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Optimization of Nonlinear, Coupled Fluid-Thermal Systems

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Presentation OutlineOverviewProject GoalsMicrogravity ResearchMGFLOOptimization TheoryPrevious Work Code Details Overview Validation Applications Conclusions Recommendations

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Слайд 1Optimization of Nonlinear, Coupled Fluid-Thermal Systems
Carrie Keyworth and Benjamin

Kirk
Advisors: Dr. Graham Carey and Bill Barth
ASE 463Q
May 3, 2000

Optimization of Nonlinear, Coupled Fluid-Thermal Systems Carrie Keyworth and Benjamin KirkAdvisors: Dr. Graham Carey and Bill BarthASE

Слайд 2Presentation Outline
Overview
Project Goals
Microgravity Research
MGFLO
Optimization Theory
Previous Work


Code Details
Overview
Validation

Applications

Conclusions
Recommendations

Presentation OutlineOverviewProject GoalsMicrogravity ResearchMGFLOOptimization TheoryPrevious Work Code Details Overview Validation Applications Conclusions Recommendations

Слайд 3Project Goals

To Design and Implement an optimization algorithm for a

fluid-thermal simulator
MGFLO
Boundary Condition Manipulation

Project Goals	To Design and Implement an optimization algorithm for a fluid-thermal simulatorMGFLOBoundary Condition Manipulation

Слайд 4Microgravity Fluid Research
Surface Tension
Smallest Surface Area Possible
Dominated on Earth by

Gravity, which Makes Surfaces Flat

Liquid Bridges
ALEX: A Liquid Electrohydrodynamics eXperiment
Surface

Tension Dominates with Decreased Electric Field



In a microgravity environment, surface tension and
thermocapillary effects can be dominant.

Microgravity Fluid ResearchSurface TensionSmallest Surface Area PossibleDominated on Earth by Gravity, which Makes Surfaces FlatLiquid BridgesALEX: A

Слайд 5Strong
Field
Weak
Field

StrongFieldWeak Field

Слайд 6Microgravity Test Facilities
Drop Towers
Evacuated tubes used to expose experiments to

several seconds of microgravity
Only short durations of microgravity are achieved

Microgravity Test FacilitiesDrop TowersEvacuated tubes used to expose experiments to several seconds of microgravityOnly short durations of

Слайд 7Test Facilities
NASA’s KC-135 “Vomit Comet”
Parabolic flight pattern can produce up

to 30 seconds of microgravity
Several periods of microgravity in one

flight
Test FacilitiesNASA’s KC-135 “Vomit Comet”Parabolic flight pattern can produce up to 30 seconds of microgravitySeveral periods of

Слайд 8Test Facilities
Sounding Rockets
Also flown in a parabolic flight path to

produce microgravity
Can provide 6-7 minutes of microgravity

Test FacilitiesSounding RocketsAlso flown in a parabolic flight path to produce microgravityCan provide 6-7 minutes of microgravity

Слайд 9Microgravity Simulation
Computational Fluid Dynamics (CFD) allows cost-effective microgravity simulation

Advances in

parallel supercomputing allow large problems to be solved

Microgravity SimulationComputational Fluid Dynamics (CFD) allows cost-effective microgravity simulationAdvances in parallel supercomputing allow large problems to be

Слайд 10Incompressible Navier-Stokes Equations:



Energy Equation:
Governing Equations

Incompressible Navier-Stokes Equations:Energy Equation:Governing Equations

Слайд 11MGFLO
Developed Under NASA-Grand Challenge Support
Parallel, Finite Element Formulation of Navier-Stokes

and Energy Equations
Allows for Coupled and Uncoupled Solution
Systems Optimized Through

Matlab Using Existing Algorithms

MGFLODeveloped Under NASA-Grand Challenge SupportParallel, Finite Element Formulation of Navier-Stokes and Energy EquationsAllows for Coupled and Uncoupled

