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Forced Oscillations01:06

Forced Oscillations

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When an oscillator is forced with a periodic driving force, the motion may seem chaotic. The motions of such oscillators are known as transients. After the transients die out, the oscillator reaches a steady state, where the motion is periodic, and the displacement is determined.
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Damped Oscillations01:07

Damped Oscillations

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In the real world, oscillations seldom follow true simple harmonic motion. A system that continues its motion indefinitely without losing its amplitude is termed undamped. However, friction of some sort usually dampens the motion, so it fades away or needs more force to continue. For example, a guitar string stops oscillating a few seconds after being plucked. Similarly, one must continually push a swing to keep a child swinging on a playground.
Although friction and other non-conservative...
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Simple Harmonic Motion01:21

Simple Harmonic Motion

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Simple harmonic motion is the name given to oscillatory motion for a system where the net force can be described by Hooke's law. If the net force can be described by Hooke's law and there is no damping (by friction or other non-conservative forces), then a simple harmonic oscillator will oscillate with equal displacement on either side of the equilibrium position. To derive an equation for period and frequency, the equation of motion is used. The period of a simple harmonic oscillator is given...
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Oscillations about an Equilibrium Position01:04

Oscillations about an Equilibrium Position

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Stability is an important concept in oscillation. If an equilibrium point is stable, a slight disturbance of an object that is initially at the stable equilibrium point will cause the object to oscillate around that point. For an unstable equilibrium point, if the object is disturbed slightly, it will not return to the equilibrium point. There are three conditions for equilibrium points—stable, unstable, and half-stable. A half-stable equilibrium point is also unstable, but is named so...
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Atomic Nuclei: Nuclear Relaxation Processes01:23

Atomic Nuclei: Nuclear Relaxation Processes

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In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis,  the precessing magnetic moments are randomly oriented around the z-axis.
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Standing Waves01:17

Standing Waves

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Sometimes waves do not seem to move; rather, they just vibrate in place. Unmoving waves can be seen on the surface of a glass of milk kept in a refrigerator, which is one example of standing waves. Vibrations from the refrigerator motor create waves on the milk that oscillate up and down but do not seem to move across the surface. These waves are formed or created by the superposition of two or more identical moving waves in opposite directions. The waves move through each other, with their...
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Video Experimental Relacionado

Updated: Jan 8, 2026

Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator
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Búsqueda por retorno: Rearranque estocástico en potenciales armónicos fluctuantes

Derek Frydel1

  • 1Department of Chemistry, Universidad Técnica Federico Santa María, Campus San Joaquin, Santiago, Chile.

Chaos (Woodbury, N.Y.)
|December 23, 2025
PubMed
Resumen

Este estudio explora el rearreglo estocástico (SR) con tiempos de retorno finitos, introduciendo un novedoso mecanismo de "búsqueda por retorno". Este enfoque reinicia con precisión las trayectorias de búsqueda de partículas, arrojando un tiempo de primera llegada medio de forma cerrada.

Palabras clave:
rearranque estocásticopotencial armónico fluctuantetiempo de primera llegada mediobúsqueda por retornofísica estadística

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Área de la Ciencia:

  • Física Estadística
  • Química Física
  • Sistemas Complejos

Sus antecedentes:

  • Los modelos de rearreglo estocástico (SR) de estrategias de búsqueda de partículas.
  • El SR estándar asume retornos instantáneos, lo cual no es realista.
  • Las duraciones de retorno finitas introducen imprecisión en los puntos de partida de la búsqueda.

Objetivo del estudio:

  • Analizar los procesos de SR con trayectorias de retorno de duración finita.
  • Investigar un mecanismo de retroalimentación que garantice puntos de rearreglo precisos.
  • Determinar los tiempos medios de primera llegada (MFPT) para protocolos de SR novedosos.

Principales métodos:

  • Utilización de un potencial armónico fluctuante para el confinamiento de partículas.
  • Implementación de retroalimentación posicional instantánea para controlar las trayectorias de retorno.
  • Análisis de protocolos de búsqueda, incluido un mecanismo de 'búsqueda por retorno'.

Principales resultados:

  • Desarrollado un método para el rearreglo preciso terminando las trayectorias de retorno en el origen.
  • Logrado puntos de partida consistentes para las fases de búsqueda difusiva.
  • Derivado un MFPT de forma cerrada para el protocolo de 'búsqueda por retorno'.

Conclusiones:

  • Los tiempos de retorno finitos en SR se pueden gestionar con control de retroalimentación.
  • El protocolo de 'búsqueda por retorno' ofrece una estrategia de búsqueda novedosa y eficiente.
  • Este trabajo proporciona nuevas perspectivas sobre la optimización de los procesos de búsqueda en sistemas complejos.