inter. conf. on numer. anal. & optim. theory and appl. king fahd university of petroleum and...
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Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
A Glimpse on
Optimal Control of Partial Differential Equations: Theory, Numerics, and Applications
Hans Josef Pesch
Chair of Mathematics in Engineering SciencesUniversity of Bayreuth, Bayreuth, Germany
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
multi-beam welding
weld seam
hot crack
main laser beam
mushy zone
weld pool
compression
additional beamssolidification
Motivation: Optimal placement of laser beams to avoid hot cracking
Semi-infinite optimization problemfor an elliptic PDE with state constraints
[Karkin, Ploshikin]
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Motivation: Optimal placement of laser beams to avoid hot cracking
op
enin
g d
isp
lace
men
t
weld pool region
hot crack criterium
limit
zoom
isotherms surroundingthe mushy zone
[Petzet]
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Motivation: Optimal load changes for fuel cell systems
Molten Carbonate Fuel Cell
cellstack
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Motivation: Optimal load changes for fuel cell systems
German Federal Pollution Control Act: Air
CO32-
O2
N2
½O2 + CO2 + 2e- CO32-
CH4 + H2O CO + 3H2
CO + H2O CO2 + H2H2 + CO3
2- H2O + CO2 + 2e-
CO + CO32- 2CO2 + 2e-
U
e-
Recirculation
Exhaust
CH4
H2O
Cathode
Anode
Elektrolyte
Mixer
Catalyticburner
Anode gas channel
Cathode gas channel
1D counter-flow design
Air inlet
only ions can movethrough electrolyte
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
catalyticburner
mixeranode
anode inlet
cathode inlet
anode exhaust
cathodeexhaust
exhaust air inletrecirculation
cathode
2D cross-flow design
CO32-
solid
Motivation: Optimal load changes for fuel cell systems
28 semi-linear partial integro-differential equations with non-standard non-linear boundary conditions
[Sundmacher][Heidebrecht]
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Motivation: Optimal placement of laser beams to avoid hot cracking
0 0.1 1.1 11.1 111.1 1111.1
using control
optimal controlsimulation
0.8 sec
0 0.1 1.1 11.1 111.1 1111.1scaled time
using controls
optimal controlsimulation
0.4 sec
scaled time
cell voltage 0.7 0.6for a load change
[Sternberg]
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Motivation: Minimum fuel transcontinental flights at hypersonic speeds
Europe - USA in 2 hrs / Europe - Australia in 4.5 hrs
ODE
PDE
2 box constraints1 control-state constraint1 state constraint
quasilinear heat equationnon-linear boundary conditionscoupled with ODE
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Motivation: Minimum fuel transcontinental flights at hypersonic speeds
velocity [m/s] altitude [10,000 m] flight path angle [deg]
temperature [K] temperature [K] temperature [K]
1st layer 2nd layer 3rd layer
limittemperature
1000 Kon a boundary arc
[s]
[s]
[Wächter, Chudej, LeBras]
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Outline
A glimpse on the theory
A glimpse on the numerics
An application
Conclusions
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Outline
A glimpse on the theory
A glimpse on the numerics
An application
Conclusions
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Elliptic optimal control problemwith distributed control
An example: optimal stationary temperature distribution
subject to
tracking functional Tikhonov regularizationset of admissible controls
A simple elliptic optimal control problems
Lions (since 1970s), Casas (1987-), Tröltzsch (1980-)
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
An example: optimal stationary temperature distribution
subject to
A simple elliptic optimal control problems
Elliptic optimal control problemwith boundary control
tracking functional Tikhonov regularizationset of admissible controls
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Necessary condition: variational inequality
with linear and continuous solution operatorsubject to
An example: Optimal stationary temperature distribution
Elliptic optimal control problemwith distributed control
Optimization problem in Hilbert space
Necessary conditions
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Necessary condition: variational inequalityDescripton with the adjoint solution operator
Optimization problem in Hilbert space
Necessary conditions
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Description with the adjoint solution operator
Description with the adjoint state
Necessary conditions
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Optimality system: semi-linear elliptic, distributed + boundary control
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Optimal Controlof PDE
FunctionalAnalysis
Partial DifferentialEquations
Optimization
in Banach spaces
Numerics ofPDE
Numerical Methods
of Optimization
High PerformanceScientific Computing
Numerical Methods of
Linear Algebra
ParallelNumerical Methods
Challenges in PDE constrained optimization
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Outline
A glimpse on the theory
A glimpse on the numerics
An application
Conclusions
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Methods for PDE constrained optimization
The general problem
The aims
concepts for real-life application
small constanteffort of simulation
effort of optimization
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
capture as much structure
of ( P )as possibleon discrete
level( Ph )
First Discretize then Optimize vs. First Optimize then Discretize
First discretize then optimze (fDtO)
First optimze then discretize (fOtD)
Questions
appropriate choice of and ansatz for ?
appropriate choice of and ansatz for ?
appropriate ansatz for adjoint variables and multipliers?
