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1 Optimization of Differential- Algebraic Equation Systems L. T. Biegler Chemical Engineering Department Carnegie Mellon University Pittsburgh, PA 2 I Introduction Process Examples II Parametric Optimization - Gradient Methods • Perturbation Direct - Sensitivity Equations • Adjoint Equations III Optimal Control Problems - Optimality Conditions - Model Algorithms Sequential Methods Multiple Shooting Indirect Methods IV Simultaneous Solution Strategies - Formulation and Properties - Process Case Studies - Software Demonstration DAE Optimization Outline
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Page 1: Optimization of Differential- Algebraic Equation Systemsnumero.cheme.cmu.edu/content/06720/Dynopt2.pdf · Optimization of Differential-Algebraic Equation Systems L. T. Biegler Chemical

1

Optimization of Differential-Algebraic Equation Systems

L. T. BieglerChemical Engineering Department

Carnegie Mellon UniversityPittsburgh, PA

2

I IntroductionProcess Examples

II ParametricOptimization- Gradient Methods

• Perturbation• Direct - Sensitivity Equations• Adjoint Equations

III Optimal ControlProblems- Optimality Conditions- Model Algorithms

• Sequential Methods• Multiple Shooting• Indirect Methods

IV SimultaneousSolutionStrategies- Formulation and Properties- Process Case Studies- Software Demonstration

DAE Optimization Outline

Page 2: Optimization of Differential- Algebraic Equation Systemsnumero.cheme.cmu.edu/content/06720/Dynopt2.pdf · Optimization of Differential-Algebraic Equation Systems L. T. Biegler Chemical

2

3

tf, final timeu, control variablesp, time independent parameters

t, timez, differential variablesy, algebraic variables

Dynamic Optimization Dynamic Optimization ProblemProblem

( )ftp,u(t),y(t),z(t), min Φ

( )pttutytzfdt

tdz,),(),(),(

)( =

( ) 0,),(),(),( =pttutytzg

ul

ul

ul

ul

o

ppp

utuu

ytyy

ztzz

zz

≤≤≤≤≤≤≤≤≤≤≤≤≤≤≤≤≤≤≤≤≤≤≤≤

≤≤≤≤≤≤≤≤====

)(

)(

)(

)0(

s.t.

4

DAE Models in Process Engineering

Differential Equations•Conservation Laws (Mass, Energy, Momentum)

Algebraic Equations•Constitutive Equations, Equilibrium (physical properties, hydraulics, rate laws)•Semi-explicit form•Assume to be index one (i.e., algebraic variables can be solved uniquely by algebraic equations)•If not, DAE can be reformulated to index one (see Ascher and Petzold)

Characteristics•Large-scale models – not easily scaled•Sparse but no regular structure•Direct linear solvers widely used•Coarse-grained decomposition of linear algebra

Page 3: Optimization of Differential- Algebraic Equation Systemsnumero.cheme.cmu.edu/content/06720/Dynopt2.pdf · Optimization of Differential-Algebraic Equation Systems L. T. Biegler Chemical

3

5

Catalytic Cracking of Gasoil (Tjoa, 1991)

number of states and ODEs: 2number of parameters:3no control profilesconstraints: pL ≤ p ≤ pU

Objective Function: Ordinary Least Squares

(p1, p2, p3)0 = (6, 4, 1)(p1, p2, p3)* = (11.95, 7.99, 2.02)(p1, p2, p3)true = (12, 8, 2)

1.00.80.60.40.20.00.0

0.2

0.4

0.6

0.8

1.0

YA_data

YQ_data

YA_estimate

YQ_estimate

t

Yi

Parameter Estimation

0)0( ,1)0(

)(

, ,

22

1

231

321

==−−=

+−=

→→→

qa

qpapq

appa

SASQQA ppp

&

&

6

Batch Distillation Multi-product Operating Policies

•Run between distillation batches•Treat as boundary value optimization problem

•When to switch from A to offcut to B?•How much offcut to recycle?•Reflux?•Boilup Rate?•Operating Time?

A B

Page 4: Optimization of Differential- Algebraic Equation Systemsnumero.cheme.cmu.edu/content/06720/Dynopt2.pdf · Optimization of Differential-Algebraic Equation Systems L. T. Biegler Chemical

4

7

Nonlinear Model Predictive Control (NMPC)

Process

NMPC Controller

d : disturbancesz : differential statesy : algebraic states

u : manipulatedvariables

ysp : set points

( )( )dpuyzG

dpuyzFz

,,,,0

,,,,

==′

NMPC Estimation and Control

sConstraintOther

sConstraint Bound

)()),(),(),((0

)),(),(),(()(..

||))||||)(||min

init

1sp

ztztttytzG

tttytzFtzts

yty uy Q

kk

Q

==

=′

−+−∑ ∑ −

u

u

u(tu(tu

NMPC Subproblem

Why NMPC?

n Track a profile

n Severe nonlinear dynamics (e.g, sign changes in gains)

n Operate process over wide range (e.g., startup and shutdown)

Model Updater( )

( )dpuyzG

dpuyzFz

,,,,0

,,,,

==′

8

Optimization of dynamic batch process operation resulting from reactor and distillation column

DAE models:z' = f(z, y, u, p)g(z, y, u, p) = 0

number of states and DAEs: nz + nyparameters for equipment design (reactor, column)nu control profiles for optimal operation

Constraints: uL ≤ u(t) ≤ uU zL ≤ z(t) ≤ zU

yL ≤ y(t) ≤ yU pL ≤ p ≤ pU

Objective Function: amortized economic function at end of cycle time tf

zi,I0 zi,II

0zi,III0 zi,IV

0

zi,IVf

zi,If zi,II

f zi,IIIf

Bi

A+B→C

C+B→P+E

P+C→G

5

10

15

20

25

580

590

600

610

620

630

640

0 0.5 1 1.5 2 2.50 0.25 0.5 0.75 1 1.25Time (h r.)

Dyn a m ic

C o nsta nt

Dyn a mic

C o nsta nt

optimal reactor temperature policy optimal column reflux ratio

Batch Process Optimization

Page 5: Optimization of Differential- Algebraic Equation Systemsnumero.cheme.cmu.edu/content/06720/Dynopt2.pdf · Optimization of Differential-Algebraic Equation Systems L. T. Biegler Chemical

5

9

FexitC H2 4

Texit ≤ 1180K

C2H CH

6 32→ • CH CH CH C H

3 2 6 4 2 5•+ → + •

C2H CH H

5 2 4•→ + •H CH H CH•+ → + •

2 6 2 2 52C

2H CH

5 4 10•→C

2H C H CH CH

5 2 4 3 6 3•+ → + •

H CH C H•+ → •2 4 2 5

0

1

2

3

4

5

6

0 2 4 6 8 10

Length m

Flo

w r

ate

mol

/s

0

500

1000

1500

2000

2500

Hea

t flu

x kJ

/m2s

C2H4 C2H6 log(H2)+12 q

Reactor Design ExamplePlug Flow Reactor Optimization

The cracking furnace is an important example in the olefin production industry, where various hydrocarbon feedstocks react. Consider a simplified model for ethane cracking (Chen et al., 1996). The objective is to find an optimal profile for the heat flux along the reactor in order to maximize the production of ethylene.

Max s.t. DAE

The reaction system includes six molecules, three free radicals, and seven reactions. The model also includes the heat balance and the pressure drop equation. This gives a total of eleven differential equations.

Concentration and Heat Addition Profile

10

Dynamic Optimization Approaches

DAE Optimization Problem

Sequential Approach

Vassiliadis(1994)Discretize controls

Variational Approach

Pontryagin(1962)

Inefficient for constrained problems

Apply a NLP solver

Efficient for constrained problems

Page 6: Optimization of Differential- Algebraic Equation Systemsnumero.cheme.cmu.edu/content/06720/Dynopt2.pdf · Optimization of Differential-Algebraic Equation Systems L. T. Biegler Chemical

6

11

Sequential Approaches - Parameter Optimization

Consider a simpler problem without control profiles:

e.g., equipment design with DAE models - reactors, absorbers, heat exchangers

Min Φ (z(tf))

z' = f(z, p), z (0) = z0

g(z(tf)) ≤ 0, h(z(tf)) = 0

By treating the ODE model as a "black-box" a sequential algorithm can be constructed that can be treated as a nonlinear program.

Task: How are gradients calculated for optimizer?

NLPSolver

ODEModel

GradientCalculation

P

φ,g,h

z (t)

12

Gradient Calculation

Perturbation

Sensitivity Equations

Adjoint Equations

Perturbation

Calculate approximate gradient by solving ODE model (np + 1) times

Let ψ = Φ, g and h (at t = tf)

dψ/dpi = {ψ (pi + ∆pi) - ψ (pi)}/ ∆pi

Very simple to set up

Leads to poor performance of optimizer and poor detection of optimum unless roundoff error (O(1/∆pi) and truncation error (O(∆pi)) are small.

