A rectangular conduit with a closed end has water flowing in/out at the other end. The water level at the open end has an imposed sinusoidal movement. When this level is higher than the ceiling of the conduit, a certain mass of air is trapped under the ceiling. In a previous article (T.D. Nguyen, La
Numerical Simulation of the Lock-In Effect of a Fixed-Fixed Tube in Cross Flow
โ Scribed by Michael Fischer; Klaus Strohmeier
- Publisher
- John Wiley and Sons
- Year
- 1999
- Tongue
- English
- Weight
- 461 KB
- Volume
- 22
- Category
- Article
- ISSN
- 0930-7516
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โฆ Synopsis
This paper deals with the development of a numerical calculation code that is able to simulate the three-dimensional flow through a heat exchanger tube bundle and therefore allows a coupled calculation of fluid-structure interaction between the flow and the tube bundle. The incompressible flow field is calculated by a Navier-Stokes solver using a first-order power law scheme, a SIMPLEC algorithm to calculate the pressure and velocity correction fields, and a line-by-line Gauss-Seidl tridiagonal algorithm to solve the linearised system of equations. The transient parts of the Navier-Stokes equations are discretised by a second-order forward finite differencing scheme. The turbulence is examined with the aid of a large-eddy turbulence model. The transient fluid forces acting on the tubes are calculated by integration of all local flow pressure values on the surfaces of the tubes. As an example a single fixed-fixed cylinder in a flow channel is considered using the structural calculation part already developed as well as the new flow field and flow forces subroutines. The time series of the tube's motion and the fluid forces acting on the tube are analysed by Fourier's transformation. The lock-in effect occurring when the vortex shedding frequency approaches the first natural frequency of the tube can be excellently demonstrated by varying the inflow velocity over a wide range of Reynolds numbers.
๐ SIMILAR VOLUMES
A direct numerical scheme is developed to study the temporal ampliยฎcation of a 2D disturbance in plane Poiseuille ยฏow. The transient non-linear NavierยฑStokes equations are applied in a region of wavelength moving with the wave propagation speed. The complex amplitude involved in the perturbation fun