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Related Concept Videos

Viscosity of Fluid01:19

Viscosity of Fluid

Viscosity measures the resistance a fluid offers to flow and deformation. It results from internal friction between layers of fluid moving relative to one another. Dynamic viscosity, denoted by the Greek letter mu (μ), quantifies the force needed to move one fluid layer over another. For Newtonian fluids like water and air, the relationship between the shearing stress and the rate of shearing strain is linear, meaning their viscosity remains constant regardless of the applied stress.
Stokes' Law01:20

Stokes' Law

Viscous forces, like friction, are intermolecular forces that resist the relative motion of molecules over each other. When a solid body moves through a liquid, viscous forces drag it in the opposite direction. The force's magnitude depends on the solid's shape and size, as well as its speed and the liquid's coefficient of viscosity, density and temperature.
The expression for the force on a solid spherical object in a fluid is called Stokes' law. Stokes' law is valid only for low Reynolds...
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Individual molecules in a gas move in random directions, but a gas containing numerous molecules has a predictable distribution of molecular speeds, which is known as the Maxwell-Boltzmann distribution, f(v).
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Capillarity in Fluid01:19

Capillarity in Fluid

Capillarity describes the movement of liquid in small spaces without external forces acting on it. The capillarity is driven by surface tension and adhesive interactions between the liquid and surrounding solid surfaces. This effect is often seen in narrow tubes, porous materials, and fine particles.
Surface tension is crucial to capillarity. It results from cohesive forces between liquid molecules at the liquid-air boundary, forming a skin that resists external forces. When the capillary tube...
Accelerating Fluids01:17

Accelerating Fluids

When a fluid is in constant acceleration, the pressure and buoyant force equations are modified. Suppose a beaker is placed in an elevator accelerating upward with a constant acceleration, a. In the beaker, assume there is a thin cylinder of height h with an infinitesimal cross-sectional area, ΔS.
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Dimensionless Groups in Fluid Mechanics01:15

Dimensionless Groups in Fluid Mechanics

Dimensionless groups in fluid mechanics provide simplified ratios that help analyze fluid behavior without relying on specific units. The Reynolds number (Re), which represents the ratio of inertial to viscous forces, distinguishes between laminar and turbulent flows, making it essential in the design of pipelines and aerodynamic surfaces. The Froude number (Fr), the ratio of inertial to gravitational forces, is particularly useful in predicting wave formation and hydraulic jumps in...

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Related Experiment Video

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Experimental Measurement of Settling Velocity of Spherical Particles in Unconfined and Confined Surfactant-based Shear Thinning Viscoelastic Fluids
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Transport coefficients for the hard-sphere granular fluid.

Aparna Baskaran1, James W Dufty, J Javier Brey

  • 1Department of Physics, University of Florida, Gainesville, Florida 32611, USA.

Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|June 4, 2008
PubMed
Summary

This study details Navier-Stokes hydrodynamics for inelastic hard spheres, providing exact expressions for cooling rate and transport coefficients. Results are compared to elastic systems, offering insights into granular fluid behavior.

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Area of Science:

  • Physics
  • Fluid Dynamics
  • Statistical Mechanics

Background:

  • Linear response methods were previously used for general Navier-Stokes order hydrodynamics.
  • The prior analysis encompassed normal and granular fluids with diverse collision rules.

Purpose of the Study:

  • Specialize general hydrodynamic expressions to smooth, inelastic, hard spheres.
  • Derive explicit formulas for key physical parameters.
  • Compare inelastic results with those for elastic systems.

Main Methods:

  • Application of linear response theory.
  • Mathematical derivation for specific particle interactions (inelastic hard spheres).
  • Comparative analysis between inelastic and elastic hard sphere systems.

Main Results:

  • Formally exact expressions for cooling rate, pressure, and transport coefficients.
  • Quantitative comparison of transport properties in inelastic versus elastic granular fluids.
  • Demonstration of specialized hydrodynamic parameters for inelastic collisions.

Conclusions:

  • The derived expressions provide a foundation for further analytical and numerical studies.
  • Highlights the distinct behavior of granular fluids under inelastic collisions.
  • Confirms the utility of linear response methods for complex fluid systems.