Work is proportional to np (expensive)

Page 7: Optimization of Differential- Algebraic Equation Systemsnumero.cheme.cmu.edu/content/06720/Dynopt2.pdf · Optimization of Differential-Algebraic Equation Systems L. T. Biegler Chemical

7

13

Direct Sensitivity

From ODE model:

(nz x np sensitivity equations)

• z and si , i = 1,…np, an be integrated forward simultaneously.

• for implicit ODE solvers, si(t) can be carried forward in time after converging on z

• linear sensitivity equations exploited in ODESSA, DASSAC, DASPK, DSL48s and a number of other DAE solvers

Sensitivity equations are efficient for problems with many more constraints than parameters (1 + ng + nh > np)

{ }

iii

T

iii

ii

p

zss

z

f

p

fs

dt

ds

ip

tzts

pzztpzfzp

∂∂=

∂∂+

∂∂==′

=∂

∂=

==′∂∂

)0()0( ,)(

...np 1, )(

)( define

)()0(),,,( 0

14

Example: Sensitivity Equations

0)0(,0

22

1)0(,0

22

2,1,/)()(,/)()(

)0(,5

2,1,

1,1,22,112,

2,21,11,

2,1,

1,1,22,12,

2,21,11,

,,

21

1212

22

211

==

+++=′

+=′

==

++=′

+=′

=∂∂=∂∂===

+=′+=′

bb

bbbbb

bbb

aa

baaaa

aaa

bjjbajja

a

b

ss

psszszzs

szszs

ss

psszszs

szszs

jptztsptzts

pzz

pzzzz

zzz

Page 8: Optimization of Differential- Algebraic Equation Systemsnumero.cheme.cmu.edu/content/06720/Dynopt2.pdf · Optimization of Differential-Algebraic Equation Systems L. T. Biegler Chemical

8

15

Adjoint Sensitivity

Adjoint or Dual approach to sensitivity

Adjoin model to objective function orconstraint

(ψ = Φ,g or h)

(λ(t)) serve as multipliers on ODE's)

Now, integrate by parts

Take variations and find dψ/dp subject to feasibility of ODE's

Now, set all terms notin dp to zero.

∫ −′−=ft

Tf dttpzfzt

0

)),,(()( λψψ

∫ +′+−+=ft

TTf

Tf

Tf dttpzfztztpzt

0

0 )),,(()()()()0()( λλλλψψ

00

∂∂+

∂∂+′+

∂∂+

∂∂

=ft TTT

fff

f dtdpp

ftz

z

fdp

p

pztzt

tz

tzd

0

0 )()0()(

)()()(

))((λδλλλδλ

ψψ

16

Adjoint System

Integrate model equations forward

Integrate adjoint equations backward and evaluate integral and sensitivities.

Notes:

nz (ng + nh + 1) adjoint equations must be solved backward (one for each objective and constraint function)

for implicit ODE solvers, profiles (and even matrices) can be stored and carried backward after solving forward for z as in DASPK/Adjoint (Li and Petzold) and CVODES (Serban and Hindmarsh)

more efficient on problems where: np > 1 + ng + nh

∂∂+

∂∂=

∂∂

=∂∂−=′

ft

f

ff

dttp

f

p

pz

dp

d

tz

tztt

z

f

0

0 )()0()(

)(

))(()( ),(

λλψ

ψλλλ

Page 9: Optimization of Differential- Algebraic Equation Systemsnumero.cheme.cmu.edu/content/06720/Dynopt2.pdf · Optimization of Differential-Algebraic Equation Systems L. T. Biegler Chemical

9

17

Example: Adjoint Equations

dttztdp

td

dp

td

tz

ttzz

tz

ttpzz

dttp

f

p

pz

dp

d

tz

tztt

z

f

pzzzzztpzf

pzz

pzzzz

zzz

f

f

t

b

f

a

f

f

ff

f

ffb

t

f

ff

bT

a

b

)()()(

)0()(

)(

)()( ,2

)(

)()( ),(2

:becomesthen

)()0()(

)(

))(()( ),(

)()(),,( Form

)0(,5

1

0

2

2

2212212

1122111

0

0

121222

211

21

1211

22

211

=

=

∂∂

=−−=′

∂∂

=+−−=′

∂∂+

∂∂=

∂∂

=∂∂−=′

+++=

==

+=′+=′

λψ

λψ

ψλλλλ

ψλλλλ

λλψ

ψλλλ

λλλ

18

A + 3B --> C + 3D

L

Ts

TR

TP

3:1 B/A 383 K

TP = specified product temperatureTR = reactor inlet, reference temperatureL = reactor lengthTs = steam sink temperatureq(t) = reactor conversion profileT(t) = normalized reactor temperature profile

Cases considered:• Hot Spot - no state variable constraints• Hot Spot with T(t) ≤ 1.45

Example: Hot Spot Reactor

Roo

P

Pproducto

Rfeed

RS

L

RSTLTT

C/T C, T(L) T

, T(L)) (THC) -,(T∆H

Tdt

dqTTtT

dt

dT

qtTtqdt

dqts

dtTTtTLMinSRP

101120

0110

1)0( ,3/2)/)((5.1

0)0( )],(/2020exp[))(1(3.0 ..

)/)(( 0

,,,

+==

=∆

=+−−=

=−−=

−−=Φ ∫

Page 10: Optimization of Differential- Algebraic Equation Systemsnumero.cheme.cmu.edu/content/06720/Dynopt2.pdf · Optimization of Differential-Algebraic Equation Systems L. T. Biegler Chemical

10

19

1.51.00.50.0

0.0

0.2

0.4

0.6

0.8

1.0

1.2

Normalized Length

Con

vers

ion,

q

1.51.00.50.0

1.0

1.1

1.2

1.3

1.4

1.5

1.6

Normalized LengthN

orm

aliz

ed T

empe

ratu

re

Method: SQP (perturbation derivatives)

L(norm) TR(K) TS(K) TP(K)Initial: 1.0 462.23 425.26 250Optimal: 1.25 500 470.1 188.413 SQP iterations / 2.67 CPU min. (µVax II)

Constrained Temperature Case (T ≤ 1.45): could not be solved with sequential method

Hot Spot Reactor: Unconstrained Case

20

Variable Final Time(Miele, 1980)

Define t = pn+1 τ, 0 ≤ τ ≤ 1, pn+1 = tf

Let dz/dt = (1/ pn+1) dz/dτ = f(z, p) ⇒ dz/dτ = (pn+1) f(z, p)

Converting Path Constraints to Final Time

Define measure of infeasibility as a new variable, znz+1(t) (Sargent & Sullivan, 1977):

Tricks to generalize classes of problems

)degenerate is constraint (however, )( Enforce

0)0( , ))(),((,0max()(

))(),((,0max()(

1

12

1

0

21

ε≤

==

=

+

++

+

∑∫

fnz

nzj

jnz

j

t

jfnz

tz

ztutzgtzor

dttutzgtzf

&

Page 11: Optimization of Differential- Algebraic Equation Systemsnumero.cheme.cmu.edu/content/06720/Dynopt2.pdf · Optimization of Differential-Algebraic Equation Systems L. T. Biegler Chemical

11

21

Profile Optimization - (Optimal Control)

Optimal Feed Strategy (Schedule) in Batch Reactor

Optimal Startup and Shutdown Policy

Optimal Control of Transients and Upsets

Sequential Approach: Approximate control profile as through parameters (piecewise constant, linear, polynomial, etc.)

Apply NLP to discretization as with parametric optimization

Obtain gradients through adjoints (Hasdorff; Sargentand Sullivan; Goh and Teo) or sensitivity equations (Vassiliadis, Pantelides and Sargent; Gill, Petzold et al.)

