Numerical Synthesis of Pontryagin Optimal Control Minimizers Using Sampling-Based Methods
|
|
- Calvin Campbell
- 5 years ago
- Views:
Transcription
1 Numerical Synthesis of Pontryagin Optimal Control Minimizers Using Sampling-Based Methods Humberto Gonzalez Department of Electrical & Systems Engineering Washington University in St. Louis April 7th, 2017 Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 1
2 Critical Point Characterization Synthesis of Optimal Control Inputs Simulation: Optimal HVAC Operation Optimal Control Applications x x1 4 5 x2 2 Path Planning (Vasudevan et al., 2013) Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 2
3 Critical Point Characterization Synthesis of Optimal Control Inputs Simulation: Optimal HVAC Operation Optimal Control Applications x x1 4 5 x2 2 Dynamic Game Verification (Margellos & Lygeros, 2011) Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 2
4 Critical Point Characterization Synthesis of Optimal Control Inputs Simulation: Optimal HVAC Operation Optimal Control Applications x x1 4 5 x2 2 Robust & Ensemble Control (Zlotnik & Li, 2012) Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 2
5 General Optimal Control Formulation min u( ), x 0, T T 0 L ( x(s), u(s) ) ds + ϕ ( x(t ) ), subject to: ẋ(t) = f ( x(t), u(t) ), t [0, T ], x(0) = x 0, x(t) X, t [0, T ], u(t) U, t [0, T ], ( x0, x(t ) ) S. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 3
6 From Theory to Practice... Pros: Optimal control framework is flexible. Decades of accumulated literature. Particular cases can be efficiently solved. Cons: General numerical solvers are prone to converge to non-minimizers. Computation time can be very long, even for small problems. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 4
7 From Theory to Practice... Pros: Optimal control framework is flexible. Decades of accumulated literature. Particular cases can be efficiently solved. Cons: General numerical solvers are prone to converge to non-minimizers. Computation time can be very long, even for small problems. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 4
8 From Theory to Practice... Pros: Optimal control framework is flexible. Decades of accumulated literature. Particular cases can be efficiently solved. Cons: General numerical solvers are prone to converge to non-minimizers. Computation time can be very long, even for small problems. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 4
9 From Theory to Practice... Pros: Optimal control framework is flexible. Decades of accumulated literature. Particular cases can be efficiently solved. Cons: General numerical solvers are prone to converge to non-minimizers. Computation time can be very long, even for small problems. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 4
10 Summary of this Talk We developed a new class of numerical optimal control synthesis method. Trade-off between accuracy and efficiency can be easily configured. Aim to solve large-scale problems. Our algorithm avoids many undesirable stationary points. Enable real-time applications. R. He and H. Gonzalez, Numerical Synthesis of Pontryagin Optimal Control Minimizers Using Sampling-Based Methods,, arxiv: Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 5
11 Summary of this Talk We developed a new class of numerical optimal control synthesis method. Trade-off between accuracy and efficiency can be easily configured. Aim to solve large-scale problems. Our algorithm avoids many undesirable stationary points. Enable real-time applications. R. He and H. Gonzalez, Numerical Synthesis of Pontryagin Optimal Control Minimizers Using Sampling-Based Methods,, arxiv: Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 5
12 Summary of this Talk We developed a new class of numerical optimal control synthesis method. Trade-off between accuracy and efficiency can be easily configured. Aim to solve large-scale problems. Our algorithm avoids many undesirable stationary points. Enable real-time applications. R. He and H. Gonzalez, Numerical Synthesis of Pontryagin Optimal Control Minimizers Using Sampling-Based Methods,, arxiv: Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 5
13 Summary of this Talk We developed a new class of numerical optimal control synthesis method. Trade-off between accuracy and efficiency can be easily configured. Aim to solve large-scale problems. Our algorithm avoids many undesirable stationary points. Enable real-time applications. R. He and H. Gonzalez, Numerical Synthesis of Pontryagin Optimal Control Minimizers Using Sampling-Based Methods,, arxiv: Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 5
14 1. Critical Point Characterization 2. Synthesis of Optimal Control Inputs 3. Simulation: Optimal HVAC Operation Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 6
15 Simplified Optimal Control Formulation Let us define the original optimal control problem: where: (P o ) min u( ) ϕ( x(t ) ), x 0 R n is given subject to: ẋ(t) = f ( x(t), u(t) ), t [0, T ], x(0) = x 0, U R m is compact and convex. u(t) U, t [0, T ]. E. Polak, Optimization: Algorithms and Consistent Approximations, ser. Applied Mathematical Sciences. Springer, 1997, Chapter Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 7
16 Relaxed Optimal Control Formulation Now consider the relaxed optimal control problem: (P r ) min {µ t} t [0,T ] ϕ ( x(t ) ), subject to: ẋ(t) = R m f ( x(t), u ) dµ t (u), t [0, T ], x(0) = x 0, supp(µ t ) U, t [0, T ]. where, for each t [0, T ], µ t is a unitary Borel measure, i.e.: R m dµ t (u) = 1. J. Warga, Optimal Control of Differential and Functional Equations. Academic Press, 1972 Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 8
17 Original-Relaxed Equivalence Given û(t): [0, T ] U, let µ t (u) = 1[u = û(t)] for each t. Then both original and relaxed trajectories generated by û and µ are equivalent. Thus, Feas(P o ) Feas(P r ), and Value(P o ) > Value(P r ). Proposition Value(P o ) = Value(P r ). The proof follows using Berkovitz s Chattering Lemma for switched systems and the fact that L 2 convergence of inputs implies uniform convergence of the trajectories. L. D. Berkovitz, Optimal Control Theory, ser. Applied Mathematical Sciences. Springer, 1974 Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 9