Слайд 12Optimization Theory
Attempt to find “best value” of a merit function

within defined constraints
Gradient versus non-gradient methods
Gradient methods can be complex

and require several merit function evaluations
Non-gradient methods optimize based on a sample set of merit function values
Nelder-Mead Simplex Search Algorithm
Optimization TheoryAttempt to find “best value” of a merit function within defined constraintsGradient versus non-gradient methodsGradient methods

Слайд 13Nelder and Mead’s Method
Efficient search method for minimizing a merit

function of up to six variables
Optimization points are nodes of

a polygon
Optimal solution is determined by:
Reflection
Expansion
Contraction
Nelder and Mead’s MethodEfficient search method for minimizing a merit function of up to six variablesOptimization points

Слайд 14Simplex Steps
Reflection
Expansion
Contraction

Simplex StepsReflectionExpansionContraction

Слайд 15Previous Work
Investigated Operation of the MGFLO Code
Designed Simple Optimization Routine

in Matlab
Established Algorithms to Optimize Complex Fluid-Thermal Systems

Previous WorkInvestigated Operation of the MGFLO CodeDesigned Simple Optimization Routine in Matlab Established Algorithms to Optimize Complex

Слайд 16Code Overview
Developed Matlab Routines to Analyze MGFLO Output.
Matlab Can Compute

Quantities of Interest:
Vorticity, Divergence
Gradient, Laplacian
0th, 1st, 2nd Order

Derivatives Normal to Walls
Average Quantities in Large Datasets
Code OverviewDeveloped Matlab Routines to Analyze MGFLO Output.Matlab Can Compute Quantities of Interest:Vorticity, Divergence Gradient, Laplacian 0th,

Слайд 17Code Functions
Initializes the solution
Calls MGFLO for each simplex step
Checks that

user-specified constraints are satisfied
Calculates the user-specified merit function
Allows user to

monitor solution progression
Code FunctionsInitializes the solutionCalls MGFLO for each simplex stepChecks that user-specified constraints are satisfiedCalculates the user-specified merit

Слайд 19Debugging & Validation

Attempt to find answer to a known problem
Position

heat source on top surface to maximize heat flux out

of the bottom
Run on the 16-node Beowulf cluster in the CFDLab

Debugging & ValidationAttempt to find answer to a known problemPosition heat source on top surface to maximize

Слайд 22Optimization Path

Optimization Path

Слайд 23Limitations

Merit function dependence for pathological problems
Not successful at maximizing vorticity

in previous case
Non-smooth merit functions (too many local maxima)

LimitationsMerit function dependence for pathological problemsNot successful at maximizing vorticity in previous caseNon-smooth merit functions (too many

Слайд 24Applications
Solve more complicated problem whose answer is not known a-priori
System

exposed to external environment via Newton’s law of cooling (mixed

boundary condition)
Use particle tracing as a visualization technique
ApplicationsSolve more complicated problem whose answer is not known a-prioriSystem exposed to external environment via Newton’s law

Слайд 26Case 1: Tdesired=310K

Case 1: Tdesired=310K

Слайд 27Particle Tracing Algorithm
Heun predictor-corrector method
Second-order accurate in time




Allows visualization/quantification

of mixing

Particle Tracing AlgorithmHeun predictor-corrector methodSecond-order accurate in time Allows visualization/quantification of mixing

Слайд 30Convergence History

Convergence History

Слайд 31Case 2: Tdesired=340K

Case 2: Tdesired=340K

Слайд 34Convergence History

Convergence History

Слайд 35Conclusions
We became familiar with the CFDLab and the MGFLO code
Successfully

developed a method to optimize nonlinear fluid-thermal systems
Implemented a particle

tracing algorithm in Matlab to visualize fluid mixing
ConclusionsWe became familiar with the CFDLab and the MGFLO codeSuccessfully developed a method to optimize nonlinear fluid-thermal

Слайд 36Recommendations
Use particle tracing algorithm to optimize system mixing (currently takes

a long time!)
Implement feedback control for time-varying systems
Calculate merit function

interior to MGFLO
Faster
More accurate
Support unstructured grids

RecommendationsUse particle tracing algorithm to optimize system mixing (currently takes a long time!)Implement feedback control for time-varying

Слайд 37Questions?

Questions?

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