cfx12 04 solver

38
4-1 ANSYS, Inc. Proprietary © 2009 ANSYS, Inc. All rights reserved. April 28, 2009 Inventory #002598 Chapter 4 Solver Settings Introduction to CFX

Upload: arvind-srinivasan

Post on 02-Jul-2015

969 views

Category:

Design


4 download

TRANSCRIPT

Page 1: Cfx12 04 solver

4-1ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Chapter 4

Solver Settings

Introduction to CFX

Page 2: Cfx12 04 solver

Solver Settings

4-2ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training ManualOverview

• Initialization

• Solver Control

• Output Control

• Solver Manager

Note: This chapter considers solver settings for steady-state simulations. Settings specific to transient simulation are discussed in a later chapter.

Page 3: Cfx12 04 solver

Solver Settings

4-3ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training Manual

• Iterative solution procedures require that all solution variables are assigned initial values before calculating a solution

• A good initial guess can reduce the solution time

• In some cases a poor initial guess may cause the solver to fail during the first few iterations

• The initial values can be set in 3 ways:

1. Solver automatically calculates the initial values

2. Initial values are entered by the user

3. Initial values are obtained from a previous solution

• Initial values can be set on a per-domain basis or globally for all domains

Initialization

Page 4: Cfx12 04 solver

Solver Settings

4-4ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training ManualInitialization – Setting Initial Values

• Insert Global Initialisation from the toolbar or by right-clicking on Flow Analysis 1

• Edit each Domain to set initial values on a per-domain basis– When both are defined the

domain settings take precedence

– Solid domain must have initial conditions set on a per-domain basis

Page 5: Cfx12 04 solver

Solver Settings

4-5ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training ManualInitialization – Setting Initial Values

• The Automatic option means that the CFX-Solver will calculate an initial value for the solved variable unless a previous results file is provided

– Will be based on boundary condition values and domain settings

• The Automatic with Value option means that the specified value will be used unless a previous results file is provided

– Can use a constant value or an expression

Page 6: Cfx12 04 solver

Solver Settings

4-6ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training ManualInitialization – Using a Previous Solution

• To use a previous solution as the initial guess enable the Initial Values Specification toggle when launching the Solver

– You can provide multiple initial values files

• When simulating a system you can provide previous solutions for each component of the system as the initial guess

• Usually each file would correspond to a separate region of space

• It is best if domains in the Solver Input File do not overlap with multiple initial values files

Page 7: Cfx12 04 solver

Solver Settings

4-7ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training Manual

• Edit the Solver Control object in the Outline tree

Solver Control – Editing

Page 8: Cfx12 04 solver

Solver Settings

4-8ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training Manual

• The Solver Control panel contains various controls that influence the behavior of the solver

• These controls are important for the accuracy of the solution, the stability of the solver and the length of time it takes to obtain a solution

Solver Control – Options

Page 9: Cfx12 04 solver

Solver Settings

4-9ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training ManualSolver Control – Advection Scheme

• The Advection Scheme refers to the way the advection term in the transport equations is modeled numerically

– i.e. the term that accounts for bulk fluid motion– Often the dominant term

• Three schemes are available, High Resolution, Upwind and Specified Blend

– Discussed in more detail next

• There is rarely any reason to change from the default High Resolution scheme

Unsteady

Advection

Diffusion

Generation

Page 10: Cfx12 04 solver

Solver Settings

4-10ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training ManualSolver Control – Advection Scheme Theory

• Solution data is stored at nodes, but variable values are required at the control volume faces to calculate fluxes

• The upstream nodal values (φ up) are interpolated to the integration points (φ ip) on the control volume faces using:

– Where is the variable gradient and is the vector between the upstream node and the integration point

– In other words, the ip value is equal to the upstream value plus a correction due to the gradient

– β can have values between 0 and 1 …

φip φup β φ∇ ∆r⋅+=

∇φ φip φup β φ∇ ∆r⋅+=

Page 11: Cfx12 04 solver

Solver Settings

4-11ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training ManualSolver Control – Advection Scheme Theory

• If β = 0 we get the Upwind advection scheme, i.e. no correction

– This is robust but only first order accurate– Sometimes useful for initial runs, but

usually not necessary

• The Specified Blend scheme allows you to specify β between 0 and 1 (i.e. between no correction up to full correction)

– But this is not guaranteed to be bounded, meaning that when the correction is included it can overshoot or undershoot what is physically possible

• The High Resolution scheme maximizes β throughout the flow domain while keeping the solution bounded

φip φup β φ∇ ∆r⋅+= Theory

High ResolutionScheme

Upwind Scheme

β=1.00

Flow is misaligned with mesh

0

1

Page 12: Cfx12 04 solver

Solver Settings

4-12ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training ManualSolver Control – Turbulence Numerics

