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increasing mesh quality is leading to poor convergence |
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May 4, 2009, 18:27 |
increasing mesh quality is leading to poor convergence
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#1 |
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Join Date: Apr 2009
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Hello!
I am trying to make a mesh quality study. Therefore, i'd like to calculate the average heat transfer coeficient of a wall. (attached you can find a jpeg about the geometry, the meshing and the momentum and mass chart) The fluid domain is air at 400°C in a very narrow duct with an overall lenght of about 6m, the solid domain is steel. I'm using a SST - model . Inlet condition: 21.8m/s, 400°C Outlet condition: Average Static Pressure 0 Pa (i also tried a velocity of 21.8m/s but nothing changes) On both walls of the fluid i am using inflation. As long as i keep the overall number of elements below 700 000, the simulation reaches a convergence of 1.0e-004 within 35-40 time steps. The result for the heat transfer coeficcient looks reasonably correct. Everytime i am increasing the the mesh quality by decreasing the min. edge length at default face spacing, the simulations has a very very poor convergence. That means, it eaven don't reaches 1.0e-003, as you can see in the attached chart! (eg. from 500 000 to 1 400 000 nodes), Can you see any obvious mistakes in my simulation? Are there some general tips how to solve such problems (narrow duct which is very long)? This is one of my first cfx simulations and i am waiting for my instruction course. Many thanks in advance, tippo Ps: i know that a convergence with 1.000e-004 is also not good, but that is as far as i get in the moment. Outputfile with bad convergence: This run of the CFX-11.0 Solver started at 21:25:51 on 4 May 2009 by user Andreas on NB-ANDREAS (intel_p3.sse_winnt5.1) using the command: "C:\Programme\ANSYS Inc\v110\CFX\bin\perllib\cfx5solve.pl" -stdout-comms -batch -ccl - -P 35 -sharedlic-port 1177 Setting up CFX Solver run ... +--------------------------------------------------------------------+ | | | CFX Command Language for Run | | | +--------------------------------------------------------------------+ LIBRARY: MATERIAL: Air at 25 C Material Description = Air at 25 C and 1 atm (dry) Material Group = Air Data, Constant Property Gases Option = Pure Substance Thermodynamic State = Gas PROPERTIES: Option = General Material Thermal Expansivity = 0.003356 [K^-1] ABSORPTION COEFFICIENT: Absorption Coefficient = 0.01 [m^-1] Option = Value END DYNAMIC VISCOSITY: Dynamic Viscosity = 1.831E-05 [kg m^-1 s^-1] Option = Value END EQUATION OF STATE: Density = 1.185 [kg m^-3] Molar Mass = 28.96 [kg kmol^-1] Option = Value END REFERENCE STATE: Option = Specified Point Reference Pressure = 1 [atm] Reference Specific Enthalpy = 0. [J/kg] Reference Specific Entropy = 0. [J/kg/K] Reference Temperature = 25 [C] END REFRACTIVE INDEX: Option = Value Refractive Index = 1.0 [m m^-1] END SCATTERING COEFFICIENT: Option = Value Scattering Coefficient = 0.0 [m^-1] END SPECIFIC HEAT CAPACITY: Option = Value Specific Heat Capacity = 1.0044E+03 [J kg^-1 K^-1] Specific Heat Type = Constant Pressure END THERMAL CONDUCTIVITY: Option = Value Thermal Conductivity = 2.61E-02 [W m^-1 K^-1] END END END MATERIAL: Steel Material Group = CHT Solids, Particle Solids Option = Pure Substance Thermodynamic State = Solid PROPERTIES: Option = General Material EQUATION OF STATE: Density = 7854 [kg m^-3] Molar Mass = 55.85 [kg kmol^-1] Option = Value END REFERENCE STATE: Option = Specified Point Reference Specific Enthalpy = 0 [J/kg] Reference Specific Entropy = 0 [J/kg/K] Reference Temperature = 25 [C] END SPECIFIC HEAT CAPACITY: Option = Value Specific Heat Capacity = 4.34E+02 [J kg^-1 K^-1] END THERMAL CONDUCTIVITY: Option = Value Thermal Conductivity = 60.5 [W m^-1 K^-1] END END END END FLOW: SOLUTION UNITS: Angle Units = [rad] Length Units = [m] Mass Units = [kg] Solid Angle Units = [sr] Temperature Units = [K] Time Units = [s] END SIMULATION TYPE: Option = Steady State EXTERNAL SOLVER COUPLING: Option = None END END DOMAIN: Fluid Coord Frame = Coord 0 Domain Type = Fluid Fluids List = Air at 25 C Location = B4 BOUNDARY: Default Fluid Solid Interface Side 1 Boundary Type = INTERFACE Location = F1762.4 BOUNDARY CONDITIONS: HEAT TRANSFER: Option = Conservative Interface Flux END WALL INFLUENCE ON FLOW: Option = No Slip END END END BOUNDARY: Fluid Default Boundary Type = WALL Location = F1306.4,F981.4,F985.4 BOUNDARY CONDITIONS: HEAT TRANSFER: Option = Adiabatic END WALL INFLUENCE ON FLOW: Option = No Slip END END END BOUNDARY: inlet Boundary Type = INLET Location = Inlet BOUNDARY CONDITIONS: FLOW REGIME: Option = Subsonic END HEAT TRANSFER: Option = Static Temperature Static Temperature = 400 [C] END MASS AND MOMENTUM: Normal Speed = 21.82 [m s^-1] Option = Normal Speed END