18 Original-Relaxed Equivalence Given û(t): [0, T ] U, let µ t (u) = 1[u = û(t)] for each t. Then both original and relaxed trajectories generated by û and µ are equivalent. Thus, Feas(P o ) Feas(P r ), and Value(P o ) > Value(P r ). Proposition Value(P o ) = Value(P r ). The proof follows using Berkovitz s Chattering Lemma for switched systems and the fact that L 2 convergence of inputs implies uniform convergence of the trajectories. L. D. Berkovitz, Optimal Control Theory, ser. Applied Mathematical Sciences. Springer, 1974 Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 9
19 Original-Relaxed Equivalence Given û(t): [0, T ] U, let µ t (u) = 1[u = û(t)] for each t. Then both original and relaxed trajectories generated by û and µ are equivalent. Thus, Feas(P o ) Feas(P r ), and Value(P o ) > Value(P r ). Proposition Value(P o ) = Value(P r ). The proof follows using Berkovitz s Chattering Lemma for switched systems and the fact that L 2 convergence of inputs implies uniform convergence of the trajectories. L. D. Berkovitz, Optimal Control Theory, ser. Applied Mathematical Sciences. Springer, 1974 Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 9
20 Optimality Functions Definition (Polak, 1997) Consider the following optimization problem: min{ψ(x) x X }. We say that θ : X R is an optimality function of this problem if: θ(x) 0 for each x X ; and, if x is a minimizer of ψ, then θ(x) = 0. For example, if X R n then: θ(x) = min ψ(x), h, and θ(x) = min ψ(x), h + h 2 2, h 1 h are optimality functions. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 10
21 Optimality Functions Definition (Polak, 1997) Consider the following optimization problem: min{ψ(x) x X }. We say that θ : X R is an optimality function of this problem if: θ(x) 0 for each x X ; and, if x is a minimizer of ψ, then θ(x) = 0. For example, if X R n then: θ(x) = min ψ(x), h, and θ(x) = min ψ(x), h + h 2 2, h 1 h are optimality functions. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 10
22 Original Problem Optimality Functions Let u 0 : [0, T ] U and x 0 be its associated trajectory. Let: ϕ( θ o,l (x 0, u 0 ) = min x0 (T ) ) δx(t ), δu( ) x subject to: δẋ(t) = f ( x0 (t), u 0 (t) ) δx(t)+ x + f ( x0 (t), u 0 (t) ) δu(t), u δx(0) = 0, u 0 (t) + δu(t) U, t [0, T ]. We say that θ o,l is the linearized, or variational, optimality function of P o. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 11
23 Original Problem Optimality Functions Let u 0 : [0, T ] U and x 0 be its associated trajectory. Let: ϕ( θ o,l (x 0, u 0 ) = min x0 (T ) ) δx(t ), δu( ) x subject to: δẋ(t) = f ( x0 (t), u 0 (t) ) δx(t)+ x + f ( x0 (t), u 0 (t) ) δu(t), u δx(0) = 0, u 0 (t) + δu(t) U, t [0, T ]. We say that θ o,l is the linearized, or variational, optimality function of P o. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 11
24 Original Problem Optimality Functions Also, let: θ o,h (x 0, u 0 ) = min u( ) subject to: T 0 p 0 (t) T ( f ( x 0 (t), u(t) ) f ( x 0 (t), u 0 (t) )) dt, ṗ 0 (t) = f T ( x0 (t), u 0 (t) ) p 0 (t), x p 0 (T ) = ϕ ( ) x(t ), x u(t) U, t [0, T ]. We say that θ o,h is the Pontryagin optimality function of P o. Proposition θ o,h (x 0, u 0 ) = 0 θ o,l (x 0, u 0 ) = 0. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 12
25 Original Problem Optimality Functions Also, let: θ o,h (x 0, u 0 ) = min u( ) subject to: T 0 p 0 (t) T ( f ( x 0 (t), u(t) ) f ( x 0 (t), u 0 (t) )) dt, ṗ 0 (t) = f T ( x0 (t), u 0 (t) ) p 0 (t), x p 0 (T ) = ϕ ( ) x(t ), x u(t) U, t [0, T ]. We say that θ o,h is the Pontryagin optimality function of P o. Proposition θ o,h (x 0, u 0 ) = 0 θ o,l (x 0, u 0 ) = 0. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 12
26 Original Problem Optimality Functions Also, let: θ o,h (x 0, u 0 ) = min u( ) subject to: T 0 p 0 (t) T ( f ( x 0 (t), u(t) ) f ( x 0 (t), u 0 (t) )) dt, ṗ 0 (t) = f T ( x0 (t), u 0 (t) ) p 0 (t), x p 0 (T ) = ϕ ( ) x(t ), x u(t) U, t [0, T ]. We say that θ o,h is the Pontryagin optimality function of P o. Proposition θ o,h (x 0, u 0 ) = 0 θ o,l (x 0, u 0 ) = 0. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 12
27 Relaxed Problem Optimality Functions Let: θ r,l (x 0, µ 0 ) = min {δµ t} t ϕ( x0 (T ) ) δx(t ), x ( ( x0 (t), u ) ) dµ 0,t (u) δx(t)+ f subject to: δẋ(t) = R m x + f ( x 0 (t), u ) dδµ t (u), R m δx(0) = 0, supp(µ 0,t + δµ t ) U, t [0, T ]. We say that θ r,l is the linearized, or variational, optimality function of P r. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 13
28 Relaxed Problem Optimality Functions Let: θ r,l (x 0, µ 0 ) = min {δµ t} t ϕ( x0 (T ) ) δx(t ), x ( ( x0 (t), u ) ) dµ 0,t (u) δx(t)+ f subject to: δẋ(t) = R m x + f ( x 0 (t), u ) dδµ t (u), R m δx(0) = 0, supp(µ 0,t + δµ t ) U, t [0, T ]. We say that θ r,l is the linearized, or variational, optimality function of P r. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 13
29 Relaxed Problem Optimality Functions Also, let: θ r,h (x 0, µ 0 ) = min {δµ t} t T 0 p 0 (t) ( R T f ( x 0 (t), u ) ) dδµ t (u) dt, m ( f T ( subject to: ṗ 0 (t) = x0 (t), u ) dµ 0 (u)) p 0 (t), R m x p 0 (T ) = ϕ ( ) x(t ), x supp(µ 0,t + δµ t ) U, t [0, T ], dδµ t (u) = 0, t [0, T ]. R m We say that θ r,h is the Pontryagin optimality function of P r. Proposition θ r,h (x 0, u 0 ) = θ r,l (x 0, u 0 ), and so are their minimizing arguments. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 14
30 Relaxed Problem Optimality Functions Also, let: θ r,h (x 0, µ 0 ) = min {δµ t} t T 0 p 0 (t) ( R T f ( x 0 (t), u ) ) dδµ t (u) dt, m ( f T ( subject to: ṗ 0 (t) = x0 (t), u ) dµ 0 (u)) p 0 (t), R m x p 0 (T ) = ϕ ( ) x(t ), x supp(µ 0,t + δµ t ) U, t [0, T ], dδµ t (u) = 0, t [0, T ]. R m We say that θ r,h is the Pontryagin optimality function of P r. Proposition θ r,h (x 0, u 0 ) = θ r,l (x 0, u 0 ), and so are their minimizing arguments. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 14
31 Relaxed Problem Optimality Functions Also, let: θ r,h (x 0, µ 0 ) = min {δµ t} t T 0 p 0 (t) ( R T f ( x 0 (t), u ) ) dδµ t (u) dt, m ( f T ( subject to: ṗ 0 (t) = x0 (t), u ) dµ 0 (u)) p 0 (t), R m x p 0 (T ) = ϕ ( ) x(t ), x supp(µ 0,t + δµ t ) U, t [0, T ], dδµ t (u) = 0, t [0, T ]. R m We say that θ r,h is the Pontryagin optimality function of P r. Proposition θ r,h (x 0, u 0 ) = θ r,l (x 0, u 0 ), and so are their minimizing arguments. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 14