• Regardless of the Advection Scheme selection, the Turbulence equations default to the First Order (Upwind) scheme

– Usually this is sufficient

• The High Resolution scheme can be selected for additional accuracy

– Can give better accuracy in boundary layers on unstructured meshes

Page 13: Cfx12 04 solver

Solver Settings

4-13ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training ManualSolver Control – Convergence Control

• The Solver will finish when it reaches Max. Iterations unless convergence is achieved sooner

– If Max. Iterations is reached you may not have a converged solution

– Can be useful to set Max. Iterations to a large number

• When the Solver finishes you should always check why it finished

• Fluid Timescale Control sets the timescale in a steady-state simulation …

Page 14: Cfx12 04 solver

Solver Settings

4-14ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training Manual

• ANSYS CFX employs the so called False Transient Algorithm– A timescale is used to move the solution towards the final answer

• In a steady-state simulation the timescale provides relaxation of the equation non-linearities

• A steady-state simulation is a “transient” evolution of the flow from the initial guess to the steady-state conditions

– Converged solution is independent of the timescale used

Initial Guess

50 iterations

100 iterations

150 iterations

Final Solution

Solver Control – Timescale Background

Page 15: Cfx12 04 solver

Solver Settings

4-15ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training Manual

• For obtaining successful convergence, the selection of the timescale plays an important role

– If the timescale is too large, the convergence becomes bouncy or may even lead to the failure of the Solver

– If the timescale is too small, the convergence will be very slow and the solution may not be fully accurate

Solver Control – Timescale Selection

Page 16: Cfx12 04 solver

Solver Settings

4-16ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training ManualSolver Control – Timescale Selection

• For advection dominated flow, a fraction of the fluid residence time is often a good estimate for the timescale

– A timescale of 1/3 of (Length Scale / Velocity Scale) is often optimal

– May need a smaller timescale for the first few iterations and for complex physics, transonic flow,…..

• For rotating machines, 1/ω (ω in rad/s) is a good choice

• For buoyancy driven flows, the timescale should be based on a function of gravity, thermal expansivity, temperature difference and length scale (see documentation)

Page 17: Cfx12 04 solver

Solver Settings

4-17ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training Manual

• Timescale Control can be Auto Timescale, Physical Timescale or Local Timescale Factor

• Physical Timescale

– Specify the timescale. Usually a constant but can also be variable via an expression

– Can often set a better timescale than Auto Timescale would produce – faster convergence

Solver Control – Timescale Control

Page 18: Cfx12 04 solver

Solver Settings

4-18ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training ManualSolver Control – Timescale Control

• Auto Timescale– The Solver calculates a timescale based on

boundary / initial conditions or current solution and domain length scale

– Use a Conservative or Aggressive estimate for the domain length scale, or a specified value

– Timescale is re-calculated and updated every few iterations as the flow field changes

– Can set a Maximum Timescale to provide an upper limit

– Tends to produce a conservative timescale

– Timescale factor (default = 1) is a multiplier which can be changed to adjust the automatically calculated timescale

Page 19: Cfx12 04 solver

Solver Settings

4-19ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training Manual

• Local Timescale Factor– Timescale varies throughout the domain

– Can accelerate convergence when vastly different local velocity scales exist• E.g. a jet entering a plenum

– Best used on fairly uniform meshes, since small element will have a small timescale which can slow convergence

– Local Timescale Factor is a multiplier of the local timescale– Never use as final solution; always finish off with a constant timescale

Local Timescale =Local Mesh Length Scale

Local Velocity Scale

Smaller Timescale in high velocity and/or fine mesh regions

Solver Control – Timescale Control

Page 20: Cfx12 04 solver

Solver Settings

4-20ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training ManualSolver Control – Convergence Criteria

• Convergence Criteria settings determine when the solution is considered converged and hence when the Solver will stop

– Assuming Max. Iterations is not reached

• Residuals are a measure of how accurately the set of equations have been solved

– Since we are iterating towards a solution, we never get the exact solution to the equations

– Lower residuals mean a more accurate solution to the set of equations (more on the next slide)

– Do not confuse accurately solving the equations with overall solution accuracy – the equations may or may not be a good representation of the true system!

