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Supersonic 2D Ramp Air Intake Outlet Back Pressure 

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February 5, 2022, 05:43 
Supersonic 2D Ramp Air Intake Outlet Back Pressure

#1 
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Hello everyone,
I'm trying to run viscous simulation for Supersonic flow over 2D Ramp Air Intake of McDonnell Douglas F15 Eagle. But I have a problem with Outlet boundary conditions. As a result of the simulation, when the flow passes through the throat of the air intake, it slows down as expected due to the oblique shocks and decreases to subsonic speeds. But the problem is that as the flow moves towards the outlet, it speeds up again and reaches supersonic speeds. Everything I tried to prevent this was unsuccessful. No matter how much I changed the Outlet Back Pressure, the result was still the same. Should I define the Outlet back pressure more than the static Pressure I have defined for Inlet? It didn't make sense for me. You can see my configuration file and my boundary markers below. I'm also attaching the simulation results from Praview. Could someone help me to understand how should I solve this problem? I would be really appriciate for any kind of suggesstion. This is my graduation project. %  DIRECT, ADJOINT, AND LINEARIZED PROBLEM DEFINITION % % % Physical governing equations (EULER, NAVIER_STOKES, % WAVE_EQUATION, HEAT_EQUATION, FEM_ELASTICITY, % POISSON_EQUATION) SOLVER= RANS % % Specify turbulence model (NONE, SA, SA_NEG, SST, SA_E, SA_COMP, SA_E_COMP, SST_SUST) KIND_TURB_MODEL= SST % % Mathematical problem (DIRECT, CONTINUOUS_ADJOINT) MATH_PROBLEM= DIRECT % % Restart solution (NO, YES) RESTART_SOL= NO % % System of measurements (SI, US) % International system of units (SI): ( meters, kilograms, Kelvins, % Newtons = kg m/s^2, Pascals = N/m^2, % Density = kg/m^3, Speed = m/s, % Equiv. Area = m^2 ) % United States customary units (US): ( inches, slug, Rankines, lbf = slug ft/s^2, % psf = lbf/ft^2, Density = slug/ft^3, % Speed = ft/s, Equiv. Area = ft^2 ) SYSTEM_MEASUREMENTS= SI %  NONEQUILIBRIUM GAS, IDEAL GAS, POLYTROPIC, VAN DER WAALS AND PENG ROBINSON CONSTANTS % % % Fluid model (STANDARD_AIR, IDEAL_GAS, VW_GAS, PR_GAS, % CONSTANT_DENSITY, INC_IDEAL_GAS, INC_IDEAL_GAS_POLY, MUTATIONPP, SU2_NONEQ) FLUID_MODEL= STANDARD_AIR % %  COMPRESSIBLE AND INCOMPRESSIBLE FREESTREAM DEFINITION % % % Mach number (nondimensional, based on the freestream values) MACH_NUMBER= 2.2 % % Reynolds number (nondimensional, based on the freestream values) REYNOLDS_NUMBER= 6947291 % Reynolds length (1 m, 1 inch by default) REYNOLDS_LENGTH= 1.0 % % Angle of attack (degrees) AOA= 3 % % Sideslip angle (degrees) SIDESLIP_ANGLE= 0.0 % % Freestream pressure (101325.0 N/m^2 by default, only Euler flows) FREESTREAM_PRESSURE= 8830 % % Freestream temperature (288.15 K by default) FREESTREAM_TEMPERATURE= 216.75 % % Freestream velocity (1.0 m/s, 1.0 ft/s by default) FREESTREAM_VELOCITY= ( 649.5, 0.00, 0.00 ) %  VISCOSITY MODEL % % % Viscosity model (SUTHERLAND, CONSTANT_VISCOSITY). VISCOSITY_MODEL= SUTHERLAND % % Sutherland Viscosity Ref (1.716E5 default value for AIR SI) MU_REF= 1.716E5 % % Sutherland Temperature Ref (273.15 K default value for AIR SI) MU_T_REF= 273.15 % % Sutherland constant (110.4 default value for AIR SI) SUTHERLAND_CONSTANT= 110.4 % %  REFERENCE VALUE DEFINITION % % % Reference origin for moment computation REF_ORIGIN_MOMENT_X = 0.25 REF_ORIGIN_MOMENT_Y = 0.00 REF_ORIGIN_MOMENT_Z = 0.00 % % Reference length for pitching, rolling, and yawing nondimensional moment REF_LENGTH= 1.0 % % Reference area for force coefficients (0 implies automatic calculation) REF_AREA= 1.0 %  BOUNDARY CONDITION