32 Idea Solve the relaxed problem using (tried and tested) variational-based methods, where at each step we compute θ r,h to check for optimality. 2. Once we find a minimizer, synthesize an input signal that approximates the optimal relaxed trajectory. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 15
33 Idea Solve the relaxed problem using (tried and tested) variational-based methods, where at each step we compute θ r,h to check for optimality. 2. Once we find a minimizer, synthesize an input signal that approximates the optimal relaxed trajectory. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 15
34 1. Critical Point Characterization 2. Synthesis of Optimal Control Inputs 3. Simulation: Optimal HVAC Operation Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 16
35 Computing θ r,h Note that θ r,h is a convex optimization problem. In fact, it is a linear infinite-dimensional program. Also note that we can rewrite θ r,h as: T θ r,h (x 0, µ 0 ) = min p 0 (t) T f {µ 1,t } t 0 ( R ( x 0 (t), u ) dµ 1,t (u)+ m f ( x 0 (t), u ) ) dµ 0,t (u) dt, R m subject to: supp(µ 1,t ) U, t [0, T ]. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 17
36 Computing θ r,h Note that θ r,h is a convex optimization problem. In fact, it is a linear infinite-dimensional program. Also note that we can rewrite θ r,h as: T θ r,h (x 0, µ 0 ) = min p 0 (t) T f {µ 1,t } t 0 ( R ( x 0 (t), u ) dµ 1,t (u)+ m f ( x 0 (t), u ) ) dµ 0,t (u) dt, R m subject to: supp(µ 1,t ) U, t [0, T ]. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 17
37 Computing θ r,h Proposition Let x R n. Then: { } f(x, u) dµ(u) supp(µ) U = co{f(x, u) u U}. R m Hence: T θ r,h (x 0, µ 0 ) = min p 0 (t) (z(t) T f ( x 0 (t), u ) ) dµ 0,t (u) dt, {µ 1,t } t 0 R m subject to: z(t) co { f ( x 0 (t), u ) u U }. Computing Pontryagin-optimal points is as hard as finding a good representation for the convex hull of f(x, ). Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 18
38 Computing θ r,h Proposition Let x R n. Then: { } f(x, u) dµ(u) supp(µ) U = co{f(x, u) u U}. R m Hence: T θ r,h (x 0, µ 0 ) = min p 0 (t) (z(t) T f ( x 0 (t), u ) ) dµ 0,t (u) dt, {µ 1,t } t 0 R m subject to: z(t) co { f ( x 0 (t), u ) u U }. Computing Pontryagin-optimal points is as hard as finding a good representation for the convex hull of f(x, ). Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 18
39 Computing θ r,h Proposition Let x R n. Then: { } f(x, u) dµ(u) supp(µ) U = co{f(x, u) u U}. R m Hence: T θ r,h (x 0, µ 0 ) = min p 0 (t) (z(t) T f ( x 0 (t), u ) ) dµ 0,t (u) dt, {µ 1,t } t 0 R m subject to: z(t) co { f ( x 0 (t), u ) u U }. Computing Pontryagin-optimal points is as hard as finding a good representation for the convex hull of f(x, ). Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 18
40 Sampling-Based Synthesis Let {u i } N i=1 U be a set of samples. Then for each t [0, T ]: co { f ( x 0 (t), u ) u U } { N ω i (t) f ( ) N } x 0 (t), u i ω i (t) = 1, ω i (t) 0. i=1 After sampling, our classical dynamical system becomes a switched hybrid system. Hence, we can use the PWM-based projection method in Vasudevan et al. (SICON, 2013) to synthesize input signals. i=1 R. Vasudevan, H. Gonzalez, R. Bajcsy, and S. S. Sastry, Consistent Approximations for the Optimal Control of Constrained Switched Systems Part 1: A Conceptual Algorithm, Siam journal on control and optimization, vol. 51, no. 6, pp , 2013 R. Vasudevan, H. Gonzalez, R. Bajcsy, and S. S. Sastry, Consistent Approximations for the Optimal Control of Constrained Switched Systems Part 2: An Implementable Algorithm, Siam journal on control and optimization, vol. 51, no. 6, pp , 2013 Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 19
41 Sampling-Based Synthesis Let {u i } N i=1 U be a set of samples. Then for each t [0, T ]: co { f ( x 0 (t), u ) u U } { N ω i (t) f ( ) N } x 0 (t), u i ω i (t) = 1, ω i (t) 0. i=1 After sampling, our classical dynamical system becomes a switched hybrid system. Hence, we can use the PWM-based projection method in Vasudevan et al. (SICON, 2013) to synthesize input signals. i=1 R. Vasudevan, H. Gonzalez, R. Bajcsy, and S. S. Sastry, Consistent Approximations for the Optimal Control of Constrained Switched Systems Part 1: A Conceptual Algorithm, Siam journal on control and optimization, vol. 51, no. 6, pp , 2013 R. Vasudevan, H. Gonzalez, R. Bajcsy, and S. S. Sastry, Consistent Approximations for the Optimal Control of Constrained Switched Systems Part 2: An Implementable Algorithm, Siam journal on control and optimization, vol. 51, no. 6, pp , 2013 Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 19
42 Sampling-Based Synthesis Algorithm 1. Compute samples of U. 2. Iteratively solve the relaxed optimal control problem using a gradient-based method. 3. Synthesize an approximation of the optimal relaxed input using PWM-based projection. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 20
43 Numerical Considerations Note that if f(x, u k ) lays strictly in the relative interior of co{f(x, u) u {u i } i }, then its computation is irrelevant. Use qhull to reduce the number of samples. In large-scale problems most of the computation time is spent calculating f ( x 0 (t), u i ) for each of the samples. Use an l 1 regularizer to force sparsity on the set {ω i (t)} i. If smoothness is desirable, then use an l 2 regularizer and a large number of samples. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 21
44 Numerical Considerations Note that if f(x, u k ) lays strictly in the relative interior of co{f(x, u) u {u i } i }, then its computation is irrelevant. Use qhull to reduce the number of samples. In large-scale problems most of the computation time is spent calculating f ( x 0 (t), u i ) for each of the samples. Use an l 1 regularizer to force sparsity on the set {ω i (t)} i. If smoothness is desirable, then use an l 2 regularizer and a large number of samples. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 21
45 Numerical Considerations Note that if f(x, u k ) lays strictly in the relative interior of co{f(x, u) u {u i } i }, then its computation is irrelevant. Use qhull to reduce the number of samples. In large-scale problems most of the computation time is spent calculating f ( x 0 (t), u i ) for each of the samples. Use an l 1 regularizer to force sparsity on the set {ω i (t)} i. If smoothness is desirable, then use an l 2 regularizer and a large number of samples. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 21
