Viscosity
Average Speed The Maxwell-Boltzmann distribution is a function of the particle speed. The average speed follows from integration. Spherical shell in velocity- space The relative velocity between particles is reduced by sqrt(2).
Relative Speed The mean relative speed differs from the mean speed. Each molecule contributes
Collision Rate A reduced version of transport theory can found from a simple model of collisions. Probability P(t) Collision rate w The probability distribution in time is exponential. Normalized to 1 at t = 0 Differential probability p
Mean Free Path The mean time between collisions comes from the probability distribution. Integrate by parts The kinetic energy of a gas can be characterized by the mean particle speed. The mean free path combines the mean time and velocity.
Scattering Scattering cross-section depends on the relative size of particles and their relative velocity. Identical particles Relative velocity v ’, mass m, radius a. Hard spheres have cross sections independent of velocity. a a b
Relative Flux A particle in a small volume experiences a relative flux. Incidence based on relative speed The total scattered is the flux times the cross section. Collision rate The mean free path can be related to the cross section.
Shear Stress A stress is a force per unit area. Normal stress perpendicular to area Shear stress perpendicular A fluid in motion static can support a shear stress. Velocity gradient Coefficient of viscosity z uxux P zx P zz x
Momentum Transport One sixth of the particles will cross a plane in a given direction at a time. The stress is related to the net momentum change. Relate this to the gradient to get the viscosity coefficient .
Viscosity The viscosity is a retarding force due to motion in the fluid. Friction or drag The viscosity depends on the material and temperature, not on the density. Assumed low density – single collisions High enough density to primarily collide with particles, not walls
Self-Diffusion Assume a fluid that is non- uniform in one dimension. Number density n(z ) Identify a plane with a flux. Plane area A Perpendicular flux J z Flux proportional to gradient The proportionality is the coefficient of self-diffusion D.
Diffusion Equation The particles are conserved in the layer z. Relates number to flux Partial differential equation in t, z Use the assumed gradient to get a pde in n only. This is Fick’s diffusion equation.
Diffusion Coefficient One sixth of the particles will cross a plane in a given direction at a time. Find the flux from the mean velocity. Relate this to the gradient to get D.
Thermal Transport Consider the flow of heat through a plane. Temperature gradient Coefficient of thermal conductivity Find the coefficient by using the mean energy transfer. Relate to specific heat