Transition to Turbulence

From UMaine SECS Numerical Modeling Laboratory
Revision as of 23:28, 19 February 2019 by Ian (talk | contribs)
Jump to: navigation, search

Created by Ian Nesbitt and Jukes Liu on 2019-02-19

In this module, you will learn how viscosity affects the dynamics of a simple fluid system with a single cylindrical impediment placed in the flow path. Our tools in this endeavor are COMSOL Multiphysics and ParaView. At the end of the module, you should be able to describe the initial conditions of a system, the transition from laminar to turbulent flow, and the effect viscosity has on the inertia, complexity, and predictability of a system.

We will start with a higher viscosity regime and move to lower viscosity.

First, let's start by learning how to talk about the various components of flow.

Basics

Model

Honey (μ = 101.5 Pa s)

In the first example, we have a fluid with the viscosity of about that of honey, 101.5 Pascal seconds (Pa s). This is a two-dimensional example, but let's assume that this model has a depth that does not affect the flow in any way. Both the horizontal walls and the walls of the cylinder on the left side of the model have a "no slip" condition. This means that as the flow gets closer to the wall, velocity goes to zero. This condition sets up a velocity gradient.

Velocity field

Mu101.5 ux1 velocity.gif

Shear rate

Mu101.5 ux1 shear.gif

Vorticity magnitude

Mu101.5 ux1 vorticity.gif

Reynolds number

Mu101.5 ux1 reynolds.gif

Pressure

Mu101.5 ux1 pressure.gif


Water (μ = 10-3 Pa s)

Air (μ = 10-5 Pa s)