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Multigrid unsteady Navier-Stokes calculations with aeroelastic applications
103
Citations
16
References
1995
Year
AeroacousticsUnsteady FlowAeronauticsEngineeringImplicit ApproachIncompressible FlowAerospace EngineeringFluid MechanicsTurbulence ModelingAeroelasticityAerodynamicsCircular CylinderNumerical DissipationNavier-stokes EquationsComputational MechanicsAerostructureAeroelastic Applications
An implicit approach to the solution of the unsteady two-dimensional Navier-Stokes equations is presented.After spatial discretization, the resulting set of coupled implicit non-linear equations is solved iteratively.This is accomplished using well proven convergence acceleration techniques for explicit schemes such as multigrid, residual averaging, and local time-stepping in order to achieve large computational efficiency in the calculation.Calculations are performed in parallel using a domain decomposition technique with optimized communication requirements.In addition, particular care is taken to minimize the effect of numerical dissipation with flux-limited dissipation schemes.Results for the unsteady shedding flow behind a circular cylinder and for a pitching NACA 64A010 airfoil are presented with experimental comparisons, showing the feasibility of accurate, efficient, time-dependent viscous calculations.Finally, a two-dimensional structural model of the cylinder is coupled with the unsteady flow solution, and time responses of the deflections of the structure are analyzed.Nomenclature C l coefficient of lift C d coefficient of drag Cx, Cy damping coefficients in the two coordinate directions D cylinder diameter, cylinder drag E total energy (internal plus kinetic) E(wij ) convective Euler fluxes f , g Euler flux vectors H total enthalpy Kx, Ky spring constants in the two coordinate directions L airfoil section lift (normal to free stream), positive up m cylinder mass M∞ free stream Mach number n frequency, 1/sec NS(wij ) viscous flux residual for cell i,j p static pressure qi heat flux component R(wij ) total flux residual for cell i,j R * modified residual R, S viscous flux vectors ReD Reynolds number based on the diameter St Strouhal frequency, St = nD U∞ T static temperature u, v cartesian velocity components U∞ free stream velocity Vij volume of i,j cell w vector of flow variables
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