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Angular Momentum: Single Particle01:10

Angular Momentum: Single Particle

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Angular momentum is directed perpendicular to the plane of the rotation, and its magnitude depends on the choice of the origin. The perpendicular vector joining the linear momentum vector of an object to the origin is called the “lever arm.” If the lever arm and linear momentum are collinear, then the magnitude of the angular momentum is zero. Therefore, in this case, the object rotates about the origin such that it lies on the rim of the circumference defined by the lever arm...
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Angular Momentum01:21

Angular Momentum

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Angular momentum characterizes an object's rotational motion and is defined as the moment of its linear momentum about a specified point O. When a particle moves along a curved path in the x-y plane, the scalar formulation calculates the magnitude of its angular momentum, utilizing the moment arm (d), representing the perpendicular distance from point O to the line of action of the linear momentum. Despite being scalar in formulation, angular momentum is inherently a vector quantity. Its...
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Conservation of Angular Momentum: Application01:18

Conservation of Angular Momentum: Application

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A system's total angular momentum remains constant if the net external torque acting on the system is zero. Examples of such systems include a freely spinning bicycle tire that slows over time due to torque arising from friction, or the slowing of Earth's rotation over millions of years due to frictional forces exerted on tidal deformations. However in the absence of a net external torque, the angular momentum remains conserved. The conservation of angular momentum principle requires a...
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Conservation of Angular Momentum01:09

Conservation of Angular Momentum

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A system's total angular momentum remains constant if the net external torque acting on the system is zero. Considering a system that consists of n tiny particles, the angular momentum of any tiny particle may change, but the system's total angular momentum would remain constant. The principle of conservation of angular momentum only considers the net external torque acting on the system. While there are internal forces exerted by different particles within the system that also produce...
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Angular Momentum about an Arbitrary Axis01:11

Angular Momentum about an Arbitrary Axis

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Imagine a rigid body with a mass denoted as 'm', which has its center of mass at point G and is rotating around an inertial reference frame. The angular momentum at an arbitrary point P can be calculated by taking the cross product of the position vector and linear momentum vector for each individual mass element.
The velocity of a mass element comprises its translational velocity and the relative velocity instigated by the body's rotation. Substituting the velocity equation into...
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Angular Momentum: Rigid Body01:11

Angular Momentum: Rigid Body

16.0K
The total angular momentum of a rigid body can be calculated using the summation of the angular momentum of all the tiny particles rotating in the same plane. Considering all the tiny particles rotating in the x-y plane, the direction of angular momentum of all such particles and that of the rigid body would be perpendicular to the plane of the rotation along the z-axis.
This calculation can get complicated when tiny particles within the rigid body are not rotating in the same plane but have...
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Video Experimental Relacionado

Updated: Mar 17, 2026

Shaping the Amplitude and Phase of Laser Beams by Using a Phase-only Spatial Light Modulator
08:39

Shaping the Amplitude and Phase of Laser Beams by Using a Phase-only Spatial Light Modulator

Published on: January 28, 2019

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Microlaser de movimiento angular orbital

Pei Miao1, Zhifeng Zhang1, Jingbo Sun1

  • 1Department of Electrical Engineering, The State University of New York at Buffalo, Buffalo, NY 14260, USA.

Science (New York, N.Y.)
|July 30, 2016
PubMed
Resumen
Este resumen es generado por máquina.

Los investigadores crearon un láser de microanillo que genera un vórtice de impulso angular orbital (OAM). Este avance en la fotónica no hermetiana controla con precisión la carga topológica y la polarización OAM para las comunicaciones ópticas avanzadas.

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Automation of Mode Locking in a Nonlinear Polarization Rotation Fiber Laser through Output Polarization Measurements
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Automation of Mode Locking in a Nonlinear Polarization Rotation Fiber Laser through Output Polarization Measurements

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Área de la Ciencia:

  • Óptica y fotónica
  • Física no hermética
  • Lasers a microescala

Sus antecedentes:

  • La luz estructurada, incluido el momento angular orbital (OAM), ofrece capacidades avanzadas en óptica.
  • La generación de láseres OAM a micro y nanoescala es crucial para aumentar la capacidad de información.
  • La fotónica no hermética y los puntos excepcionales ofrecen nuevos paradigmas de diseño para dispositivos ópticos.

Objetivo del estudio:

  • Para demostrar un láser de microanillo capaz de generar láser de vórtice OAM de modo único.
  • Para controlar con precisión la carga topológica del modo OAM.
  • Para permitir la manipulación bajo demanda de la polarización para la emisión de vórtice radialmente polarizada.

Principales métodos:

  • Explotación de los principios de diseño de la fotónica no hermética en un punto excepcional.
  • Desarrollo de una estructura láser de microrrado para la generación de OAM.
  • Integración de los mecanismos de control de polarización dentro del micro láser.

Principales resultados:

  • Demostración exitosa de un láser de microrrado que produce láser de vórtice OAM de modo único.
  • Control preciso de la carga topológica de los modos OAM generados.
  • Logró la manipulación de la polarización bajo demanda, resultando en una emisión de vórtice radialmente polarizada.

Conclusiones:

  • El microlaser OAM desarrollado genera y controla efectivamente los haces de vórtice OAM.
  • Esta tecnología aprovecha la fotónica no hermética para funcionalidades ópticas avanzadas.
  • Las aplicaciones potenciales incluyen dispositivos optoelectrónicos integrados de próxima generación para comunicaciones ópticas cuánticas y clásicas.