46 Numerical Considerations Note that if f(x, u k ) lays strictly in the relative interior of co{f(x, u) u {u i } i }, then its computation is irrelevant. Use qhull to reduce the number of samples. In large-scale problems most of the computation time is spent calculating f ( x 0 (t), u i ) for each of the samples. Use an l 1 regularizer to force sparsity on the set {ω i (t)} i. If smoothness is desirable, then use an l 2 regularizer and a large number of samples. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 21
47 Numerical Considerations Note that if f(x, u k ) lays strictly in the relative interior of co{f(x, u) u {u i } i }, then its computation is irrelevant. Use qhull to reduce the number of samples. In large-scale problems most of the computation time is spent calculating f ( x 0 (t), u i ) for each of the samples. Use an l 1 regularizer to force sparsity on the set {ω i (t)} i. If smoothness is desirable, then use an l 2 regularizer and a large number of samples. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 21
48 1. Critical Point Characterization 2. Synthesis of Optimal Control Inputs 3. Simulation: Optimal HVAC Operation Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 22
49 Comprehensive Building Operation Besides controlling the HVAC unit in a building, we can make suggestions to the occupants regarding door configuration to improve efficiency and comfort. d 3 h 2 s 2 h 4 d 4 s 3 d 2 d 1 s 1 h 3 h 1 Let θ {0, 1} 4, where θ i = 1 if i-th door is open. Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 23
50 CFD Model Heat convection-diffusion: T e t (x, t) x (κ(x, θ) x T e (x, t))+ + u(x) x T e (x, t) = g Te (x, t), Stationary imcompressible Navier-Stokes: 1 Re xu(x) + ( u(x) x ) u(x)+ + x p(x) + α(x, θ) u(x) = g u (x), u = 0 Initial condition: T e (x, 0) = π 0, Boundary conditions: T e (t, x) = 0, and u(x) = 0, x Ω R. He and H. Gonzalez, Zoned HVAC Control via PDE-Constrained Optimization, in Proceedings of the 2016 american control conference, arxiv: R. He and H. Gonzalez, Gradient-Based Estimation of Air Flow and Geometry Configurations in a Building Using Fluid Dynamic Adjoint Equations, in Proceedings of the 4th international high performance buildings conference at purdue, arxiv: Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 24
51 Critical Point Characterization Synthesis of Optimal Control Inputs Simulation: Optimal HVAC Operation Single Zone Control Closed doors: Open doors: 4.8 d3 h4 d4 h2 d2 d h3 4.8 d3 4.0 target h4 d4 d2 0.8 h3 target ms Sampling-Based Optimal Control Synthesis 4.0 d h1 h2 1.6 h ms ESE, Washington Univ. in St. Louis 25
52 Critical Point Characterization Synthesis of Optimal Control Inputs Simulation: Optimal HVAC Operation Dual Zone Control Closed doors: target h4 d4 d3 h3 h2 d2 d1 target h1 0.5 ms Sampling-Based Optimal Control Synthesis Open doors: target h4 d4 d3 h3 h2 d2 d1 target h ms ESE, Washington Univ. in St. Louis 26
53 There is nothing so practical as a good theory Kurt Lewin Sampling-Based Optimal Control Synthesis ESE, Washington Univ. in St. Louis 27
An Integral-type Constraint Qualification for Optimal Control Problems with State Constraints
An Integral-type Constraint Qualification for Optimal Control Problems with State Constraints S. Lopes, F. A. C. C. Fontes and M. d. R. de Pinho Officina Mathematica report, April 4, 27 Abstract Standard
More informationLecture Note 13:Continuous Time Switched Optimal Control: Embedding Principle and Numerical Algorithms
ECE785: Hybrid Systems:Theory and Applications Lecture Note 13:Continuous Time Switched Optimal Control: Embedding Principle and Numerical Algorithms Wei Zhang Assistant Professor Department of Electrical
More informationEuler Equations: local existence
Euler Equations: local existence Mat 529, Lesson 2. 1 Active scalars formulation We start with a lemma. Lemma 1. Assume that w is a magnetization variable, i.e. t w + u w + ( u) w = 0. If u = Pw then u
More informationarxiv: v4 [math.oc] 30 Apr 2016
Zoned HVAC Control via PDE-Constrained Optimization Runxin He Humberto Gonzalez arxiv:1504.04680v4 [math.oc] 30 Apr 2016 Abstract Efficiency, comfort, and convenience are three major aspects in the design
More informationOn Weak Topology for Optimal Control of. Switched Nonlinear Systems
On Weak Topology for Optimal Control of 1 Switched Nonlinear Systems Hua Chen and Wei Zhang arxiv:1409.6000v3 [math.oc] 24 Mar 2015 Abstract Optimal control of switched systems is challenging due to the
More informationEE291E/ME 290Q Lecture Notes 8. Optimal Control and Dynamic Games
EE291E/ME 290Q Lecture Notes 8. Optimal Control and Dynamic Games S. S. Sastry REVISED March 29th There exist two main approaches to optimal control and dynamic games: 1. via the Calculus of Variations
More informationReflected Brownian Motion
Chapter 6 Reflected Brownian Motion Often we encounter Diffusions in regions with boundary. If the process can reach the boundary from the interior in finite time with positive probability we need to decide
More informationMean field games and related models
Mean field games and related models Fabio Camilli SBAI-Dipartimento di Scienze di Base e Applicate per l Ingegneria Facoltà di Ingegneria Civile ed Industriale Email: Camilli@dmmm.uniroma1.it Web page:
More informationGradient-Based Estimation of Air Flow and Geometry Configurations in a Building Using Fluid Dynamic Adjoint Equations
Purdue University Purdue e-pubs International High Performance Buildings Conference School of Mechanical Engineering 2016 Gradient-Based Estimation of Air Flow and Geometry Configurations in a Building
More informationElectronic Companion to Optimal Policies for a Dual-Sourcing Inventory Problem with Endogenous Stochastic Lead Times
e-companion to Song et al.: Dual-Sourcing with Endogenous Stochastic Lead times ec1 Electronic Companion to Optimal Policies for a Dual-Sourcing Inventory Problem with Endogenous Stochastic Lead Times
More informationDiscontinuous Galerkin Methods
Discontinuous Galerkin Methods Joachim Schöberl May 20, 206 Discontinuous Galerkin (DG) methods approximate the solution with piecewise functions (polynomials), which are discontinuous across element interfaces.