Variational (Indirect) approach: Apply optimality conditions and solve as boundary value problem

22

Optimality Conditions(Bound constraints on u(t))

Min φ(z(tf))s.t. dz/dt= f(z, u), z (0) = z0

g (z(tf)) ≤ 0h (z(tf)) = 0a ≤ u(t) ≤ b

Form Lagrange function - adjoin objective function and constraints:

Derivation of Variational Conditions Indirect Approach

dt)b)t(u())t(ua()u,z(fz

)t(z)t()(z)(v))t(z(h))t(z(g)t(

dt)b)t(u())t(ua()z)u,z(f(

v))t(z(h))t(z(g)t(

Tb

tTa

TT

ffTTT

fT

ff

Tb

tTa

T

Tf

Tff

f

f

00

:partsby Integrate

0

0

−+−+++

−+++=

−+−+−+

++=

ααλλ

λλµφφ

ααλ

µφφ

&

&

Page 12: Optimization of Differential- Algebraic Equation Systemsnumero.cheme.cmu.edu/content/06720/Dynopt2.pdf · Optimization of Differential-Algebraic Equation Systems L. T. Biegler Chemical

12

23

λ ft( )=∂φ∂z

+∂g

∂zµ +

∂h

∂zγ

ft =t

∂f

∂uλ =

∂H

∂u= 0

∂ H

∂u= α a − α b

α aT (a − u(t))

αbT (u(t) − b)

ua ≤ u(t) ≤ ub

α a ≥ 0,α b ≥ 0

∂H

∂u= −α b ≤ 0

∂H

∂u= αa ≥ 0

At optimum, δφ ≥ 0. Since u is the control variable, let all other terms vanish.⇒ δz(tf):

δz(0): λ(0) = 0 (if z(0) is not specified)δz(t):

Define Hamiltonian, H = λTf(z,u)For u notat bound:

For u atbounds:

Upper bound, u(t) = b, Lower bound, u(t) = a,

Derivation of Variational Conditions

λλz

f

z

H

∂∂−=

∂∂−=&

0 )(),(

)(),(

)0()0()(

0≥

−+∂

∂+

∂∂++

+

−∂∂+

∂∂+

∂∂=

∫ dttuu

uzftz

z

uzf

ztzvz

h

z

g

z

ftT

ab

T

Tf

T

δααλδλλ

δλδλµφδφ

&

24

Car ProblemTravel a fixed distance (rest-to-rest) in minimum time.

0)(',0)0('

)(,0)0(

)(

" ..

==

==≤≤

=

f

f

f

txx

Ltxx

btua

uxts

tMin

0)(,0)0(

)(,0)0(

)(

1'

'

' ..

22

11

3

2

21

3

==

==≤≤

===

f

f

f

txx

Ltxx

btua

x

ux

xxts

)(tMin x

s

f

ff

f

f

tt

auctt

buctctttcc

u

H

tt

ttcct

ct

uxH

==

=>==<+=

−+==∂∂

====>=

−+===>−=

===>=

++=

at occurs )0(Crossover

,0,

,0,0)(

1)( ,1)(0

)()(

)(0 :Adjoints

:n Hamiltonia

2

2

21122

333

12212

111

3221

λ

λ

λλλ

λλλλλ

λλλ

&

&

&

Page 13: Optimization of Differential- Algebraic Equation Systemsnumero.cheme.cmu.edu/content/06720/Dynopt2.pdf · Optimization of Differential-Algebraic Equation Systems L. T. Biegler Chemical

13

25

t f

u(t)

b

a

t s

1 / 2 bt2, t < ts

1 / 2 bts2 - a ts - t f( )2( ), t ≥ ts

bt, t < ts

bts + a t - ts( ), t ≥ ts

2L

b 1- b / a( )

1/2

(1− b / a)2L

b 1 - b / a( )

1/2

Optimal Profile

From state equations:

x1(t) =

x2 (t) =

Apply boundary conditions at t = tf:x1(tf) = 1/2 (b ts

2 - a (ts - tf)2) = Lx2(tf) = bts + a (tf - ts) = 0⇒ ts =

tf =

•Problem is linear in u(t). Frequently these problems have "bang-bang" character.•For nonlinear and larger problems, the variational conditions can be solved numerically as boundary value problems.

Car ProblemAnalytic Variational Solution

26

A B

C

u

u /22

u(T(t))

Example: Batch reactor - temperature profile

Maximize yield of B after one hour's operation by manipulating a transformed temperature, u(t).

Optimality conditions:

Cases Considered1. NLP Approach- piecewise constant and linear profiles.2. Indirect Approach

50

00

10 2

1 2

≤≤==

=+−=

)t(u

)(b,ua'b

)(a,a)/uu('a.t.s

)(bMin

10 0

00 2

050 00

1

2

2

50

50

2

−===−+=

≥−⊥≤≥⊥≤−=++−=∂∂

++−=

)(,'

)(,u)/uu('

)u(,u

aa)u(u/H

uaa)/uu(H

bb

abaa

ba

ba

λλλλλλ

ααααλλ

λλ

Page 14: Optimization of Differential- Algebraic Equation Systemsnumero.cheme.cmu.edu/content/06720/Dynopt2.pdf · Optimization of Differential-Algebraic Equation Systems L. T. Biegler Chemical

14

27

Batch Reactor Optimal Temperature Program Piecewise Constant

Opt

imal

Pro

file,

u(t

)

0. 0.2 0.4 0.6 0.8 1.0

2

4

6

Time, h

ResultsPiecewise Constant Approximation with Variable Time ElementsOptimum B/A: 0.57105

28

Opt

imal

Pro

file,

u(t

)

0. 0.2 0.4 0.6 0.8 1.0

2

4

6

Time, h

Results:Piecewise Linear Approximation with Variable Time ElementsOptimum B/A: 0.5726Equivalent # of ODE solutions: 32

Batch Reactor Optimal Temperature Program Piecewise Linear

Page 15: Optimization of Differential- Algebraic Equation Systemsnumero.cheme.cmu.edu/content/06720/Dynopt2.pdf · Optimization of Differential-Algebraic Equation Systems L. T. Biegler Chemical

15

29

Opt

imal

Pro

file,

u(t

)

0. 0.2 0.4 0.6 0.8 1.0

2

4

6

Time, h

Results:Control Vector Iteration with Conjugate GradientsOptimum (B/A): 0.5732Equivalent # of ODE solutions: 58

Batch Reactor Optimal Temperature Program

Indirect Approach

30

Dynamic Optimization - Sequential Strategies

Small NLP problem, O(np+nu) (large-scale NLP solver not required) • Use NPSOL, NLPQL, etc. • Second derivatives difficult to get

Repeated solution of DAE model and sensitivity/adjoint equations, scales with nz and np

• Dominant computational cost• May fail at intermediate points

Sequential optimization is not recommended for unstable systems. State variables blow up at intermediate iterations for control variables and parameters.

Discretize control profiles to parameters (at what level?)

Path constraints are difficult to handle exactly for NLP approach

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16

31

Instabilities in DAE ModelsThis example cannot be solved with sequential methods (Bock, 1983):

dy1/dt = y2

dy2/dt = τ2 y1 + (π2 − τ2) sin (π t)

The characteristic solution to these equations is given by:

y1(t) = sin (π t) + c1 exp(-τ t) + c2 exp(τ t)

y2 (t) = π cos (π t) - c1 τ exp(-τ t) + c2 τ exp(τ t)

Both c1 and c2 can be set to zero by either of the following equivalent conditions:

IVP y1(0) = 0, y2 (0) = π

BVP y1(0) = 0, y1(1) = 0

32

IVP SolutionIf we now add roundoff errors e1 and e2 to the IVP and BVP conditions, we see significant differences in the sensitivities of the solutions.

For the IVP case, the sensitivity to the analytic solution profile is seen by large changes in the profiles y1(t) and y2(t) given by:

y1(t) = sin (π t) + (e1 - e2/τ) exp(-τ t)/2

+(e1 + e2/τ) exp(τ t)/2

y2 (t) = π cos (π t) - (τ e1 - e2) exp(-τ t)/2

+ (τ e1 + e2) exp(τ t)/2

Therefore, even if e1 and e2 are at the level of machine precision (< 10-13), a large value of τ and t will lead to unbounded solution profiles.

Page 17: Optimization of Differential- Algebraic Equation Systemsnumero.cheme.cmu.edu/content/06720/Dynopt2.pdf · Optimization of Differential-Algebraic Equation Systems L. T. Biegler Chemical

17

33

BVP Solution

On the other hand, for the boundary value problem, the errors affect the analyticsolution profiles in the following way:

y1(t) = sin (π t) + [e1 exp(τ)- e2] exp(-τ t)/[exp(τ) - exp(-τ)]

+ [e1 exp(-τ) - e2] exp(τ t)/[exp(τ) - exp(-τ)]

y2(t) = π cos (π t) – τ [e1 exp(τ)- e2] exp(-τ t)/[exp(τ) - exp(-τ)]

+ τ [e1 exp(-τ) - e2] exp(τ t)/[exp(τ) - exp(-τ)]

Errors in these profiles never exceed τ (e1 + e2), and as a result a solution to the BVP is readily obtained.

34

BVP and IVP Profiles

e1, e2 = 10-9

Linear BVP solves easily

IVP blows up before midpoint

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35

Dynamic Optimization Dynamic Optimization ApproachesApproaches

DAE Optimization Problem

Multiple Shooting

Sequential Approach

Vassiliadis(1994)

Can not handle instabilities properlySmall NLP

Handles instabilities Larger NLP

Discretize some state variables

Discretize controls

Variational Approach

Pontryagin(1962)

Inefficient for constrained problems

Apply a NLP solver

Efficient for constrained problems

36

Multiple Shooting for Dynamic Optimization

Divide time domain into separate regions

Integrate DAEs state equations over each region

Evaluate sensitivities in each region as in sequential approach wrt uij, p and zj

Impose matching constraints in NLP for state variables over each region

Variables in NLP are due to control profiles as well as initial conditions in each region

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37

Multiple ShootingNonlinear Programming Problem

uL

x

xxx

xc

xfn

≤≤

=

ℜ∈

0)(s.t

)(min

( ))(),( min,,

ffpu

tytzji

ψ

( ) z)z(tpuyzfdt

dzjjji ==

,,,, ,

( ) 0,ji, =pz,y,ug

ul

uiji

li

ukkjij

lk

ukkjij

lk

jjjij

ppp

uuu

ytpuzyy

ztpuzzz

ztpuzz

≤≤

≤≤

≤≤

≤≤

=− ++

,

,

,

11,

),,,(

),,,(

0),,,(s.t.

