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Thin-Walled Hollow Shafts01:15

Thin-Walled Hollow Shafts

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In analyzing a thin-walled hollow shaft subjected to torsional loading, a segment with width dx is isolated for examination. Despite its equilibrium state, this segment faces torsional shearing forces at its ends. These forces are quantitatively described by the product of the longitudinal shearing stress on the segment's minor surface and the area of this surface, leading to the concept of shear flow. This shear flow is consistent throughout the structure, indicating a uniform distribution of...
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Plane Potential Flows01:23

Plane Potential Flows

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Plane potential flows simplify fluid motion by assuming the fluid to be irrotational and incompressible. These characteristics allow these flows to be described by a velocity potential function, ϕ, representing the flow speed in a given direction, and a stream function, ψ, that visualizes the flow path, both governed by Laplace's equation. These parameters help in estimating flow patterns, velocity distributions, and pressure fields around various hydraulic structures.
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Rolling Without Slipping01:09

Rolling Without Slipping

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People have observed the rolling motion without slipping ever since the invention of the wheel. For example, one can look at the interaction between a car's tires and the surface of the road. If the driver presses the accelerator to the floor so that the tires spin without the car moving forward, there must be kinetic friction between the wheels and the road's surface. If the driver slowly presses the accelerator, causing the car to move forward, the tires roll without slipping. It is...
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Irrotational Flow01:28

Irrotational Flow

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Irrotational flow is characterized by fluid motion where particles do not rotate around their axes, resulting in zero vorticity. For a flow to be irrotational, the curl of the velocity field must be zero. This imposes specific conditions on velocity gradients. For instance, to maintain zero rotation about the z-axis, the gradient condition:
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Characteristics of Fluids01:20

Characteristics of Fluids

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When a force is applied parallel to the top surface of a solid, it resists the applied force due to the internal frictional forces between the layers of the solid known as shearing resistance. However, when the force is removed, the shearing forces restore the original shape of the solid. Other deformation forces also cause temporary changes in shape if the forces are not beyond a threshold magnitude. Solids tend to retain their shape, making the study of their rest and motion easier. Beyond...
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Couette Flow01:22

Couette Flow

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Couette flow represents the flow of fluid between two parallel plates, with one plate fixed and the other moving with a constant velocity. This configuration allows for a simplified analysis using the Navier-Stokes equations, which govern fluid motion under conditions of viscosity and incompressibility. For Couette flow, the assumptions include a steady, laminar, incompressible flow with a zero-pressure gradient in the flow direction. This flow type is beneficial for understanding shear-driven...
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Video Experimental Relacionado

Updated: Feb 24, 2026

Controlling Flow Speeds of Microtubule-Based 3D Active Fluids Using Temperature
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Sólidos Activos: Auto-propulsión de Defectos Topológicos sin Flujo

Fridtjof Brauns1, Myles O'Leary2, Arthur Hernandez3

  • 1Kavli Institute for Theoretical Physics, University of California, Santa Barbara, Santa Barbara, California 93106, USA.

Physical review letters
|February 22, 2026
PubMed
Resumen
Este resumen es generado por máquina.

Los defectos topológicos auto-propulsados en sólidos activos se mueven mediante remodelación de la textura, no por flujo. Este nuevo mecanismo difiere de los fluidos activos y puede explicar la morfogénesis y regeneración de tejidos.

Palabras clave:
Sólidos activosDefectos topológicosAuto-propulsiónFísica de materia blandaMateriales activosFísica biológicaMorfogénesisRegeneración

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Área de la Ciencia:

  • Física de Materia Blanda
  • Ciencia de Materiales
  • Biofísica

Sus antecedentes:

  • Los defectos topológicos en fluidos nemáticos activos exhiben auto-propulsión debido a los campos de flujo que generan.
  • La comprensión de la dinámica de defectos en materiales activos similares a sólidos es crucial para los procesos biológicos.

Objetivo del estudio:

  • Proponer y analizar un modelo mínimo para defectos topológicos auto-propulsados en sólidos nemáticos activos.
  • Elucidar el mecanismo de movimiento de defectos en medios elásticos con tensión activa.

Principales métodos:

  • Desarrollo de un modelo teórico mínimo para un sólido nemático activo.
  • Análisis de la dinámica de defectos que surge del acoplamiento de la textura nemática y las deformaciones elásticas.
  • Investigación de la desvinculación de pares de defectos y la estabilización.

Principales resultados:

  • Los defectos +1/2 auto-propulsados se mueven por remodelación local de la textura nemática, independientemente de la advección.
  • Este mecanismo difiere fundamentalmente de la auto-propulsión en fluidos nemáticos activos.
  • El modelo predice la desvinculación de pares de defectos y la estabilización de defectos +1.

Conclusiones:

  • La auto-propulsión de defectos en sólidos activos ocurre a través de un novedoso mecanismo de remodelación local de la textura.
  • Este mecanismo ofrece información sobre la reconfiguración del orden orientacional durante la morfogénesis, como en las fibras musculares.
  • Los hallazgos pueden explicar la motilidad y fusión de defectos en la regeneración de tejidos, como en Hydra.