Solvelarge scale
NLP
Solvecoupled PDE
system
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
First Discretize then Optimize vs. First Optimize then Discretize
First discretize then optimze (fDtO):replace all quantities of the infinite dimensional optimization problemby finite dimensional substitutes and solve an NLP
First optimze then discretize (fOtD):Derive optimality conditions of the infinite dimensional system,discretize the optimality system and find solution of the discretizedoptimality system
In general
Ideal: discrete concept for which both approaches commuteDiscontinuous Galerkin methods
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Mathematical Toolbox (incomplete list)
• Structure of optimality system allows one-shot-iterations Griewank, Schulz• Constraints require non-smooth solution techniques Ito, Hintermüller, Kunisch, M. Ulbrich• Structure of optimality system allows multigrid methods Borzi, Schulz• Structure of optimality system allows taylored discrete concepts Hinze, Meyer, Rösch• Relaxation of constraints by penalty or barrier methods Hintermüller, Kunisch, Schiela• State constraints: set optimal control problem with shape calculus Frey, Bechmann, Pesch, Rund• Adaptive algorithms Becker, Rannacher; Vexler; Hintermüller, Hoppe; Hinze, Günther; et.al.• Surrogate models for the PDE system in the optimality system Hinze et.al., Sachs et.al., Kunisch, Tröltzsch, S. Ulbrich, Volkwein• Shape calculus for shape optimization Sokolowski, Zolesio; Gauger, Schulz; Hintermüller, Ring; M. Ulbrich, S. Ulbrich• Automatic differentiation provides adjoints Griewank, Walther
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Outline
A glimpse on the theory
A glimpse on the numerics
An application
optimal control of a molten carbonate fuel cell
process control via model reduction techniques
Conclusions
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
catalyticburner
mixeranode
solid
anode inlet
cathode inlet
anode exhaust
cathodeexhaust
exhaust air inletrecirculation
cathode
Configuration and function of MCFC
2D cross-flow design
controllable
controllable
controllable
load changesinput
boundary conditionsby ODAE
slow
statevariable
fastvery fastalgebraic
[Heidebrecht] [Sundmacher]
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
anode gas temperature cathode gas temperature
[2.8 ≈ 560 °C]
[3.2 ≈ 680 °C]
Numerical results: simulation of load change
reforming reactions are endothermicoxidation reaction is exothermic
reduction reaction is exothermic
flow directions
[Chudej, Sternberg]
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
[2.8 ≈ 560 °C]
[3.2 ≈ 680 °C]
solid temperature
Numerical results: simulation of load change
flow directionsin anode
and cathode
[Chudej, Sternberg]
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
[2.8 ≈ 560 °C]
[3.2 ≈ 680 °C]
solid temperature
Numerical results: simulation of load change
state constraint would be desirable
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
with
Pareto performance index:
Numerical results: optimal control of fast load changewhile temperature gradients stay small
fast
slow
on
on
0.7 0.6
instead of state constraint
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Aim for process control
How to apply optimal solutions in practise?
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
• measurable: cell voltage, gas temperatures and concentrations at anode and cathode outlet
• diserable for process control: information on spatial temperatur and concentration profiles
• solution ansatz: observer / state estimator
• Problem: complexity of model
Aim for process control
?
??Remedy: model reduction technique
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Model reduction by POD (proper orthogonal decomposition)or Karhunen-Loève decomposition (K.: 1946, L: 1955, Lumley: 1967,…)
• good accuracy for a wide range of operation conditions
• suitable for describing the nonlinear behavior of the cell
• ability for extrapolation in case of varying parameter
Demands on model reduction techniques
German Industrial Partners:CFC Solutions GmbH,
offspring of MTU, Munich;IPF Berndt KG, Reilingen,
constructor and operator of power plants
2002-2005
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Model reduction by POD: idea
Complete model:
Ansatz (separation of variables):
Reduced model:
orthogonalsnapshots
low order model: ODAE of index 1
Method of weighted residuals:
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
test signal
1. temperature basis function
Model reduction by POD: computation of snapshotsby the complete model
2. temperature basis function
orthogonalizationby singular value
decomposition
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Model reduction by POD: comparison of reduced vs. complete model
random variation of cell current
perfect coincidencewith reference model
appropriate forprocess control
[Mangold, Sheng]
#eqs. 4759 vs. 1313200 sec vs. 82 sec
2 < N < 10
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Model reduction by POD: comparison of reduced vs. complete model
example: response to changes
of the steam-to-carbon ratio in the feed
steam-to-carbon ratio temperature
complete
reduced
voltage
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Scheme for state estimator for discrete measurements
process
input
MCFCsensors
y
Simulator
state
sensor models
y
measurement
?
observer
observer correction+
-
MCFC model
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Temperature control at Hotmodule:nonlinear feed forward controller + PID controller
PID controller 1
PID controller 2
MCFCsystem
-
-
feed forward controller
[Sheng et al]
state estimator state estimator
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Temperature control at Hotmodule:nonlinear feed forward controller + PID controller
feed forward controller only feed forward controller +
PID controller
significantlybetter process
behaviour
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Focus on Theory:
Tröltzsch, F.: Optimal Control of Partial Differential Equations: Theory, Methods, and ApplicationsAMS, Graduate Studies in Mathematics, Vol. 112, 2010.
Focus on Methods:
Hinze, M., Pinnau, R., Ulbrich, M., Ulbrich, S.: Optimization with PDE ConstraintsMathematical Modelling: Theorie and Applications, Vol. 23, 2008.
Focus on Applications:
See my homepage: google: Hans Josef Pesch
References
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Conclusions
Concerning theory: already well developed
Concerning numerics: still improving
Concerning applications: has to be intensified
one always abuts against limits
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011
Thank you for your attention
Inter. Conf. On Numer. Anal. & Optim. Theory and Appl.King Fahd University of Petroleum and Minerals
Dhahran, Saudi Arabia, Dec. 17 – 21, 2011