More informationMinimal periods of semilinear evolution equations with Lipschitz nonlinearity
Minimal periods of semilinear evolution equations with Lipschitz nonlinearity James C. Robinson a Alejandro Vidal-López b a Mathematics Institute, University of Warwick, Coventry, CV4 7AL, U.K. b Departamento
More informationPontryagin s Minimum Principle 1
ECE 680 Fall 2013 Pontryagin s Minimum Principle 1 In this handout, we provide a derivation of the minimum principle of Pontryagin, which is a generalization of the Euler-Lagrange equations that also includes
More informationOn John type ellipsoids
On John type ellipsoids B. Klartag Tel Aviv University Abstract Given an arbitrary convex symmetric body K R n, we construct a natural and non-trivial continuous map u K which associates ellipsoids to
More informationPOD for Parametric PDEs and for Optimality Systems
POD for Parametric PDEs and for Optimality Systems M. Kahlbacher, K. Kunisch, H. Müller and S. Volkwein Institute for Mathematics and Scientific Computing University of Graz, Austria DMV-Jahrestagung 26,
More informationNeighboring feasible trajectories in infinite dimension
Neighboring feasible trajectories in infinite dimension Marco Mazzola Université Pierre et Marie Curie (Paris 6) H. Frankowska and E. M. Marchini Control of State Constrained Dynamical Systems Padova,
More informationA generalised Ladyzhenskaya inequality and a coupled parabolic-elliptic problem
A generalised Ladyzhenskaya inequality and a coupled parabolic-elliptic problem Dave McCormick joint work with James Robinson and José Rodrigo Mathematics and Statistics Centre for Doctoral Training University
More informationThe HJB-POD approach for infinite dimensional control problems
The HJB-POD approach for infinite dimensional control problems M. Falcone works in collaboration with A. Alla, D. Kalise and S. Volkwein Università di Roma La Sapienza OCERTO Workshop Cortona, June 22,
More informationThe Relativistic Heat Equation
Maximum Principles and Behavior near Absolute Zero Washington University in St. Louis ARTU meeting March 28, 2014 The Heat Equation The heat equation is the standard model for diffusion and heat flow,
More informationOn a Class of Multidimensional Optimal Transportation Problems
Journal of Convex Analysis Volume 10 (2003), No. 2, 517 529 On a Class of Multidimensional Optimal Transportation Problems G. Carlier Université Bordeaux 1, MAB, UMR CNRS 5466, France and Université Bordeaux
More informationLinear conic optimization for nonlinear optimal control
Linear conic optimization for nonlinear optimal control Didier Henrion 1,2,3, Edouard Pauwels 1,2 Draft of July 15, 2014 Abstract Infinite-dimensional linear conic formulations are described for nonlinear
More informationGradient Sampling for Improved Action Selection and Path Synthesis
Gradient Sampling for Improved Action Selection and Path Synthesis Ian M. Mitchell Department of Computer Science The University of British Columbia November 2016 mitchell@cs.ubc.ca http://www.cs.ubc.ca/~mitchell
More informationDeterministic Dynamic Programming
Deterministic Dynamic Programming 1 Value Function Consider the following optimal control problem in Mayer s form: V (t 0, x 0 ) = inf u U J(t 1, x(t 1 )) (1) subject to ẋ(t) = f(t, x(t), u(t)), x(t 0
More informationSingular solutions for vibration control problems
Journal of Physics: Conference Series PAPER OPEN ACCESS Singular solutions for vibration control problems To cite this article: Larisa Manita and Mariya Ronzhina 8 J. Phys.: Conf. Ser. 955 3 View the article
More informationHEATING, Ventilation, and Air Conditioning (HVAC)
1 Comfort-Aware Building Climate Control Using Distributed-Parameter Models Runxin He, Student Member, IEEE, and Humberto Gonzalez, Member, IEEE arxiv:1708.08495v1 [math.oc] 8 Aug 017 Abstract Controlling
More informationAffine covariant Semi-smooth Newton in function space
Affine covariant Semi-smooth Newton in function space Anton Schiela March 14, 2018 These are lecture notes of my talks given for the Winter School Modern Methods in Nonsmooth Optimization that was held
More informationDifferential Games II. Marc Quincampoix Université de Bretagne Occidentale ( Brest-France) SADCO, London, September 2011
Differential Games II Marc Quincampoix Université de Bretagne Occidentale ( Brest-France) SADCO, London, September 2011 Contents 1. I Introduction: A Pursuit Game and Isaacs Theory 2. II Strategies 3.
More informationMath background. Physics. Simulation. Related phenomena. Frontiers in graphics. Rigid fluids
Fluid dynamics Math background Physics Simulation Related phenomena Frontiers in graphics Rigid fluids Fields Domain Ω R2 Scalar field f :Ω R Vector field f : Ω R2 Types of derivatives Derivatives measure
More informationOn the Bellman equation for control problems with exit times and unbounded cost functionals 1
On the Bellman equation for control problems with exit times and unbounded cost functionals 1 Michael Malisoff Department of Mathematics, Hill Center-Busch Campus Rutgers University, 11 Frelinghuysen Road
More information1 Lyapunov theory of stability
M.Kawski, APM 581 Diff Equns Intro to Lyapunov theory. November 15, 29 1 1 Lyapunov theory of stability Introduction. Lyapunov s second (or direct) method provides tools for studying (asymptotic) stability
More informationFinite Convergence for Feasible Solution Sequence of Variational Inequality Problems
Mathematical and Computational Applications Article Finite Convergence for Feasible Solution Sequence of Variational Inequality Problems Wenling Zhao *, Ruyu Wang and Hongxiang Zhang School of Science,
More information1. Introduction. The Stokes problem seeks unknown functions u and p satisfying
A DISCRETE DIVERGENCE FREE WEAK GALERKIN FINITE ELEMENT METHOD FOR THE STOKES EQUATIONS LIN MU, JUNPING WANG, AND XIU YE Abstract. A discrete divergence free weak Galerkin finite element method is developed
More informationOPTIMAL CONVERGENCE RATES FOR THE COMPRESSIBLE NAVIER-STOKES EQUATIONS WITH POTENTIAL FORCES
OPTIMAL CONVERGENCE RATES FOR THE COMPRESSIBLE NAVIER-STOKES EQUATIONS WITH POTENTIAL FORCES RENJUN DUAN Department of Mathematics, City University of Hong Kong 83 Tat Chee Avenue, Kowloon, Hong Kong,
More informationA Numerical Method for the Optimal Control of Switched Systems
A Numerical Method for the Optimal Control of Switched Systems Humberto Gonzalez, Ram Vasudevan, Maryam Kamgarpour, S. Shankar Sastry, Ruzena Bajcsy, Claire Tomlin Abstract Switched dynamical systems have
More informationNumerical approximation for optimal control problems via MPC and HJB. Giulia Fabrini
Numerical approximation for optimal control problems via MPC and HJB Giulia Fabrini Konstanz Women In Mathematics 15 May, 2018 G. Fabrini (University of Konstanz) Numerical approximation for OCP 1 / 33
More informationReproducing Kernel Hilbert Spaces
Reproducing Kernel Hilbert Spaces Lorenzo Rosasco 9.520 Class 03 February 11, 2009 About this class Goal To introduce a particularly useful family of hypothesis spaces called Reproducing Kernel Hilbert
More informationIMPLEMENTATION OF A PARALLEL AMG SOLVER
IMPLEMENTATION OF A PARALLEL AMG SOLVER Tony Saad May 2005 http://tsaad.utsi.edu - tsaad@utsi.edu PLAN INTRODUCTION 2 min. MULTIGRID METHODS.. 3 min. PARALLEL IMPLEMENTATION PARTITIONING. 1 min. RENUMBERING...