DEFINITION % % % NavierStokes (noslip), constant heat flux wall marker(s) (NONE = no marker) % Format: ( marker name, constant heat flux (J/m^2), ... ) MARKER_HEATFLUX= ( UpperWall, 0, LowerWall, 0 ) % % Marker of the far field (0 implies no marker) MARKER_FAR= ( FarField ) % % Supersonic inlet boundary marker(s) (NONE = no marker) % Total Conditions: (inlet marker, temperature, static pressure, velocity_x, % velocity_y, velocity_z, ... ), i.e. all variables specified. MARKER_SUPERSONIC_INLET= ( Inlet, 216.75, 8830, 649.5, 0.0, 0.0 ) % % Outlet boundary marker(s) (NONE = no marker) % Format: ( outlet marker, back pressure (static), ... ) MARKER_OUTLET= ( Outlet, 1000.0 ) % % Marker(s) of the surface to be plotted or designed MARKER_PLOTTING= ( Outlet ) % % Marker(s) of the surface where the functional (Cd, Cl, etc.) will be evaluated MARKER_MONITORING= ( UpperWall, LowerWall ) %  COMMON PARAMETERS DEFINING THE NUMERICAL METHOD % % % Numerical method for spatial gradients (GREEN_GAUSS, LEAST_SQUARES, % WEIGHTED_LEAST_SQUARES) NUM_METHOD_GRAD= WEIGHTED_LEAST_SQUARES % % CourantFriedrichsLewy condition of the finest grid CFL_NUMBER= 5.0 % % Adaptive CFL number (NO, YES) CFL_ADAPT= NO % % Parameters of the adaptive CFL number (factor down, factor up, CFL min value, % CFL max value ) CFL_ADAPT_PARAM= ( 0.1, 2.0, 5.0, 1e10 ) % % RungeKutta alpha coefficients RK_ALPHA_COEFF= ( 0.66667, 0.66667, 1.000000 ) % % Number of total iterations ITER= 100000 % % Linear solver for the implicit formulation (BCGSTAB, FGMRES) LINEAR_SOLVER= FGMRES % % Preconditioner of the Krylov linear solver (ILU, JACOBI, LINELET, LU_SGS) LINEAR_SOLVER_PREC= ILU % % Min error of the linear solver for the implicit formulation LINEAR_SOLVER_ERROR= 1E6 % % Max number of iterations of the linear solver for the implicit formulation LINEAR_SOLVER_ITER= 20 %  MULTIGRID PARAMETERS % % % MultiGrid Levels (0 = no multigrid) MGLEVEL= 0 % % Multigrid cycle (V_CYCLE, W_CYCLE, FULLMG_CYCLE) MGCYCLE= W_CYCLE % % Multigrid presmoothing level MG_PRE_SMOOTH= ( 1, 2, 3, 3 ) % % Multigrid postsmoothing level MG_POST_SMOOTH= ( 0, 0, 0, 0 ) % % Jacobi implicit smoothing of the correction MG_CORRECTION_SMOOTH= ( 0, 0, 0, 0 ) % % Damping factor for the residual restriction MG_DAMP_RESTRICTION= 1.0 % % Damping factor for the correction prolongation MG_DAMP_PROLONGATION= 1.0 %  FLOW NUMERICAL METHOD DEFINITION % % % Convective numerical method (JST, LAXFRIEDRICH, CUSP, ROE, AUSM, HLLC, % TURKEL_PREC, MSW) CONV_NUM_METHOD_FLOW= JST % % Monotonic Upwind Scheme for Conservation Laws (TVD) in the flow equations. % Required for 2nd order upwind schemes (NO, YES) MUSCL_FLOW= YES % % Slope limiter (NONE, VENKATAKRISHNAN, VENKATAKRISHNAN_WANG, % BARTH_JESPERSEN, VAN_ALBADA_EDGE) SLOPE_LIMITER_FLOW= VENKATAKRISHNAN % % Coefficient for the limiter (smooth regions) VENKAT_LIMITER_COEFF= 0.006 % % 2nd and 4th order artificial dissipation coefficients JST_SENSOR_COEFF= ( 0.5, 0.02 ) % % Time discretization (RUNGEKUTTA_EXPLICIT, EULER_IMPLICIT, EULER_EXPLICIT) TIME_DISCRE_FLOW= EULER_IMPLICIT %  CONVERGENCE PARAMETERS % % % Convergence criteria (CAUCHY, RESIDUAL) CONV_FIELD= RMS_DENSITY % % Min value of the residual (log10 of the residual) CONV_RESIDUAL_MINVAL= 8 % % Start convergence criteria at iteration number CONV_STARTITER= 10 % % Number of elements to apply the criteria CONV_CAUCHY_ELEMS= 100 % % Epsilon to control the series convergence CONV_CAUCHY_EPS= 1E10 %  TURBULENT NUMERICAL METHOD DEFINITION % % % Convective numerical method (SCALAR_UPWIND) CONV_NUM_METHOD_TURB= SCALAR_UPWIND % % Time discretization (EULER_IMPLICIT) TIME_DISCRE_TURB= EULER_IMPLICIT % % Reduction factor of the CFL coefficient in the turbulence problem CFL_REDUCTION_TURB= 1.0 