(0)0 zz o = Solved Implicitly

38

BVP Problem Decomposition

Consider: Jacobian of Constraint Matrix for NLP

• bound unstable modes with boundary conditions (dichotomy)

• can be done implicitly by determining stable pivot sequences in multiple shooting constraints approach

• well-conditioned problem implies dichotomy in BVP problem (deHoog and Mattheij)

Bock Problem (with τ = 50)

• Sequential approach blows up (starting within 10-9 of optimum)

• Multiple Shooting optimization requires 4 SQP iterations

B1 A1

A2

A3

A4

AN

B2

B3

B4

BN

IC

FC

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39

Dynamic Optimization – Multiple Shooting Strategies

Larger NLP problem O(np+NE (nu+nz)) • Use SNOPT, MINOS, etc.• Second derivatives difficult to get

Repeated solution of DAE model and sensitivity/adjoint equations, scales with nzand np

• Dominant computational cost• May fail at intermediate points

Multiple shooting can deal with unstable systems with sufficient time elements.

Discretize control profiles to parameters (at what level?)

Path constraints are difficult to handle exactly for NLP approach

Block elements for each element are dense!

Extensive developments and applications by Bock and coworkers using MUSCOD code

40

Dynamic Optimization Dynamic Optimization ApproachesApproaches

DAE Optimization Problem

Simultaneous Approach

Sequential Approach

Vassiliadis(1994)

Can not handle instabilities properlySmall NLP

Handles instabilities Large NLP

Discretize all state variables

Discretize controls

Variational Approach

Pontryagin(1962)

Inefficient for constrained problems

Apply a NLP solver

Efficient for constrained problems

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41

Nonlinear DynamicOptimization Problem

Collocation onfinite Elements

Continuous variablesContinuous variables

Nonlinear ProgrammingProblem (NLP)Discretized variablesDiscretized variables

Nonlinear Programming Formulation

42

Discretization of Differential Equations Orthogonal Collocation

Given:dz/dt = f(z, u, p), z(0)=given

Approximate zand u by Lagrange interpolation polynomials (order K+1 and K, respectively) with interpolation points, tk

kkKjk

jK

kjj

k

K

kkkK

kkKjk

jK

kjj

k

K

kkkK

ututt

ttttutu

ztztt

ttttztz

===>−−

∏==

===>−−

∏==

≠==

+

≠==

+

)()(

)()(,)()(

)()(

)()(,)()(

11

100

1

ll

ll

Substitute zN+1 and uN into ODE and apply equations at tk.

Kkuzftztr kk

K

jkjjk ,...1 ,0),()()(

0

==−=∑=

l&

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43

Collocation Example

kkNjk

jK

kjj

k

K

kkkK ztz

tt

ttttztz ===>

−−

∏== +

≠==

+ ∑ )()(

)()(,)()( 1

001 ll

2

210

22

221

22

2222211200

12

121

12

1122111100

0

2

22

2

12

1

02

0

210

76303053371

706073840319029100

2334786

23

2346412098572

23

0

0023

464103924 46410196252

391644836 448361958

612 166

7886802113200

t. t - . z(t)

). (. ), z. (. , z z

) z - z z z.(-

z - z) (t z) (t z) (tz

) z - z z. z.(

z - z) (t z) (t z) (tz

z

) , z( z - z z' Solve

.t - . (t) ,t. - t. (t)

t. - . (t) ,t. t. -(t)

t - (t) ,t - t (t)

. , t. , t t

=

===+=+

+=++

+=+

+=++

===>=+=

==

=+=

=+=

===

l&l&l&

l&l&l&

l&l

l&l

l&l

44

z(t)

zN+1 (t)

Sta

te P

rofil

e

t ft 1 t 2 t 3

r(t)

t 1 t 2 t 3

Min φ(z(tf))s.t. z' = f(z, u, p), z(0)=z0

g(z(t), u(t), p) ≤ 0h(z(t), u(t), p) = 0

to Nonlinear Program

How accurate is approximation

Converted Optimal Control Problem

Using Collocation

0)1(

,...1

0

0

z(0) ,0),()(

0

00

=−

=

=≤

==−

=

=

f

K

jjj

kk

kk

kk

K

jkjj

f

zz

Kk

),uh(z

),ug(z

zuzftz

)(z Min

l

l&

φ

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45

Results of Optimal Temperature Program Batch Reactor (Revisited)

Results- NLP with Orthogonal CollocationOptimum B/A - 0.5728# of ODE Solutions - 0.7(Equivalent)

46

to tf

×××× ×××× ×××× ××××

Collocation points

• ••• •

•• •

•••

Polynomials

×××× ×××××××× ××××

Finite element, i

ti

Mesh points

hi

×××× ×××× ×××× ××××

∑=

=K

qiqq(t) zz(t)

0

l

×××× ××××××××

××××element i

q = 1q = 1

q = 2 q = 2

××××××××××××××××Continuous Differential variables

Discontinuous Algebraic and Control variables

××××

××××

×××× ××××

Collocation on Finite ElementsCollocation on Finite Elements

∑=

=K

qiqq(t) yy(t)

1

l ∑=

=K

qiqq(t) uu(t)

1

l

τd

dz

hdt

dz

i

1=

),( uzfhd

dzi=

τ

NE 1,.. i 1,..K,k ,0),,())(()(0

===−=∑=

K

jikikikjijik puzfhztr τl&

]1,0[,1

1'' ∈+=∑

=

ττ ji

i

iiij hht

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47

Nonlinear Programming ProblemNonlinear Programming Problem

uL

x

xxx

xc

xfn

≤≤

=

ℜ∈

0)(s.t

)(min( )fzψ min

( ) 0,, ,,, =p,uyzg kikiki

ul

ujiji

lji

uji

lji

ul

ppp

uuu

yyy

zzz

≤≤

≤≤

≤≤

≤≤

,,,

,ji,,

ji, ji,ji,

s.t. ∑=

=−K

jikikikjij puzfhz

0

0),,())(( τl&

)0( ,0))1((

,..2 ,0))1((

100

,

00,1

zzzz

NEizz

K

jfjjNE

K

jijji

==−

==−

=

=−

l

l

Finite elements,hi, can also be variable to determine break points for u(t).

Add hu ≥ hi ≥ 0, Σ hi=t f

Can add constraints g(h, z, u) ≤ ε for approximation error

48

A + 3B --> C + 3D

L

Ts

TR

TP

3:1 B/A 383 K

TP = specified product temperatureTR = reactor inlet, reference temperatureL = reactor lengthTs = steam sink temperatureq(t) = reactor conversion profileT(t) = normalized reactor temperature profile

Cases considered:• Hot Spot - no state variable constraints• Hot Spot with T(t) ≤ 1.45

Hot Spot Reactor Revisited

Roo

P

Pproducto

Rfeed

RS

L

RSTLTT

C/T C, T(L) T

, T(L)) (THC) -,(T∆H

Tdt

dqTTtT

dt

dT

qtTtqdt

dqts

dtTTtTLMinSRP

101120

0110

1)0( ,3/2)/)((5.1

0)0( )],(/2020exp[))(1(3.0 ..

