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.
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.
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.
Related Concept Videos
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' 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...
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...
Maxwell-Boltzmann Distribution: Problem Solving
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).
This distribution function f(v) is defined by saying that the expected number N (v1,v2) of particles with speeds between v1 and v2 is given by
This distribution function f(v) is defined by saying that the expected number N (v1,v2) of particles with speeds between v1 and v2 is given by
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...
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 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.
The motion of the liquid within this infinitesimal cylinder is considered to obtain the pressure difference. Three vertical forces act on this liquid:
The motion of the liquid within this infinitesimal cylinder is considered to obtain the pressure difference. Three vertical forces act on this liquid:
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...


