outflow boundary conditions
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2021 ◽  
Vol 2090 (1) ◽  
pp. 012045
Author(s):  
Nikolay M. Evstigneev ◽  
Oleg I. Ryabkov

Abstract The system of governing equations for the dynamics of the compressible viscous ideal gas is considered in the 3D bounded domain with the inflow and outflow boundary conditions. The cylinder is located in the domain. Such problem is simulated using the high order WENO-scheme for inviscid part of the equations and using 4-th order central approximation for the viscous tensor part with the third order temporal discretization. The method of Proper Orthogonal Decomposition (POD) is applied to the problem at hand in order to extract the most active nodes. Cascades of bifurcations of periodic orbits and invariant tori are found that correspond to the excitation in different POD modes. The approximation of the reduced order model is analyzed and it is shown that one cannot make parameter extrapolations for the reduced order model to capture the same dynamics as is observed in the original full size model.


2019 ◽  
Vol 142 (1) ◽  
pp. 55-102 ◽  
Author(s):  
Thierry Goudon ◽  
Stella Krell ◽  
Giulia Lissoni

2019 ◽  
Vol 179 ◽  
pp. 27-33 ◽  
Author(s):  
Xuanyu Zhao ◽  
Marco Bolognin ◽  
Dongfang Liang ◽  
Alexander Rohe ◽  
Philip J. Vardon

Author(s):  
Ted G. Bagwell ◽  
Kristin L. Cody

Flow over shallow cavities is a noise concern due to the possibility of flow tone lock-in with acoustic resonators. The principal aim of this work is to understand the factors that contribute to the onset of lock-in using Computational Fluid Dynamics (CFD) models. CFD models of shallow cavity lock-in to longitudinal acoustic resonators are developed and validated against existing test data from Lehigh University. All simulations are performed using AcuSolve™. A key technical contribution is the development of admittance inflow and impedance outflow boundary conditions to model the effects of the pipe resonator. The general trends predicted by the CFD models agree with the test data. In particular, the resonator response at the strong interaction point is well represented.


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