)/)(( 0

,,,

+==

=∆

=+−−=

=−−=

−−=Φ ∫

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49

1.21.00.80.60.40.20.00

1

2

integrated profile

collocation

Normalized Length

Con

vers

ion

1.21.00.80.60.40.20.01.0

1.2

1.4

1.6

1.8

integrated profile

collocation

Normalized LengthT

empe

ratu

re

Base Case SimulationMethod: OCFE at initial point with 6 equally spaced elements

L(norm) TR(K) TS(K) TP(K)Base Case: 1.0 462.23 425.26 250

50

1.51.00.50.0

0.0

0.2

0.4

0.6

0.8

1.0

1.2

Normalized Length

Con

vers

ion,

q

1.51.00.50.01.0

1.1

1.2

1.3

1.4

1.5

1.6

Normalized Length

Nor

mal

ized

Tem

pera

ture

Unconstrained CaseMethod: OCFE combined formulation with rSQP

identical to integrated profiles at optimum L(norm) TR(K) TS(K) TP(K)

Initial: 1.0 462.23 425.26 250Optimal: 1.25 500 470.1 188.4

123 CPU s. (µVax II)φ∗ = -171.5

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51

1.51.00.50.0

0.0

0.2

0.4

0.6

0.8

1.0

1.2

Normalized Length

Con

vers

ion

1.51.00.50.01.0

1.1

1.2

1.3

1.4

1.5

Normalized Length

Tem

pera

ture

Temperature Constrained CaseT(t) ≤ 1.45

Method: OCFE combined formulation with rSQP, identical to integrated profiles at optimum

L(norm) TR(K) TS(K) TP(K)Initial: 1.0 462.23 425.26 250Optimal: 1.25 500 450.5 232.1

57 CPU s. (µVax II), φ∗ = -148.5

52

Theoretical Properties of Simultaneous Method

A. Stability and Accuracy of Orthogonal Collocation

• Equivalent to performing a fully implicit Runge-Kutta integration of the DAE models at Gaussian (Radau) points

• 2K order (2K-1) method which uses K collocation points• Algebraically stable (i.e., possesses A, B, AN and BN stability)

B. Analysis of the Optimality Conditions

• An equivalence has been established between the Kuhn-Tucker conditions of NLP and the variational necessary conditions

• Rates of convergence have been established for the NLP method

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53

Dynamic Optimization Engines

Evolution of NLP Solvers:

� for dynamic optimization, control and estimation

E.g., NPSOL and Sequential Dynamic Optimization - over 100 variables and constraints E.g, SNOPT and Multiple Shooting - over 100 d.f.s but over 105 variables and constraintsE.g., IPOPT - Simultaneous dynamic optimizationover 1 000 000 variables and constraints

SQP rSQP Full-spaceBarrier

Object Oriented Codes tailored to structure, sparse linearalgebra and computer architecture (e.g., IPOPT 3.2)

54

Hierarchy of Nonlinear Programming for Dynamic Optimization Formulations

Variables/Constraints102 104 106

Black Box

Direct Sensitivities

Single Shooting

Multiple Shooting

Adjoint Sensitivity

Simultaneous Full Space Formulation

100

SQPSQP

rSQPrSQP

Interior PointInterior Point

DFODFO

Com

putational Efficiency

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55

Comparison of Computational Complexity(α ∈ [2, 3], β ∈ [1, 2], nw, nu - assume Nm = O(N))

((nu + nw)N)------Backsolve

((nu + nw)N)β(nu N)α(nu N)αStep Determination

---nw3 N---NLP Decomposition

N (nu + nw)(nw N) (nu + nw)2(nw N) (nu N)2Exact Hessian

N (nu + nw)(nw N) (nu + nw)(nw N) (nu N)Sensitivity

---nwβ Nnw

β NDAE Integration

SimultaneousMultiple Shooting

Single Shooting

O((nuN)α + N2nwnu

+ N3nwnu2)

O((nuN)α + N nw3

+ N nw (nw +nu)2)

O((nu + nw)N)β

56

Case Studies• Reactor - Based Flowsheets• Fed-Batch Penicillin Fermenter• Temperature Profiles for Batch Reactors• Parameter Estimation of Batch Data• Synthesis of Reactor Networks• Batch Crystallization Temperature Profiles• Grade Transition for LDPE Process• Ramping for Continuous Columns• Reflux Profiles for Batch Distillation and Column Design• Source Detection for Municipal Water Networks• Air Traffic Conflict Resolution• Satellite Trajectories in Astronautics• Batch Process Integration• Optimization of Simulated Moving Beds

Simultaneous DAE Optimization

Page 29: Optimization of Differential- Algebraic Equation Systemsnumero.cheme.cmu.edu/content/06720/Dynopt2.pdf · Optimization of Differential-Algebraic Equation Systems L. T. Biegler Chemical

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57

Production of High Impact Polystyrene (HIPS)Startup and Transition Policies (Flores et al., 2005a)

Catalyst

Monomer, Transfer/Term. agents

Coolant

Polymer

58

Upper Steady−State

Bifurcation Parameter

System State

Lower Steady−State

Medium Steady−State

Phase Diagram of Steady States

Transitions considered among all steady state pairs

0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5

300

350

400

450

500

550

600

N1

N2

N3

A1

A4

A2

A3

A5

Cooling water flowrate (L/s)

Te

mp

era

ture

(K

)

1: Qi = 0.00152: Qi = 0.00253: Qi = 0.0040

3

2

1

0 0.02 0.04 0.06 0.08 0.1 0.12

300

350

400

450

500

550

600

650

Initiator flowrate (L/s)

Te

mp

era

ture

(K

)

1: Qcw = 102: Qcw = 1.03: Qcw = 0.1

32 1

3

2

1

N2

B1 B2 B3

C1C2

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59

0 0.5 1 1.5 20

0.5

1x 10

−3

Time [h]

Initi

ator

Con

c. [m

ol/l]

0 0.5 1 1.5 24

6

8

10

Time [h]

Mon

omer

Con

c. [m

ol/l]

0 0.5 1 1.5 2300

350

400

Time [h]

Rea

ctor

Tem

p. [

K]

0 0.5 1 1.5 2290

300

310

320

Time [h]

Jack

et T

emp.

[K

]0 20 40 60 80 100

0

0.5

1

1.5x 10

−3

Time [h]

Initi

ator

Flo

w. [

l/sec

]

0 0.5 1 1.5 20

0.5

1

Time [h]Coo

ling

wat

er F

low

. [l/s

ec]

0 0.5 1 1.5 20

1

2

3

Time [h]

Fee

drat

e F

low

. [l/s

ec]

• 926 variables• 476 constraints• 36 iters. / 0.95 CPU s (P4)

Startup to Unstable Steady State

60

HIPS Process Plant (Flores et al., 2005b)

•Many grade transitions considered with stable/unstable pairs

•1-6 CPU min (P4) with IPOPT

•Study shows benefit for sequence of grade changes to achieve wide range of grade transitions.

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61

Cyclic Steady StateStep

Liquid Flow

FeedDesorbent

Extract Raffinate

1

Liquid Flow

FeedDesorbent

Extract Raffinate

2

Liquid Flow

FeedDesorbent

Extract Raffinate

3

Liquid Flow

FeedDesorbent

Extract Raffinate

4

Liquid Flow

FeedDesorbent

Extract Raffinate

5

Liquid Flow

FeedDesorbent

Extract Raffinate

6

Liquid Flow

FeedDesorbent

ExtractRaffinate

7

Liquid Flow

FeedDesorbent

ExtractRaffinate

8

Liquid Flow

FeedDesorbent

ExtractRaffinate

9

Liquid Flow

FeedDesorbent

ExtractRaffinate

10

Liquid Flow

Feed Desorbent

ExtractRaffinate

11

Liquid Flow

Feed Desorbent

ExtractRaffinate

12

Liquid Flow

Feed Desorbent

ExtractRaffinate

13

Liquid Flow

Feed Desorbent

ExtractRaffinate

14

Liquid Flow

Feed Desorbent

Extract Raffinate

15

Liquid Flow

Feed Desorbent

Extract Raffinate

16

Liquid Flow

FeedDesorbent

Extract Raffinate

17

SMB Applications

• Petrochemical (Xylene isomers)

• Sugars (Fructose/glucose separation) � High fructose corn syrup

• Pharmaceuticals (Enantiomeric separation)Separate ‘good’ from ‘bad’ compounds based on chirality

62

Simulated Moving Bed

Direction of liquid flowand valve switching

Feed

Raffinate

Desorbent

ExtractRepeats exactly

the same operation

(Symmetric)

Feed Raffinate

DesorbentExtract

Operating parameters:

4 Zone velocities

+

Step time

Zone 4 Zone 2

Zone 3

Zone 1

Feed

RaffinateDesorbent

Extract

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63

Formulation of Optimization Problem

Zone velocities Step time

(Maximize average feed velocity)

Bounds on liquid velocities

Product requirements

CSS constraintSMB model

64

Treatment of PDEs: Single Discretization

t

x

1. PDE is discretized only in x ( turn a PDE into ODEs)

2. Set of ODEs are Integrated

ODE (Handled by integrator)PDE

C(xi,t)

t

Step size determined as integration proceeds

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65

Treatment of PDEs: Simultaneous Approach

t

x

(Orthogonal Collocation on Finite Elements)

k=1

k=2k=3

Algebraic equations PDE

Step size is determined a priori

tHuge number of variables (handled by optimizer)

C(xi,t)

66

Comparison of two approaches

CPU Time*

Shooting Approach 111.8 min

1.53 minSimultaneous Approach

# of iteration

49

47

0 1 2 3 4 5 6 7 8−0.1

0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

x [m]

