“…In an integral formulation where W 1 , W 2 and * correspond respectively to two test functions and to a dimensionally consistent scalar product in R 4 , this can be written as follows: (30) defines v NS (c) as soon as c is given. The delicate point is that v NS (c) is defined on a domain X c which varies with c. The contribution of Hadamard and of other workers addressing this issue is to give a rigorous context to the differentiation of v NS (c) with respect to c. The reader interested in this theory can examine Refs.…”
Section: Hadamard Formulation For Domain Deformationmentioning
“…In an integral formulation where W 1 , W 2 and * correspond respectively to two test functions and to a dimensionally consistent scalar product in R 4 , this can be written as follows: (30) defines v NS (c) as soon as c is given. The delicate point is that v NS (c) is defined on a domain X c which varies with c. The contribution of Hadamard and of other workers addressing this issue is to give a rigorous context to the differentiation of v NS (c) with respect to c. The reader interested in this theory can examine Refs.…”
Section: Hadamard Formulation For Domain Deformationmentioning
“…To avoid potential di culties associated with grid deformation and the ROM procedure described above, a transpiration boundary condition is applied at y = 0 to model the e ects of a moving boundary without grid deformation [23]. For the bump problem examined herein, the transpiration boundary condition involves the enforcement of the exact condition of impermeability at the panel surface,…”
Section: Initial and Boundary Conditionsmentioning
SUMMARYThe response of a uid moving above a panel to localized oscillation of the panel is predicted using reduced-order modelling (ROM) with the proper orthogonal decomposition technique. The ow is assumed to be inviscid and is modelled with the Euler equations. These non-linear equations are discretized with a total-variation diminishing algorithm and are projected onto an energy-optimal subspace deÿned by an energy-threshold criterion applied to a modal representation of time series data. Results are obtained for a bump oscillating in a Mach 1.2 ow. ROM is found to reduce the degrees of freedom necessary to simulate the owÿeld by three orders of magnitude while preserving solution accuracy. Other observed beneÿts of ROM include increased allowable time step and robustness to variation of oscillation amplitude. Published in
“…This boundary condition is known as the transpiration boundary [18]. The geometry motion and grid motion need not coincide, and the difference is compensated by prescribing a transversal flow along the boundary (effectively a linearization of the correct boundary motion on the incorrect mesh).…”
Section: Motion Representation Under Time Refinementmentioning
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