More informationOn Pressure Stabilization Method and Projection Method for Unsteady Navier-Stokes Equations 1
On Pressure Stabilization Method and Projection Method for Unsteady Navier-Stokes Equations 1 Jie Shen Department of Mathematics, Penn State University University Park, PA 1682 Abstract. We present some
More informationVISCOSITY SOLUTIONS OF HAMILTON-JACOBI EQUATIONS, AND ASYMPTOTICS FOR HAMILTONIAN SYSTEMS
VISCOSITY SOLUTIONS OF HAMILTON-JACOBI EQUATIONS, AND ASYMPTOTICS FOR HAMILTONIAN SYSTEMS DIOGO AGUIAR GOMES U.C. Berkeley - CA, US and I.S.T. - Lisbon, Portugal email:dgomes@math.ist.utl.pt Abstract.
More informationESTIMATES FOR THE MONGE-AMPERE EQUATION
GLOBAL W 2,p ESTIMATES FOR THE MONGE-AMPERE EQUATION O. SAVIN Abstract. We use a localization property of boundary sections for solutions to the Monge-Ampere equation obtain global W 2,p estimates under
More informationarxiv: v1 [math.oc] 31 Jan 2017
CONVEX CONSTRAINED SEMIALGEBRAIC VOLUME OPTIMIZATION: APPLICATION IN SYSTEMS AND CONTROL 1 Ashkan Jasour, Constantino Lagoa School of Electrical Engineering and Computer Science, Pennsylvania State University
More informationRobust Stackelberg controllability for a heat equation Recent Advances in PDEs: Analysis, Numerics and Control
Robust Stackelberg controllability for a heat equation Recent Advances in PDEs: Analysis, Numerics and Control Luz de Teresa Víctor Hernández Santamaría Supported by IN102116 of DGAPA-UNAM Robust Control
More informationVariational approach to mean field games with density constraints
1 / 18 Variational approach to mean field games with density constraints Alpár Richárd Mészáros LMO, Université Paris-Sud (based on ongoing joint works with F. Santambrogio, P. Cardaliaguet and F. J. Silva)
More informationTHE CONVECTION DIFFUSION EQUATION
3 THE CONVECTION DIFFUSION EQUATION We next consider the convection diffusion equation ɛ 2 u + w u = f, (3.) where ɛ>. This equation arises in numerous models of flows and other physical phenomena. The
More informationL 2 -induced Gains of Switched Systems and Classes of Switching Signals
L 2 -induced Gains of Switched Systems and Classes of Switching Signals Kenji Hirata and João P. Hespanha Abstract This paper addresses the L 2-induced gain analysis for switched linear systems. We exploit
More informationSimultaneous Robust Design and Tolerancing of Compressor Blades
Simultaneous Robust Design and Tolerancing of Compressor Blades Eric Dow Aerospace Computational Design Laboratory Department of Aeronautics and Astronautics Massachusetts Institute of Technology GTL Seminar
More informationConservative Control Systems Described by the Schrödinger Equation
Conservative Control Systems Described by the Schrödinger Equation Salah E. Rebiai Abstract An important subclass of well-posed linear systems is formed by the conservative systems. A conservative system
More information3 Generation and diffusion of vorticity
Version date: March 22, 21 1 3 Generation and diffusion of vorticity 3.1 The vorticity equation We start from Navier Stokes: u t + u u = 1 ρ p + ν 2 u 1) where we have not included a term describing a
More informationAccelerated Proximal Gradient Methods for Convex Optimization
Accelerated Proximal Gradient Methods for Convex Optimization Paul Tseng Mathematics, University of Washington Seattle MOPTA, University of Guelph August 18, 2008 ACCELERATED PROXIMAL GRADIENT METHODS
More informationImplicit Euler Numerical Simulation of Sliding Mode Systems
Implicit Euler Numerical Simulation of Sliding Mode Systems Vincent Acary and Bernard Brogliato, INRIA Grenoble Rhône-Alpes Conference in honour of E. Hairer s 6th birthday Genève, 17-2 June 29 Objectives
More informationA maximum principle for optimal control system with endpoint constraints
Wang and Liu Journal of Inequalities and Applications 212, 212: http://www.journalofinequalitiesandapplications.com/content/212/231/ R E S E A R C H Open Access A maimum principle for optimal control system
More informationJoint work with Nguyen Hoang (Univ. Concepción, Chile) Padova, Italy, May 2018
EXTENDED EULER-LAGRANGE AND HAMILTONIAN CONDITIONS IN OPTIMAL CONTROL OF SWEEPING PROCESSES WITH CONTROLLED MOVING SETS BORIS MORDUKHOVICH Wayne State University Talk given at the conference Optimization,
More informationLecture Note III: Least-Squares Method
Lecture Note III: Least-Squares Method Zhiqiang Cai October 4, 004 In this chapter, we shall present least-squares methods for second-order scalar partial differential equations, elastic equations of solids,
More informationAMS subject classifications. Primary, 65N15, 65N30, 76D07; Secondary, 35B45, 35J50
A SIMPLE FINITE ELEMENT METHOD FOR THE STOKES EQUATIONS LIN MU AND XIU YE Abstract. The goal of this paper is to introduce a simple finite element method to solve the Stokes equations. This method is in
More informationConvex Optimization in Computer Vision:
Convex Optimization in Computer Vision: Segmentation and Multiview 3D Reconstruction Yiyong Feng and Daniel P. Palomar The Hong Kong University of Science and Technology (HKUST) ELEC 5470 - Convex Optimization
More informationDesign of optimal RF pulses for NMR as a discrete-valued control problem
Design of optimal RF pulses for NMR as a discrete-valued control problem Christian Clason Faculty of Mathematics, Universität Duisburg-Essen joint work with Carla Tameling (Göttingen) and Benedikt Wirth
More informationAbout the minimal time crisis problem and applications
About the minimal time crisis problem and applications Térence Bayen, Alain Rapaport To cite this version: Térence Bayen, Alain Rapaport. About the minimal time crisis problem and applications. IFAC Word
More informationScientific Data Computing: Lecture 3
Scientific Data Computing: Lecture 3 Benson Muite benson.muite@ut.ee 23 April 2018 Outline Monday 10-12, Liivi 2-207 Monday 12-14, Liivi 2-205 Topics Introduction, statistical methods and their applications
More informationDissipative quasi-geostrophic equations with L p data