Nor

mal

ized

Con

cenr

atio

n, C

i(x,t st

ep)/

CF

,i

Comp.1 Single discretizationComp.2 Single discretizationComp.1 Full discretizationComp.2 Full discretization Shooting and Simultaneous

methods find the same optimal solution

# of variables

33999

644Implemented on gPROMS, solved using SRQPD

Implemented on AMPL, solved using IPOPT

*On Pentium IV 2.8GHz

(89% spent by integrator)

(Linear isotherm, fructose/glucose separation)

Initial feed velocity: 0.01 m/h

Optimal feed velocity: 0.52 m/h

Optimization

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67

Superstructure for Zone Configuration

uD1

uF1

uE1

uE2

uR1

uF2

uE3

uR2

uF3

uE4

uR3

uF4

uE5

uR4

uF5

uE6

uR5

uR6

All velocities are constant

8 columns, multiple streams

Repeat exactly same stream policies for each step

Constraints:

68

Allows straightforward zone configuration optimizatio n

2-2-2-2

5 6

2 1

Feed Raffinate

DesorbentExtract

3

4 7

8

Superstructure configuration AVOIDS enumerating all configurations

CPU Time*: 1.73 min

Optimal feed velocity: 1.158 m/h*On Xeon 3.2GHz

Optimal :1-3-3-1

3

4

8

2

5 6 7

1

Feed Raffinate

DesorbentExtract

Optimal feed velocity: 0.906 m/h

4

5

8

3

6 7

1

Feed Raffinate

Extract

2

Desorbent

1-4-2-1

1.052 m/h

8

4

6 7

3

Feed Raffinate

Extract Desorbent2 1

5

0.957 m/h

3-2-2-1

# of columns 8 10 12 14

# of zone configurations 35 84 165 286

Too many configurations to enumerate!

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69

� Standard SMB

Nonstandard SMB: Addressed by Extended Superstructure NLP

� Three Zone

(Circulation loop is cut open)

� VARICOL

(Asynchronous switching)

70

0 2 4 6 80

0.5

1

x [m]

Ci(x

,t)/C

F,i →

8.000 m/h

⇓u

D1 =8.000m/h

t/tstep

= 0.142

→8.000 m/h

t/tstep

= 0.142

→8.000 m/h

⇓uR3 =8.000m/h

t/tstep

= 0.142

→8.000 m/h

⇓u

D4 =8.000m/h

⇓uE4=8.000m/h

t/tstep

= 0.142

0 2 4 6 80

0.5

1

x [m]

Ci(x

,t)/C

F,i →

7.916 m/h

⇓u

D1 =7.916m/h

t/tstep

= 0.334

→7.916 m/h

t/tstep

= 0.334

→7.916 m/h

⇓uR3 =7.916m/h

t/tstep

= 0.334

→8.000 m/h

⇓u

D4 =8.000m/h

⇓uE4=8.000m/h

t/tstep

= 0.334

0 2 4 6 80

0.5

1

x [m]

Ci(x

,t)/C

F,i →

8.000 m/h

⇓u

D1 =8.000m/h

t/tstep

= 0.434

→8.000 m/h

t/tstep

= 0.434

→8.000 m/h

t/tstep

= 0.434

→8.000 m/h

⇓uE4=8.000m/h

t/tstep

= 0.434

0 2 4 6 80

0.5

1

x [m]

Ci(x

,t)/C

F,i →

6.332 m/h

⇓u

D1 =6.332m/h

t/tstep

= 0.800

→6.332 m/h

t/tstep

= 0.800

→8.000 m/h

⇓u

F3=1.668m/h

t/tstep

= 0.800

→8.000 m/h

⇓uE4=8.000m/h

t/tstep

= 0.800

0 2 4 6 80

0.5

1

x [m]

Ci(x

,t)/C

F,i →

8.000 m/h

⇓u

D1 =8.000m/h

⇓uE1=3.757m/h

t/tstep

= 1.000

→4.243 m/h

t/tstep

= 1.000

→8.000 m/h

⇓u

F3=3.757m/h

t/tstep

= 1.000

→8.000 m/h

⇓uR4 =8.000m/h

t/tstep

= 1.000

Optimal Operating Scheme:Result of Superstructure Optimization

Standard SMB

PowerFeed Super -Structure

00.10.20.30.40.50.60.70.80.9

11.11.21.31.4

Op

tim

al T

hro

ug

hp

ut

[m/h

]

CPU Time for optimization: 9.03 min*

34098 variables, 34013 equations *on Xeon 3.2 GHz

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71

Nonlinear Model Predictive Control (NMPC)

Process

NMPC Controller

d : disturbancesz : differential statesy : algebraic states

u : manipulatedvariables

ysp : set points

( )( )dpuyzG

dpuyzFz

,,,,0

,,,,

==′

NMPC Estimation and Control

sConstraintOther

sConstraint Bound

)()),(),(),((0

)),(),(),(()(..

||))||||)(||min

init

1sp

ztztttytzG

tttytzFtzts

yty uy Q

kk

Q

==

=′

−+−∑ ∑ −

u

u

u(tu(tu

NMPC Subproblem

Why NMPC?

n Track a profile

n Severe nonlinear dynamics (e.g, sign changes in gains)

n Operate process over wide range (e.g., startup and shutdown)

Model Updater( )

( )dpuyzG

dpuyzFz

,,,,0

,,,,

==′

72

Dynamic optimization in a MATLAB Framework

Dynamic Optimization Problem

Process Model

Inequality Constraints

Initial Conditions

Constraints at Final Time

Objective Function

( ) 0puyxxf =′ t,,,,,

( ) 0=t,,,, puyxg

0),,,,,( ≤′ tpuyxxh

0xx =)( 0t

( ) 0,,,)(,)(,)(,)( 0 =′fffff ttttt pxuyxxϕ

( )ffft

tttf

,,),(t,)(,)( P 0f,,(t),

min0

xpuyxxpu

NLP Optimization Problem

Process Model

Inequality Constraints

Constraints at Final Time

Objective Function

( ) 0xpuyxf 0 =,,,ˆ,ˆ,ˆˆft

( ) 0puyxg =ft,,ˆ,ˆ,ˆˆ

0),,ˆ,ˆ,ˆ(ˆ ≤ftpuyxh

( ) 0,,,, =fNNN tttt

puyxϕ

( )fNNN tttt

,,,, Pmin puyx

Full Discretization of State and

Control Variables

Discretization Method

No. of Time Elements

Collocation Order

Saturator-System

copy ofDesign

WärmeschaltplanNr. -F Ref T - Erlangen, 13.Oc t.1999

SIEM ENS AGF Ref T In Bearbeitung

P..Druck ..bar

M..Massens trom..kg/s

PHI..Luft-Feuchte..%

H..Enthalpie..kJ /kg

T..Temperatur..°C

bar kJ /kgkg/s °C (X)

JOBKENNUNG : C:\Krawal-modular\IGCC\IGCC_Puertollano_komplett.gek

Alle Drücke s ind absolut

Dynamic Process

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73

Tennessee Eastman Process

Unstable Reactor

11 Controls; Product, Purge streams

Model extended with energy balances

74

Tennessee Eastman Challenge Process

Method of Full Discretization of State and Control Variables

Large-scale Sparse block-diagonal NLP

11Difference (control variables)

141Number of algebraic equations

152Number of algebraic variables

30Number of differential equations

DAE Model

14700Number of nonzeros in Hessian

49230Number of nonzeros in Jacobian

540Number of upper bounds

780Number of lower bounds

10260Number of constraints

109200

Number of variablesof which are fixed

NLP Optimization problem

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75

Setpoint change studies

Setpoint changes for the base case [Downs & Vogel]

+2%Make a step change so that the composition of component B in the gas purge changes from 13.82 to 15.82%

StepPurge gas composition of component B change

-60 kPaMake a step change so that the reactor operating pressure changes from 2805 to 2745 kPa

StepReactor operating pressure change

-15%Make a step change to the variable(s) used to set the process production rate so that the product flow leaving the stripper column base changes from 14,228 to 12,094 kg h-1

StepProduction rate change

MagnitudeTypeProcess variable

76

Case Study:Change Reactor pressure by 60 kPa

Control profiles

All profiles return to their base case values

Same production rate

Same product quality

Same control profile

Lower pressure – leads to larger gas phase (reactor) volume

Less compressor load

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77

TE Case Study – Results I

Shift in TE process

Same production rate

More volume for reaction

Same reactor temperature

Initially less cooling water flow (more evaporation)

78

Case Study- Results II

Shift in TE process

Shift in reactor effluent to more condensables

Increase cooling water flow

Increase stripper steam to ensure same purity

Less compressor work

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79

Case Study: Change Reactor Pressure by 60 kPa

Optimization with IPOPT

1000 Optimization Cycles

5-7 CPU seconds

11-14 Iterations

Optimization with SNOPT

Often failed due to poor conditioning

Could not be solved within sampling times

> 100 Iterations

80

Parameter/State Estimation

Process

NMPC Controller

d : disturbancesz : differential statesy : algebraic states

u : manipulatedvariables

ysp : set points

( )( )dpuyzG

dpuyzFz

,,,,0

,,,,

==′

NMPC Estimation and Control

sConstraintOther

sConstraint Bound

)()),(,),(),((0

)),(,),(),(()(..