– Residuals are just one measure of accuracy and should be combined with other measures:

• Monitor Points (ch. 8) and Imbalances (below)

Page 21: Cfx12 04 solver

Solver Settings

4-21ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training Manual

• The continuous governing equations are discretized into a set of linear equations that can be solved. The set of linear equations can be written in the form:

[A] [Φ] = [b]

where [A] is the coefficient matrix and [Φ] is the solution variable

• If the equation were solved exactly we would have:

[A] [Φ] - [b] = [0]

• The residual vector [R] is the error in the numerical solution:

[A] [Φ] - [b] = [R]

• Since each control volume has a residual we usually look at the RMS average or the maximum normalized residual

Solver Control – Residuals Theory

Page 22: Cfx12 04 solver

Solver Settings

4-22ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training Manual

• Residual Type– MAX: Convergence based on maximum

residual anywhere– RMS: Convergence based on average

residual from all control volumes

– Root Mean Square =

• Residual Target– For reasonable convergence MAX residuals

should be 1.0E-3, RMS should be at least 1.0E-4

– The targets dependent on the accuracy needed

• Lower values may be needed for greater accuracy

n

2∑i

iR

Solver Control – Residuals

Page 23: Cfx12 04 solver

Solver Settings

4-23ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training ManualSolver Control – Conservation Target• The Conservation Target sets a target for the

global imbalances

• The imbalances measure the overall conservation of a quantity (mass, momentum, energy) in the entire flow domain

Flux Maximum

OutFlux InFlux Imbalance %

−=

• Clearly in a converged solution Flux In should equal Flux Out

• It’s good practice to set a Conservation Target and/or monitor the imbalances during the run

• When set, the Solver must meet both the Residual and Conservation Target before stopping (assuming Max. Iterations is not reached)

• Set a target of 0.01 (1%) or less– Flux In – Flux Out < 1%

Page 24: Cfx12 04 solver

Solver Settings

4-24ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training Manual

• Elapsed Time Control– Can specify the maximum wall clock time

for a run– Solver will stop after this amount of time

regardless of whether it has converged

• Interrupt Control– Can specify other criteria for stopping

the Solver based on logical CEL expressions

– When the expression returns true the solver will stop

• Any value >= 0.5 is true

Solver Control – Elapsed Time and Interrupt Control

– Examples• If temperature exceeds a specified value

if(areaAve(T)@wall>200[C],1,0)

• If mesh quality drops below a specified value in a moving mesh case

– More on logical expressions in the CEL lecture

Page 25: Cfx12 04 solver

Solver Settings

4-25ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training Manual

• This option is only available when a solid domain is included in the simulation

• The Solid Timescale should be selected such that it is MUCH larger than the fluid timescale (100 times larger is typical)

– the energy equation is usually very stable in the solid zone

– solid timescales are typically much larger than fluid timescales

Solver Control – Solid Timescale Control

• The fluid timescale is estimated using Length Scale / Velocity Scale

• The solid timescale is automatically calculated as function of the length scale, thermal conductivity, density and specific heat capacity

– Or you can choose the Physical Timescale option and provide a timescale directly

Page 26: Cfx12 04 solver

Solver Settings

4-26ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training Manual

• The Equation Class Settings tab is an advanced option that can be used to set Solver controls on an equation specific basis

– Not usually needed– Will override the controls set on Basic

Settings for the selected equation

• Advanced Options– Advanced solver control options– Rarely needed

Solver Control – Equation Class Settings

Page 27: Cfx12 04 solver

Solver Settings

4-27ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training ManualOutput Controls – Results

• The Output Control settings control the output produced by the Solver

– The Trn Results, Trn Stats and Export tab only apply to transient simulations and are covered in the Transient chapter

• The Results tab controls the final .res file– Generally do not use the Selected Variables (or None!)

option since it probably won’t contain enough information to restart the run later

– Output Equation Residuals is useful if you need to check where convergence problems are occurring

– Extra Output Variables Listcontains variables that are notwritten to the standard resultsfile

• E.g. Vorticity

Page 28: Cfx12 04 solver

Solver Settings

4-28ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training Manual

Frequency of output can be adjusted

Output Controls – Backup

• The Backup tab controls if and when backup results files are automatically written by the Solver

• Recommend for long Solver runs in case of power failure, network interruptions, etc

• Option:– Standard: Like a full results file– Essential: Allows a clean solver restart– Smallest: Can restart the solver, but there’ll

be a jump in the residuals– Selected Variables: Not recommended

• Can also manually request a backup file from the Solver Manager at any time

Page 29: Cfx12 04 solver

Solver Settings

4-29ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training Manual

• The Monitor tab allows you to create Monitor Points

– These are used to track values of interest as the Solver runs

• The Cartesian Coordinates Option is used to track the value of a variable at a specific X, Y, Z location

• The Expression Option is used to monitor the values of a CEL expression

– E.g. Calculate the area average of Cp at the inlet boundary: areaAve(Cp)@inlet

– E.g. Mass flow of particular fluid through an outlet: oil.massFlow()@outlet

• In steady-state simulations you should create monitor points for quantities of interest

