Error bounds on engineering turbulence models: A framework for uncertainty quantification (UQ) Sharath S. Girimaji Department of Aerospace Engineering Texas A&M University 2011 Annual meeting of American Physical Society – Division of Fluid Dynamics Baltimore, Maryland November 20, 2011
APS talk by girimaji on Uncertainty quantification for turbulence
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Error bounds on engineering turbulence models: A framework for uncertainty quantification (UQ)
Sharath S. Girimaji
Department of Aerospace EngineeringTexas A&M University
2011 Annual meeting of American Physical Society – Division of Fluid Dynamics Baltimore, Maryland
November 20, 2011
Motivation
Someday CFD will replace experiments as the main design tool
Are we there yet? Not really
Why not? Turbulence modeling, numerics etc.
Which is more important? Modeling errors (IMHO)
Current modeling status Making lines pass through symbols,
Current engineering models not predictive
but post-dictive
For engineering turbulence models to become predictive tools:
1.Improve fidelity
2. Uncertainty quantification
UQ in turbulence context
• How do you assess error/uncertainty of a chaotic system?
• Is the concept of UQ meaningful in turbulence computations?
• Is standard UQ terminology/framework applicable to turbulence?
Best we can do: Ignorance management UQ
What should we aim for: In the absence of data
• Catastrophic failure detection
• Physics-based error/uncertainty estimates
Or at least: as in Hurricane trajectory predictions
• Multi-valued prediction envelop; not a single-valued prediction
• Multiple calculations w/different models
Further Questions
Is Reynolds stress a metric of error in mean flow prediction?• Yes: In a well-conducted experiment
• No: In a good numerical implementation of a bad model
• No: In a bad numerical implementation of a good model
• May be: In a good numerical implementation of a good model
Therefore,
1)Mean flow UQ is possible only if Reynolds stress is reliable
2)UQ of Reynolds stress is necessary
Objectives
Develop a framework for UQ of Reynolds stress Rij:
• Identify general sources of uncertainties in Rij
• Characterize and categorize general sources of uncertainties
• Develop guidelines/procedures for quantifying source errors
Provide some direction for Rij UQ in• Empirical/Semi-empirical closure• Higher-order physics based closure
Types of uncertainty – turbulence context
General Types of uncertaintyAleatoric/statistical uncertainty: • From sources outside model parameters• Statistical analysis to quantify uncertainty
• Bayesian approach possible
Epistemic /systematic uncertainty: • From sources within – but not accounted for due to various reasons• Physics-based analysis needed to quantify uncertainty
• Must be based on turbulence physics
Generally, both aleatoric and epistemic occur together and difficult to separate
Sources of Uncertainty
Model Calculations: Mean and moments are not chaotic
Numerical errors: aleatoric/epistemic – standard V&V may apply
Closure errors: Type of error depends upon the level of
modeling
•Empirical models large aleatoric errors
•Physics-based models more epistemic errors
Empirical closure models
Empirical models: Zero equation closures
•Most errors aleatoric; no basis for establishing epistemic error
•Model coefficient sensitivity can be established
•For a given flow, best-fit model coefficient can be found
• Bayesian Analysis
•No basis for assessing error in a new family of flows
Semi-empirical models: Standard 1 & 2 equation models
•For K & possible to distinguish aleatoric and epistemic
•Error in constitutive relation can be estimated using ARSM
Incomplete UQ of CGiven the constitutive model ij = -C Sij
Epistemic uncertainty can estimated using the ARSM closure model.
ARSM reduction
RANSLESDNS
2-eqn. ARSM
Averaging Invariance
Application
7-eqn. SMC Multi-point/global
stability effects
Linear Pressure
Effects: RDT
Nonlinear pressure effects
Spectral and dissipative processes
2-eqn. PANS
Navier-Stokes Equations
Reynolds stress closure models
Any attempt at UQ must start at RSCM level• Turbulent transport Gradient-Diffusion model• Remaining closures Piece-wise homogeneous
All closure models based on incomplete information
Critical `game-changing’ closure• Inhomogeneity Missing global stability physics•Rapid Pressure-strain correlation (r) Missing information
Less critical Closures• Slow Pressure-strain correlation (s) Missing information•Dissipation () Missing details of cascade
Global Instabilities
Flow instabilities are the biggest reason of RSCM error• Multi-point phenomena not amenable to one-point closure
• Large-scale inviscid instabilities more dynamically important
• Small-scale viscous instabilities interesting but unimportant
• Dissipative and not dynamically important
Must resolve large-scale inviscid instabilities
rational UQ unlikely
What else can be done:
Possibility of instability can be forecast and be prepared
for all consequences
Global Instability/Coherent Structure Forecast
Hypothetical velocity amplitude vector
Ominous sign 1: Large variation in velocity gradients
Global Instability/Coherent Structure Forecast
Ominous sign 2: Vanishing 2nd derivative
UQ Rapid Pressure Strain Corr.Traditional RPSC development
•Much theoretical/analytical work to improve RPSC fidelity•Seeking single-valued closure model – despite multi-valued possibility
• = f(R, A, ) simplified to = f(R, A)
•In pursuit of an improbable single-valued closure with limited basis• Conflicting closure requirements (realizability vs. linearity)• Unholy compromises made • Much knowledge of physics discarded
Change in model development paradigm• Multivalued closure model: For a given R and A,
• min = f(R, A) based on worst case • probable = f(R, A) based on most probable • max = f(R, A) based on best case
Redirect modeling effort to explore the range of closure space and identify most probable
Closed streamline flows : Modal behavior.
Most unstable mode
Most stable mode
Most unstable mode
Most stable mode
Closed streamline flows : envelope.
Hypothetical velocity amplitude vector
Envelope of probable behavior
Some observations on UQ for turbulence closures
Epistemic UQ possible only at RSCM level
Locality and incomplete basis are main reasons for epistemic uncertainty
Success of UQ hinges on how well we can fill-in incomplete information
Critical Uncertainty 1: Global stability effectsVirtually impossible to fill-in at one-point closure level