February 5, 2022, 06:43 

#2 
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Or should I define the outlet marker as INC_OUTLET_TYPE= MASS_FLOW_OUTLET . Then set a appropriate massflow rate for outlet to be able to decrease the mach towards the outlet.


February 5, 2022, 17:30 

#3 
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Pedro Gomes
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You should not mix inlets and outlets with farfield when the associated surfaces intersect.
A farfield boundary is both inlet and outlet depending on the flow direction, and both sub and supersonic depending on Mach number. Your domain also looks too small, look for guidelines on how far the boundaries should be from the surface. If it's all supersonic 10x might be enough but don't quote me on that, when in doubt test the sensitivity to your modelling assumptions. 

February 5, 2022, 17:37 

#4 
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Pedro Gomes
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You are also using a weird mix of methods.
JST is not great for supersonic or for detailed viscous stuff (not our implementation anyway). Try ROE with the van Albada limiter and green Gauss gradients. And SST is probably overkill, SA is usually fine for external aero stuff and you can get away with higher y+. 

February 5, 2022, 18:08 

#5  
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Quote:
But I'm sorry, I just couldn't understand the point about the not mixing inlets and outlets with Farfield. I also ran another simulation without the outside region for the same geometry before as you can see in the attachment picture. However I had the result with same problem. 

September 7, 2023, 10:44 

#6 
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Miguel García
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I´m having the same problem, I don´t know how to impose a backpressure at the outlet. I´m trying to get the normal shock in the divergent zone, but the flow continues being supersonic, so it gets accelerated. Did you get the solution?


September 9, 2023, 02:42 

#7 
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Zhang
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I think the back pressure is setted at the MARKER_OUTLET. I don't know if I understand this correctly.


March 15, 2024, 18:45 

#8 
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Jeswin Joseph
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This reply might be too late, but...
I think the solution is physically correct. The back pressure could be much less than the design condition for the nozzle and the exit flow becomes supersonic. Try increasing the Mach number close to the inlet static pressure (say 0.75 times inlet static pressure) and you may see a subsonic outlet flow. Reviewing gas dynamics of convergent divergent nozzles will help in this regard. 

Tags 
su2, supersonic, supersonic inlet, viscous 
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