||ˆ||||ˆ)(||min

initztzttutytzG

ttutytzFtzts

uuyty uy Q

kk

Q

==

=′

−+−∑ ∑

p

p

p

Parameter Estimation Subproblem

Moving Horizon Estimation?

n Estimate a finite number of states and model parameters (unmeasured disturbances, rate constants, transport parameters)

n Compensate for process drifts and slowly changing conditions

n Allow better controller performance

Model Updater( )

( )dpuyzG

dpuyzFz

,,,,0

,,,,

==′

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81

Early Warning Detection System Municipal Water Networks

•Installed sensors provide an early warning of contamination

•System provides only a coarse measure of contamination time and location

•Desired: Accurate and fast time & location information

82

Optimization ProblemNode Concentrations &

Injection Terms Only

Pipe Boundary Concentrations

Injection Terms Only

Only Constraints with Spatial Dependence

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83

Collapsed Node Models

Plug Flow

Complete Mixing

No Reaction

Known Sources Contaminant Free

Time Dependent Mass Injections at All Nodes (Negligible Flow rates)

Decoupled Hydraulics and Water Quality Calculations

Water Quality Model

Pipes, Valves, Pumps

Storage Tanks, Junctions

84

Modeling Water Distribution Systems

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85

Existing Simulation Techniques

Eulerian

Discretize in time and space

Track concentration at fixed points or volumes

Local process for simulation, but global treatment needed for simultaneous optimization

Lagrangian

Discretize in time alone

Track concentration of elements as they move

Algorithmic in nature

Review of these methods by Rossman and Boulos, 1996.

Same as our Discretization

Too Many Constraints

No Straightforward Representation

Derivative Calculations?

86

Origin Tracking Algorithm

Known Hydraulics – Function of Time

Pipe Network PDEs Linear in Concentration

Pipe by Pipe PDEs

• Efficient for Large Networks

• Convert PDEs to DAEs with variable time delays

Removes Need to Discretize in Space

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87

Water network demands known.

Linear PDEs for concentration

Convert to delay-differential equations

Apply implicit R-K formulation

Source Inversion Formulation

HydraulicSimulator(EPANET)

FormulationToolFlow

demands

88

Municipal Source Detection Example

Algorithm successful on over 1000 numerical tests with real municipal water networks

Solution time < 2 CPU minutes for ~ 250,000 variables, ~45,000 degrees of freedom

• Effective in a real time setting

Formulation tool links to existing water network software

Can impose unique solutions through an extended MIQP formulation (post-processing phase)

0

5

10

15

20

25

30

35

40

0 1 2 3 4 5 6 7 8 9 10 11 12

Time (hrs)

Sca

led

Inje

cted

Mas

s

A

B

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89

Goal: Bridge between planning, logistics (linear, discrete problems) and detailed process models (nonlinear, spatial, dynamic)

Planning and Scheduling• Many Discrete Decisions• Few Nonlinearities

Planning

Scheduling

Site-wide Optimization

Real-time Optimization

Model Predictive Control

Regulatory Control

Fea

sibi

lity

Per

form

ance

Decision Pyramid for Process Operations

90

Real-time Optimization and Advanced Process Control• Fewer discrete decisions• Many nonlinearities• Frequent, “on-line” time-critical solutions• Higher level decisions must be feasible• Performance communicated for higher level decisions

Planning

Scheduling

Site-wide Optimization

Real-time Optimization

Model Predictive Control

Regulatory Control

Fea

sibi

lity

Per

form

ance

Decision Pyramid for Process Operations

APCMPC ⊂

Off-line (open loop)

On-line (closed loop)

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46

Steady-state On-line Optimization: Components

Plant

DR-PEc(x, u, p) = 0

RTOc(x, u, p) = 0

APC

y

p

u

w

•Data reconciliation – identify gross errors and inconsistency in data•Periodic update of process model identification •Usually requires APC loops (MPC, DMC, etc.)•RTO/APC interactions: Assume decomposition of time scales

•APC to handle disturbances and fast dynamics•RTO to handle static operations

•Typical cycle: 1-2 hours, closed loop

•What if steady state and dynamic models are inconsistent? 6

92

Dynamic Real-time Optimization Integrate On-line Optimization/Control with Off-line Planning• Consistent, first-principle models• Consistent, long-range, multi-stage planning• Increase in computational complexity • Time-critical calculations

Applications• Batch processes• Grade transitions• Cyclic reactors (coking, regeneration…)• Cyclic processes (PSA, SMB…)

Continuous processes are never in steady state:

• Feed changes• Nonstandard operations

• Optimal disturbance rejections

Simulation environments (e.g., ACM, gPROMS) and first principle dynamic models are widely used for off-line studies

8

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47

Some DRTO Case Studies• Integrated grade transitions

– MINLP of scheduling with dynamics (Flores & Grossmann, 2006, Prata et al., 2007)

– Significant reduction in transition times

• Dynamic Predictive Scheduling– Processes and supply chains need to optimally

respond to disturbances through dynamic models – Reduction in energy cost by factor of two

• Cyclic Process Optimization– Decoking scheduling– SMB optimization– PSA optimization– Productivity increases by factor of 2-3

9

94

•What are the Interactions between Design and Dynamics and Planning?

•What are the differences between Sequential and Simultaneous Strategies?

•Especially Important in Batch Systems

Batch Integration Case Study

Production PlanningStage 1

Stage 2

A

A B

B C

C

Plant Design

TR

Time Time

Dynamic Processing

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95

• discretize (DAEs), state and control profiles• large-scale optimization problem• handles profile constraints directly• incorporates equipment variables directly • DAE model solved only once• converges for unstable systems

Simultaneous Dynamic OptimizationSimultaneous Dynamic OptimizationSimultaneous Dynamic OptimizationSimultaneous Dynamic Optimization

Best transient Best constant

Higher conversion in same time

T

Time

Con

v.

Time

Fewer product batches

TSame conversion in reduced time

Time

Con

v.

Time

Shorter processing times

Dynamic Processing

Production PlanningStage 1

Stage 2

A

A B

B C

C

Shorter Planning Horizon

96

Scheduling Formulation• sequencing of tasks, products equipment• expensive discrete combinatorial optimization• consider ideal transfer policies (UIS and ZW)• closed form relations (Birewar and Grossmann, 1989)A B N

stage I

stage 2

stage I

stage 2

A B N

Zero Wait (ZW) Immediate transfer requiredSlack times dependent on pairLonger production cycle requiredUnlimited Int. Storage(UIS)Short production cycleCycle time independent of sequence

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97

Case Study ExampleCase Study Example

zi ,I0 zi ,II

0zi ,III

0 zi ,IV0

zi ,IVf

zi ,If zi ,II

f zi ,IIIf

Bi

A + B → C

C + B → P + E

P + C → G

4 stages, 3 products of different purity Dynamic reactor - temperature profileDynamic column - reflux profile

Process Optimization Cases

SQ - Sequential Design - Scheduling - DynamicsSM - Simultaneous Design and Scheduling

Dynamics with endpoints fixed . SM* - Simultaneous Design, Scheduling and Dynamics

98

5

10

15

20

25

580

590

600

610

620

630

640

0 0.5 1 1.5 2 2.50 0.25 0.5 0.75 1 1.25Tim e (h r.)

Dyn a m ic

C o nsta nt

Dyn a mic

C o nsta nt

Comparison of Dynamic vs. Best Constant Profiles

R0 - best constant temperature profileR1 - optimal temperature policy

C0 - best constant reflux ratioC1 - optimal reflux ratio

Scenarios in Case Study

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Results for Simultaneous Cases

R0/R1 best constant / optimal temperature

C0/C1best constant / optimal reflux ratio

0

5 0 0 0

1 0 0 0 0

1 5 0 0 0

2 0 0 0 0

Pro

fit (

$)

R 0 C 0 R 1 C 0 R 0 C 1 R 1 C 1

C a s e s

S Im u lt a n e o u s w it h F R E E s t a t e s

S im u lt a n e o u s w it h F I X E D s t a t e sS e q u e n t ia l

I

I II I I

I V

I

I II I I

I V

II II I I

I V

- ZW schedule becomes tighter

- less dependent on product sequences

SQ

SM*

SM

100

SummarySequential Approaches- Parameter Optimization

• Gradients by: Direct and Adjoint Sensitivity Equations- Optimal Control (Profile Optimization)

• Variational Methods• NLP-Based Methods

- Require Repeated Solution of Model- State Constraints are Difficult to Handle

Simultaneous Approach- Discretize ODE's using orthogonal collocation on finite elements (solve larger optimization problem)- Accurate approximation of states, location of control discontinuities through element placement.- Straightforward addition of state constraints.- Deals with unstable systems

Simultaneous Strategies are Effective- Directly enforce constraints- Solve model only once- Avoid difficulties at intermediate points

Large-Scale Extensions- Exploit structure of DAE discretization through decomposition- Large problems solved efficiently with IPOPT

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ReferencesBetts, J. T., ., Practical Methods for Optimal Control Using Nonlinear Programming, SIAM, (2001)Bryson, A.E. and Y.C. Ho, Applied Optimal Control, Ginn/Blaisdell, (1968).Himmelblau, D.M., T.F. Edgar and L. Lasdon, Optimization of Chemical Processes, McGraw-Hill, (2001).Ray. W.H., Advanced Process Control, McGraw-Hill, (1981).