Electronic Journal of Differential Equations, Vol. (), No. 56, pp. 3. ISSN: 7-669. URL: http://ejde.math.swt.edu or http://ejde.math.unt.edu ftp ejde.math.swt.edu (login: ftp) Dissipative quasi-geostrophic
More informationFundamentals of Fluid Dynamics: Ideal Flow Theory & Basic Aerodynamics
Fundamentals of Fluid Dynamics: Ideal Flow Theory & Basic Aerodynamics Introductory Course on Multiphysics Modelling TOMASZ G. ZIELIŃSKI (after: D.J. ACHESON s Elementary Fluid Dynamics ) bluebox.ippt.pan.pl/
More information1 Brownian Local Time
1 Brownian Local Time We first begin by defining the space and variables for Brownian local time. Let W t be a standard 1-D Wiener process. We know that for the set, {t : W t = } P (µ{t : W t = } = ) =
More informationImproved Action Selection and Path Synthesis using Gradient Sampling
Improved Action Selection and Path Synthesis using Gradient Sampling Neil Traft and Ian M. Mitchell Department of Computer Science The University of British Columbia December 2016 ntraft@cs.ubc.ca mitchell@cs.ubc.ca
More informationWeak solutions to the stationary incompressible Euler equations
Weak solutions to the stationary incompressible Euler equations Antoine Choffrut September 29, 2014 University of Sussex Analysis & PDEs Seminar Euler s equations (1757) Motivation Conservation of energy
More informationTHE STOKES SYSTEM R.E. SHOWALTER
THE STOKES SYSTEM R.E. SHOWALTER Contents 1. Stokes System 1 Stokes System 2 2. The Weak Solution of the Stokes System 3 3. The Strong Solution 4 4. The Normal Trace 6 5. The Mixed Problem 7 6. The Navier-Stokes
More informationA RECURRENCE THEOREM ON THE SOLUTIONS TO THE 2D EULER EQUATION
ASIAN J. MATH. c 2009 International Press Vol. 13, No. 1, pp. 001 006, March 2009 001 A RECURRENCE THEOREM ON THE SOLUTIONS TO THE 2D EULER EQUATION Y. CHARLES LI Abstract. In this article, I will prove
More informationBlow-up for a Nonlocal Nonlinear Diffusion Equation with Source
Revista Colombiana de Matemáticas Volumen 46(2121, páginas 1-13 Blow-up for a Nonlocal Nonlinear Diffusion Equation with Source Explosión para una ecuación no lineal de difusión no local con fuente Mauricio
More informationRobustness for a Liouville type theorem in exterior domains
Robustness for a Liouville type theorem in exterior domains Juliette Bouhours 1 arxiv:1207.0329v3 [math.ap] 24 Oct 2014 1 UPMC Univ Paris 06, UMR 7598, Laboratoire Jacques-Louis Lions, F-75005, Paris,
More informationThe Orchestra of Partial Differential Equations. Adam Larios
The Orchestra of Partial Differential Equations Adam Larios 19 January 2017 Landscape Seminar Outline 1 Fourier Series 2 Some Easy Differential Equations 3 Some Not-So-Easy Differential Equations Outline
More informationTRANSPORT IN POROUS MEDIA
1 TRANSPORT IN POROUS MEDIA G. ALLAIRE CMAP, Ecole Polytechnique 1. Introduction 2. Main result in an unbounded domain 3. Asymptotic expansions with drift 4. Two-scale convergence with drift 5. The case
More informationExact controllability of the superlinear heat equation
Exact controllability of the superlinear heat equation Youjun Xu 1,2, Zhenhai Liu 1 1 School of Mathematical Sciences and Computing Technology, Central South University, Changsha, Hunan 410075, P R China
More informationConvexity of the Reachable Set of Nonlinear Systems under L 2 Bounded Controls
1 1 Convexity of the Reachable Set of Nonlinear Systems under L 2 Bounded Controls B.T.Polyak Institute for Control Science, Moscow, Russia e-mail boris@ipu.rssi.ru Abstract Recently [1, 2] the new convexity
More informationNumerical Solution of Heat Equation by Spectral Method
Applied Mathematical Sciences, Vol 8, 2014, no 8, 397-404 HIKARI Ltd, wwwm-hikaricom http://dxdoiorg/1012988/ams201439502 Numerical Solution of Heat Equation by Spectral Method Narayan Thapa Department
More informationhal , version 6-26 Dec 2012
ON THE UNIQUENESS IN THE 3D NAVIER-STOKES EQUATIONS ABDEHAFID YOUNSI Abstract. In this paper, we give a new regularity criterion on the uniqueness results of weak solutions for the 3D Navier-Stokes equations
More informationNumerical Optimal Control Overview. Moritz Diehl
Numerical Optimal Control Overview Moritz Diehl Simplified Optimal Control Problem in ODE path constraints h(x, u) 0 initial value x0 states x(t) terminal constraint r(x(t )) 0 controls u(t) 0 t T minimize
More informationMATH 819 FALL We considered solutions of this equation on the domain Ū, where
MATH 89 FALL. The D linear wave equation weak solutions We have considered the initial value problem for the wave equation in one space dimension: (a) (b) (c) u tt u xx = f(x, t) u(x, ) = g(x), u t (x,
More informationNumerical solution of nonlinear sine-gordon equation with local RBF-based finite difference collocation method
Numerical solution of nonlinear sine-gordon equation with local RBF-based finite difference collocation method Y. Azari Keywords: Local RBF-based finite difference (LRBF-FD), Global RBF collocation, sine-gordon
More informationNonlinear Model Predictive Control Tools (NMPC Tools)
Nonlinear Model Predictive Control Tools (NMPC Tools) Rishi Amrit, James B. Rawlings April 5, 2008 1 Formulation We consider a control system composed of three parts([2]). Estimator Target calculator Regulator
More informationFREE BOUNDARY PROBLEMS IN FLUID MECHANICS
FREE BOUNDARY PROBLEMS IN FLUID MECHANICS ANA MARIA SOANE AND ROUBEN ROSTAMIAN We consider a class of free boundary problems governed by the incompressible Navier-Stokes equations. Our objective is to
More informationSPACE AVERAGES AND HOMOGENEOUS FLUID FLOWS GEORGE ANDROULAKIS AND STAMATIS DOSTOGLOU
M P E J Mathematical Physics Electronic Journal ISSN 086-6655 Volume 0, 2004 Paper 4 Received: Nov 4, 2003, Revised: Mar 3, 2004, Accepted: Mar 8, 2004 Editor: R. de la Llave SPACE AVERAGES AND HOMOGENEOUS
More informationUNCERTAINTY FUNCTIONAL DIFFERENTIAL EQUATIONS FOR FINANCE
Surveys in Mathematics and its Applications ISSN 1842-6298 (electronic), 1843-7265 (print) Volume 5 (2010), 275 284 UNCERTAINTY FUNCTIONAL DIFFERENTIAL EQUATIONS FOR FINANCE Iuliana Carmen Bărbăcioru Abstract.
