了解曲面上的光传播对于先进的光学应用至关重要.

    研究的目的:

    • 在二维恒定高斯曲率表面 (CGCS) 上研究 STOV 的传播动力学.
    • 在对轴近似下,在正曲线的CGCS上获得STOV传播的分析解决方案.

    主要方法:

    • 在分析解决方案中使用矩阵光学方法.
    • 在CGCS.上分析了在对轴近似下STOV传播.

    主要成果:

    • 在曲的表面上,STOVs表现出类似的强度摆动,与平面不同.
    • 当表面曲率半径等于光的雷利距离时,这种摆动就会停止.
    • 内在和外在的轨道角动量 (OAM) 定期交换,总横向OAM为零.

    结论:

    • 这项研究为CGCS.com上的STOV传播提供了分析解决方案.
    • 这些发现为控制复杂空间中的横向外部OAM提供了洞察力.
    • 独特的动力学使其在光学计时器件中的潜在应用成为可能.