Overview🔗
- Solver: simpleFoam
- Incompressible
- Steady
- Laminar
- Multiple Reference Frame (MRF)
- TODO: tutorial path
The case comprises two cylinders, with inner radius \(R_1\) rotating with angular velocity \(\Omega_1\), and outer radius \(R_2\) rotating with angular velocity \(\Omega_2\).
The laminar case corresponds to a Reynolds number of 100. where the Reynolds number os defined as:
\[Re = \frac{|\u_0| d}{\nu}\]Where \(\u_0\) is the angular velocity of the inner cylinder, i.e.
\[\u_0 = \Omega_1 R_1\]and \(d\) is the distance between the cylinders, i.e. \(R_2 - R_1\). Using an inner and outer radii of 1 and 2, respectively, and setting the kinematic viscosity to \(1\), the angular velocity of the inner cylinder is 100 rad/s.
Analytical solution🔗
Taylor [77] shows that the velocity, \(\u_{\theta}\) is described by:
\[\u_{\theta} = A r + \frac{B}{r}\]where \(A\) and \(B\) are constants defined as:
\[A = \frac{\Omega_1 \left( 1 - \mu \frac{R_2^2}{R_1^2} \right)}{1 - \frac{R_2^2}{R_1^2}}\] \[B = \frac{R_1^2 \Omega_1 (1 - \mu)}{1 - \frac{R_1^2}{R_2^2}}\]Here, \(\Omega_1\) and \(\Omega_2\) are the rotational speeds of the inner and outer cylinders, and
\[\mu = \frac{\Omega_2}{\Omega_1}\]The steady flow equations for this case, in cylindrical co-ordinates reduces to
\[\frac{1}{\rho}\frac{\partial p}{\partial r} - \frac{\u_{\theta}^2}{r} = 0\]On integrating with respect to radius an expression for the pressure is recovered:
\[p = \frac{A^2 r^2}{2} + 2 A B \ln (r) + \frac{B^2}{2 r^2} + C\]Mesh🔗
- 2D structured mesh created using blockMesh
Boundary conditions🔗
- Outer cylinder fixed
- Inner cylinder rotates at a fixed angular velocity
Results🔗
The rotational velocity, \(\u_\theta\) can be directly reported during the calculation using a fieldCoordinateSystemTransform function object.
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