2005
DOI: 10.1002/fld.1045
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Finite element and implicit Runge-Kutta implementation of an acoustics-convection upstream resolution algorithm for the time-dependent two-dimensional Euler equations

Abstract: SUMMARYThe second of a two-paper series, this paper details a solver for the characteristics-bias system from the acoustics-convection upstream resolution algorithm for the Euler and Navier-Stokes equations. An integral formulation leads to several surface integrals that allow e ective enforcement of boundary conditions. Also presented is a new multi-dimensional procedure to enforce a pressure boundary condition at a subsonic outlet, a procedure that remains accurate and stable. A classical ÿnite element Galer… Show more

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Cited by 6 publications
(7 citation statements)
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“…For threedimensional formulations, 16j63, and with R denoting the real-number ÿeld, the independent variable (x; t), x ≡ (x 1 ; x 2 ; x 3 ), in (1) When the 'viscosity' ux f j , 16j63, identically vanishes, this system is hyperbolic when the eigenvalues of the Jacobian matrix (@f j (q)=@q)n j are all real for arbitrary unit vectors n with direction cosines n j , the components of n along the coordinate axes. The system is also termed 'strongly' hyperbolic when this matrix possess a full set of eigenvectors [21,22].…”
Section: Navier-stokes and Euler Equationsmentioning
confidence: 99%
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“…For threedimensional formulations, 16j63, and with R denoting the real-number ÿeld, the independent variable (x; t), x ≡ (x 1 ; x 2 ; x 3 ), in (1) When the 'viscosity' ux f j , 16j63, identically vanishes, this system is hyperbolic when the eigenvalues of the Jacobian matrix (@f j (q)=@q)n j are all real for arbitrary unit vectors n with direction cosines n j , the components of n along the coordinate axes. The system is also termed 'strongly' hyperbolic when this matrix possess a full set of eigenvectors [21,22].…”
Section: Navier-stokes and Euler Equationsmentioning
confidence: 99%
“…The integral formulation for system (1), [23,24], seeks a solution q ∈ H 1 ( ), subject to prescribed boundary conditions on @ ≡ \ , such that for all test functionsŵ ∈ H where n j , 16j63, denotes the jth component of the outward pointing unit vector perpendicular to @ . For 2-D ows, 16j62, the dependent-variable array q = q(x; t) as well as the inviscid and viscous ux 'vector' components f j and f j are then deÿned as …”
Section: Navier-stokes and Euler Equationsmentioning
confidence: 99%
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