Taylor-Couette Flow
Taylor-Couette flow describes the flow of a liquid enclodes by two rotating cylinders. The inner cylinder of radius $r_i$ rotates with angular frequency $\omega_i$, the outer cylinder of radius $r_o$ rotates with angular frequency $\omega_o$.
Governing Equations
In a cylindrical domain of dimensions $d \times 2\pi \times L$, where $d = r_o - r_i$, the governing equations for Taylor-Couette flow are given by
with boundary conditions
where $\omega_o$ and $\omega_i$ are the angular frequencies of respectively the outer and inner cylinders. In the $\theta$-direction we apply periodic conditions, i.e. $u(r, 0, z, t) = u(r, 2\pi, z, t)$ and similar for other quantities. See Symbols for the definition of all quantities used here.
Nondimensional formulation
In TransiFlow, we implement the following nondimensionalized equations
with boundary conditions
Here length is scaled by $r_i$, $u = \tilde u v_i$, $t = \tilde t r_i / v_i$, $p = \tilde p \rho_0 v_i^2 - \rho_0gz$, $\omega = \tilde \omega v_i / r_i$. Moreover, the Taylor number is given by $\mathrm{Ta} = v_i r_i / \nu = \mathrm{Re}_i r_i / d = \mathrm{Re}_i (\eta^{-1} - 1)^{-1}$ with $\eta = r_i / r_o$. All other quantities are defined in Symbols.
Parameters
These are the relevant parameters in the parameters dictionary for this problem type.
Parameter name |
Default value |
Notes |
|---|---|---|
|
Set to |
|
|
1.0 |
Unused if Ta is defined |
|
Re / (1 / eta - 1) |