Software• Dynamic Optimization CodesACM – Aspen Custom ModelerDynoPC - simultaneous optimization code (CMU)COOPT - sequential optimization code (Petzold)gOPT - sequential code integrated into gProms (PSE)MUSCOD - multiple shooting optimization (Bock)NOVA - SQP and collocation code (DOT Products)• Sensitivity Codes for DAEsDASOLV - staggered direct method (PSE)DASPK 3.0 - various methods (Petzold)SDASAC - staggered direct method (sparse)DDASAC - staggered direct method (dense)

DAE Optimization Resources

ReferencesF. Allgöwer and A. Zheng (eds.), Nonlinear Model Predictive Control, Birkhaeuser, Basel (2000)

R. D. Bartusiak, “NLMPC: A platform for optimal control of feed- or product-flexible manufacturing,” in Nonlinear Model Predictive Control 05, Allgower, Findeisen, Biegler (eds.), Springer, to appear

Biegler Homepage: http://dynopt.cheme.cmu.edu/papers.htm

Forbes, J. F. and Marlin, T. E.. Model Accuracy for Economic Optimizing Controllers: The Bias Update Case. Ind.Eng.Chem.Res. 33, 1919-1929. 1994

Forbes, J. F. and Marlin, T. E.. “Design Cost: A Systematic Approach to Technology Selection for Model-Based Real-Time Optimization Systems,” Computers Chem.Engng. 20[6/7], 717-734. 1996

Grossmann Homepage: http://egon.cheme.cmu.edu/papers.html

M. Grötschel, S. Krumke, J. Rambau (eds.), Online Optimization of Large Systems, Springer, Berlin (2001)

K. Naidoo, J. Guiver, P. Turner, M. Keenan, M. Harmse “Experiences with Nonlinear MPC in Polymer Manufacturing,” in Nonlinear Model Predictive Control 05, Allgower, Findeisen, Biegler (eds.), Springer, to appear

Yip, W. S. and Marlin, T. E. “Multiple Data Sets for Model Updating in Real-Time Operations Optimization,” Computers Chem.Engng. 26[10], 1345-1362. 2002.

42

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52

References – Some DRTO Case Studies

Busch, J.; Oldenburg, J.; Santos, M.; Cruse, A.; Marquardt, W. Dynamicpredictive scheduling of operational strategies for continuous processes using mixed-logic dynamic optimization, Comput. Chem. Eng., 2007, 31, 574-587.

Flores-Tlacuahuac, A.; Grossmann, I.E. Simultaneous cyclic scheduling andcontrol of a multiproduct CSTR, Ind. Eng. Chem. Res., 2006, 27, 6698-6712.

Kadam, J.; Srinivasan, B., Bonvin, D., Marquardt, W. Optimal grade transition in industrial polymerization processes via NCO tracking. AIChE J., 2007, 53, 3, 627-639.

Oldenburg, J.; Marquardt, W.; Heinz D.; Leineweber, D. B., Mixed-logic dynamic optimization applied to batch distillation process design, AIChE J. 2003, 48(11), 2900- 2917.

E Perea, B E Ydstie and I E Grossmann, A model predictive control strategy for supply chain optimization, Comput. Chem. Eng., 2003, 27, 1201-1218.

M. Liepelt, K Schittkowski, Optimal control of distributed systems with breakpoints, p. 271 in M. Grötschel, S. Krumke, J. Rambau (eds.), Online Optimization of Large Systems, Springer, Berlin (2001)

See also Biegler homepage

43

104

Interface of DynoPC

Output/Graphics & TextsModel in FORTRAN

F2c/C++

ADOL_C

Preprocessor

DDASSL

COLDAE

Data/Config.

Simulator/Discretizer

F/DF

Starting Point Linearization

Optimal Solution

FILTER

Reduced Space IPOPT

F/DFLine Search

Calc. of independent variable move

Interior PointNewton Step

Decomposition

DynoPC – Windows Implementation

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105

A B C1 2

da

atk

E

RTa= − − ⋅1

1exp( )

db

atk

E

RTa k

E

RTb= − ⋅ − − ⋅1

12

2exp( ) exp( )

a + b + c = 1

..

)(

ts

tbMax f

T

Example: Batch Reactor Temperature

106

Example: Car Problem

Min tfs.t. z1' = z2

z2' = uz2 ≤ zmax

-2 ≤ u ≤ 1

subroutine model(nz,ny,nu,np,t,z,dmz,y,u,p,f)double precision t, z(nz),dmz(nz), y(ny),u(nu),p(np)

double precision f(nz+ny)

f(1) = p(1)*z(2) - dmz(1)f(2) = p(1)*u(1) - dmz(2)

returnend403020100

-3

-2

-1

0

1

2

0

2

4

6

8

10

12

Acceleration

Velocity

Time

Acc

eler

atio

n, u

(t)

Vel

ocit

y

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Example: Crystallizer Temperature

Steam

Cooling water

TT TC

Control variable = Tjacket = f(t)?

Maximize crystal sizeat final time

0.0E+00

5.0E-04

1.0E-03

1.5E-03

2.0E-03

2.5E-03

3.0E-03

3.5E-03

4.0E-03

4.5E-03

0 5 10 15 20

Time (hr)

Cry

stal

siz

e

0

10

20

30

40

50

60

T ja

cket

(C)

Crystal Size T jacket

SUBROUTINE model(nz,ny,nu,np,x,z,dmz,y,u,p,f)implicit double precision (a-h,o-z)double precision f(nz+ny),z(nz),dmz(nz),Y(ny),yp(4),u(1)double precision kgr, ln0, ls0, kc, ke, kex, lau, deltT, alphadimension a(0:3), b(0:3)data alpha/1.d-4/,a/-66.4309d0, 2.8604d0, -.022579d0, 6.7117d-5/,+ b/16.08852d0, -2.708263d0, .0670694d0, -3.5685d-4/, kgr/ 4.18d-3/,+ en / 1.1d0/, ln0/ 5.d-5/, Bn / 3.85d2/, em / 5.72/, ws0/ 2.d0/,+ Ls0/ 5.d-4 /, Kc / 35.d0 /, Kex/ 65.d0/, are/ 5.8d0 /,+ amt/ 60.d0 /, V0 / 1500.d0/, cw0/ 80.d0/,cw1/ 45.d0/,v1 /200.d0/,+ tm1/ 55.d0/,x6r/0.d0/, tem/ 0.15d0/,clau/ 1580.d0/,lau/1.35d0/,+ cp/ 0.4d0 /,cbata/ 1.2d0/, calfa/ .2d0 /, cwt/ 10.d0/

ke = kex*area x7i = cw0*lau/(100.d0-cw0)v = (1.d0 - cw0/100.d0)*v0 w = lau*v0 yp(1) = (deltT + dsqrt(deltT**2 + alpha**2))*0.5d0yp(2) = (a(0) + a(1)*yp(4) + a(2)*yp(4)**2 + a(3)*yp(4)**3)yp(3) = (b(0) + b(1)*yp(4) + b(2)*yp(4)**2 + b(3)*yp(4)**3)deltT = yp(2) - z(8) yp(4) = 100.d0*z(7)/(lau+z(7))

f(1) = Kgr*z(1)**0.5*yp(1)**en - dmz(1)f(2) = Bn*yp(1)**em*1.d-6 - dmz(2)f(3) = ((z(2)*dmz(1) + dmz(2) * Ln0)*1.d+6*1.d-4) -dmz(3)f(4) = (2.d0*cbata*z(3)*1.d+4*dmz(1)+dmz(2)*Ln0**2*1.d+6)-dmz(4)f(5) = (3.d0*calfa*z(4)*dmz(1)+dmz(2)*Ln0**3*1.d+6) - dmz(5)f(6) = (3.d0*Ws0/(Ls0**3)*z(1)**2*dmz(1)+clau*V*dmz(5))-dmz(6)f(7) = -dmz(6)/V - dmz(7)f(8) = (Kc*dmz(6) - Ke*(z(8) - u(1)))/(w*cp) - dmz(8)f(9) = y(1)+YP(3)- u(1) returnend


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