– One measure of convergence is when these values are no longer changing

Output Controls – Monitor

Page 30: Cfx12 04 solver

Solver Settings

4-30ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training Manual

• The CFX-Solver Manager is a graphical user interface used to:– Define a run– Control the CFX-Solver interactively– View information about the emerging solution– Export data

Solver Manager

Page 31: Cfx12 04 solver

Solver Settings

4-31ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training Manual

• Define a new Solver run

• Solver Input File should be the .def file– Can also pick .res, .bak or _full.trn files to restart a

previous incomplete run

• To make a physics change and restart a solution, create a new .def file and provide it as the Solver Input File then select the .res, .bak or _full.trn file in the Initial Values Specification section

– If both files have the same physics, this is the same as picking the .res/.bak/_full.trn file as the input file

• Use Mesh From selects which mesh to use. If the meshes are identical can use either option, otherwise:

– If you use the Solver Input File mesh, the Initial Values solution is interpolated onto the input file

– If you use the Initial Values mesh only the physics from the Solver Input File is used

• Continue History From carriers over convergence history and iteration counters

Solver Manager – Defining a Run

Page 32: Cfx12 04 solver

Solver Settings

4-32ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training ManualSolver Manager – Defining a Parallel Run

• By default the Solver will run in serial– A single solver process runs on the local

machine

• Set the Run Mode to one of the parallel options to make use of multiple cores/processors

– Requires parallel licenses– Allows you to divide a large CFD problem into

smaller partitions• Faster solution times• Solve larger problems by making use of memory

(RAM) on multiple machines

• The Local Parallel options should be used when running on a single machine

• The Distributed Parallel options should be used when running across multiple machines

Page 33: Cfx12 04 solver

Solver Settings

4-33ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training Manual

• Serial

• Local Parallel

• Distributed Parallel

• Different communication methods are available (MPICH2, HP MPI, PVM)– See documentation “When To Use MPI or PVM” for more details, but HP MPI is

recommended in most cases

Solver Manager – Defining a Parallel Run

Page 34: Cfx12 04 solver

Solver Settings

4-34ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training Manual

• The Show Advanced Control toggle enables the Partitioner, Solver and Interpolator tabs

• On the Partitioner tab you can pick different partitioning algorithms

– Partitioning is always a serial process– Can be a problem for v.large cases since you

cannot distribute the memory load across multiple machines

– The default MeTiS algorithm uses more memory than others, so if you run out of memory use a different method (see documentation for details)

• Multidomain Option:– Independent Partitioning: Each domain is

partitioned into n partitions– Coupled Partitioning: All domains are combined

and then partitioned into n partitions• There’s a specific option for Transient Rotor Stator

cases

Solver Manager – Define Run Advanced Controls

Page 35: Cfx12 04 solver

Solver Settings

4-35ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training Manual

• On the Solver tab you can select the Double Precision option

– The solver will use more significant figures in its calculations

– Doubles solver memory requirements– Use when round-off error could be a problem – if

‘small’ variations in a variable are important, where ‘small’ is relative to the global range of that variable, e.g:

• Many Mesh Motion cases, since the motion is often small relative to the size of the domain

• Most CHT cases, since thermal conductivity is vastly different in the fluid and solid

• If you have a wide pressure range, but small pressure changes are important

– Small values by themselves do not need DP

Solver Manager – Define Run Advanced Controls

• The Solver estimates its memory requirements upfront• Memory Alloc Factor is a multiplier for this estimate

– Use when the solver stops with an “Insufficient Memory Allocated” error

Page 36: Cfx12 04 solver

Solver Settings

4-36ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training ManualSolver Manager – Interactive Solver Control

• During a solution Edit Run in Progress lets you make changes on the fly– Models generally cannot be changed, but timescales, BC’s, etc can

Page 37: Cfx12 04 solver

Solver Settings

4-37ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training Manual

.out fileMonitor Plot

Solver Manager – Additional Solution Monitors

Right-click

• By default monitor plots are created showing the RMS residuals for each equation solved, plus one plot for any monitor points

• Right-click to switch between RMS and MAX

• Additional monitors can be selected showing:

– Imbalances– Boundary fluxes (FLOW)– Boundary forces

• Tangential (viscous)• Normal (pressure)

– Source terms …

New Monitor

Page 38: Cfx12 04 solver

Solver Settings

4-38ANSYS, Inc. Proprietary© 2009 ANSYS, Inc. All rights reserved.

April 28, 2009Inventory #002598

Training Manual

Start a new Simulation

Monitor Run in Progress

Monitor Finished Run

Stop Current Run

Save Current Run

Switch Residual Plot

between RMS and

MAX

• By dragging the cursor over any icon, the feature description will appear

Solver Manager – Additional Icons