TURBULENCE: Option = Medium Intensity and Eddy Viscosity Ratio END END END BOUNDARY: outlet Boundary Type = OUTLET Location = Outlet BOUNDARY CONDITIONS: FLOW REGIME: Option = Subsonic END MASS AND MOMENTUM: Option = Average Static Pressure Relative Pressure = 0 [Pa] END PRESSURE AVERAGING: Option = Average Over Whole Outlet END END END DOMAIN MODELS: BUOYANCY MODEL: Option = Non Buoyant END DOMAIN MOTION: Option = Stationary END MESH DEFORMATION: Option = None END REFERENCE PRESSURE: Reference Pressure = 1 [atm] END END FLUID MODELS: COMBUSTION MODEL: Option = None END HEAT TRANSFER MODEL: Option = Thermal Energy END THERMAL RADIATION MODEL: Option = None END TURBULENCE MODEL: Option = SST END TURBULENT WALL FUNCTIONS: Option = Automatic END END INITIALISATION: Option = Automatic INITIAL CONDITIONS: Velocity Type = Cartesian CARTESIAN VELOCITY COMPONENTS: Option = Automatic END EPSILON: Option = Automatic END K: Option = Automatic END STATIC PRESSURE: Option = Automatic END TEMPERATURE: Option = Automatic with Value Temperature = 400 [C] END END END END DOMAIN: Solid Domain Type = Solid Location = B874 Solids List = Steel BOUNDARY: Default Fluid Solid Interface Side 2 Boundary Type = INTERFACE Location = F1765.874 BOUNDARY CONDITIONS: HEAT TRANSFER: Option = Conservative Interface Flux END END END BOUNDARY: Solid Default Boundary Type = WALL Location = F1641.874,F1779.874,F843.874,F845.874,F847.874 BOUNDARY CONDITIONS: HEAT TRANSFER: Option = Adiabatic END END END DOMAIN MODELS: DOMAIN MOTION: Option = Stationary END MESH DEFORMATION: Option = None END END INITIALISATION: Option = Automatic INITIAL CONDITIONS: TEMPERATURE: Option = Automatic with Value Temperature = 400 [C] END END END SOLID MODELS: HEAT TRANSFER MODEL: Option = Thermal Energy END THERMAL RADIATION MODEL: Option = None END END END DOMAIN INTERFACE: Default Fluid Solid Interface Boundary List1 = Default Fluid Solid Interface Side 1 Boundary List2 = Default Fluid Solid Interface Side 2 Interface Type = Fluid Solid INTERFACE MODELS: Option = General Connection FRAME CHANGE: Option = None END PITCH CHANGE: Option = None END END MESH CONNECTION: Option = Automatic END END OUTPUT CONTROL: RESULTS: File Compression Level = Default Option = Standard END END SOLVER CONTROL: ADVECTION SCHEME: Option = High Resolution END CONVERGENCE CONTROL: Maximum Number of Iterations = 80 Physical Timescale = 2 [h] Solid Timescale Control = Auto Timescale Timescale Control = Physical Timescale END CONVERGENCE CRITERIA: Residual Target = 1.E-4 Residual Type = RMS END DYNAMIC MODEL CONTROL: Global Dynamic Model Control = On END END EXPERT PARAMETERS: topology estimate factor = 1.3 END END COMMAND FILE: Version = 11.0 Results Version = 11.0 END EXECUTION CONTROL: INTERPOLATOR STEP CONTROL: Runtime Priority = Standard EXECUTABLE SELECTION: Double Precision = Off END MEMORY CONTROL: Memory Allocation Factor = 1.0 END END PARALLEL HOST LIBRARY: HOST DEFINITION: nbandreas Remote Host Name = NB-ANDREAS Installation Root = C:\Programme\ANSYS Inc\v%v\CFX Host Architecture String = intel_p3.sse_winnt5.1 END END PARTITIONER STEP CONTROL: Multidomain Option = Independent Partitioning Runtime Priority = Standard EXECUTABLE SELECTION: Use Large Problem Partitioner = Off END MEMORY CONTROL: Memory Allocation Factor = 1.0 END PARTITIONING TYPE: MeTiS Type = k-way Option = MeTiS Partition Size Rule = Automatic END END RUN DEFINITION: Definition File = C:/Dokumente und \ Einstellungen/Andreas/Desktop/Stroemi/Stroemi1.def Interpolate Initial Values = Off Run Mode = Full END SOLVER STEP CONTROL: Runtime Priority = Standard EXECUTABLE SELECTION: Double Precision = Off END LICENSE CONTROL: Preferred License = 35 Shared License Port = 1177 END MEMORY CONTROL: Memory Allocation Factor = 1.0 END PARALLEL ENVIRONMENT: Number of Processes = 1 Start Method = Serial END END END +--------------------------------------------------------------------+ | | | Solver | | | +--------------------------------------------------------------------+ |
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May 4, 2009, 21:09 |
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#2 |
Super Moderator
Glenn Horrocks
Join Date: Mar 2009
Location: Sydney, Australia
Posts: 17,870
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Have a look here for some tips:
http://www.cfd-online.com/Wiki/Ansys...gence_criteria In your case I bet the better mesh refinement has lead to transient features being resolved. If the flow really is steady state then larger physical time steps should help. If it is truly transient then there is no alternative but to do transient simulations. Glenn Horrocks |
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May 5, 2009, 11:55 |
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#3 |
New Member
Join Date: Apr 2009
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Hello,
thank you, i will read through this paper. best regards tippo |
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