More informationp 1 ( Y p dp) 1/p ( X p dp) 1 1 p
Doob s inequality Let X(t) be a right continuous submartingale with respect to F(t), t 1 P(sup s t X(s) λ) 1 λ {sup s t X(s) λ} X + (t)dp 2 For 1 < p
More informationAn Optimal Control Approach to Sensor / Actuator Placement for Optimal Control of High Performance Buildings
Purdue University Purdue e-pubs International High Performance Buildings Conference School of Mechanical Engineering 01 An Optimal Control Approach to Sensor / Actuator Placement for Optimal Control of
More informationA Lévy-Fokker-Planck equation: entropies and convergence to equilibrium
1/ 22 A Lévy-Fokker-Planck equation: entropies and convergence to equilibrium I. Gentil CEREMADE, Université Paris-Dauphine International Conference on stochastic Analysis and Applications Hammamet, Tunisia,
More informationPHYSICS 234 HOMEWORK 2 SOLUTIONS. So the eigenvalues are 1, 2, 4. To find the eigenvector for ω = 1 we have b c.
PHYSICS 34 HOMEWORK SOUTIONS.8.. The matrix we have to diagonalize is Ω 3 ( 4 So the characteristic equation is ( ( ω(( ω(4 ω. So the eigenvalues are,, 4. To find the eigenvector for ω we have 3 a (3 b
More informationTonelli Full-Regularity in the Calculus of Variations and Optimal Control
Tonelli Full-Regularity in the Calculus of Variations and Optimal Control Delfim F. M. Torres delfim@mat.ua.pt Department of Mathematics University of Aveiro 3810 193 Aveiro, Portugal http://www.mat.ua.pt/delfim
More informationA generalized forward-backward method for solving split equality quasi inclusion problems in Banach spaces
Available online at www.isr-publications.com/jnsa J. Nonlinear Sci. Appl., 10 (2017), 4890 4900 Research Article Journal Homepage: www.tjnsa.com - www.isr-publications.com/jnsa A generalized forward-backward
More informationAlberto Bressan. Department of Mathematics, Penn State University
Non-cooperative Differential Games A Homotopy Approach Alberto Bressan Department of Mathematics, Penn State University 1 Differential Games d dt x(t) = G(x(t), u 1(t), u 2 (t)), x(0) = y, u i (t) U i
More informationInput to state set stability for pulse width modulated control systems with disturbances
Input to state set stability for pulse width modulated control systems with disturbances A.R.eel and L. Moreau and D. Nešić Abstract New results on set stability and input-to-state stability in pulse-width
More informationConvergence and Error Bound Analysis for the Space-Time CESE Method
Convergence and Error Bound Analysis for the Space-Time CESE Method Daoqi Yang, 1 Shengtao Yu, Jennifer Zhao 3 1 Department of Mathematics Wayne State University Detroit, MI 480 Department of Mechanics
More informationCHAPTER 3 THE MAXIMUM PRINCIPLE: MIXED INEQUALITY CONSTRAINTS. p. 1/73
CHAPTER 3 THE MAXIMUM PRINCIPLE: MIXED INEQUALITY CONSTRAINTS p. 1/73 THE MAXIMUM PRINCIPLE: MIXED INEQUALITY CONSTRAINTS Mixed Inequality Constraints: Inequality constraints involving control and possibly
More informationContinuous methods for numerical linear algebra problems
Continuous methods for numerical linear algebra problems Li-Zhi Liao (http://www.math.hkbu.edu.hk/ liliao) Department of Mathematics Hong Kong Baptist University The First International Summer School on
More informationValue Function in deterministic optimal control : sensitivity relations of first and second order
Séminaire de Calcul Scientifique du CERMICS Value Function in deterministic optimal control : sensitivity relations of first and second order Hélène Frankowska (IMJ-PRG) 8mars2018 Value Function in deterministic
More informationRobust error estimates for regularization and discretization of bang-bang control problems
Robust error estimates for regularization and discretization of bang-bang control problems Daniel Wachsmuth September 2, 205 Abstract We investigate the simultaneous regularization and discretization of
More informationAdaptive Nonlinear Model Predictive Control with Suboptimality and Stability Guarantees
Adaptive Nonlinear Model Predictive Control with Suboptimality and Stability Guarantees Pontus Giselsson Department of Automatic Control LTH Lund University Box 118, SE-221 00 Lund, Sweden pontusg@control.lth.se
More informationNumerical methods for Mean Field Games: additional material
Numerical methods for Mean Field Games: additional material Y. Achdou (LJLL, Université Paris-Diderot) July, 2017 Luminy Convergence results Outline 1 Convergence results 2 Variational MFGs 3 A numerical
More informationb) The system of ODE s d x = v(x) in U. (2) dt
How to solve linear and quasilinear first order partial differential equations This text contains a sketch about how to solve linear and quasilinear first order PDEs and should prepare you for the general
More informationSTRUCTURAL OPTIMIZATION BY THE LEVEL SET METHOD
Shape optimization 1 G. Allaire STRUCTURAL OPTIMIZATION BY THE LEVEL SET METHOD G. ALLAIRE CMAP, Ecole Polytechnique with F. JOUVE and A.-M. TOADER 1. Introduction 2. Setting of the problem 3. Shape differentiation
More informationNumerical simulations and mesh adaptation : exercise sessions Charles Dapogny 1, Pascal Frey 2, Yannick Privat 2
Numerical simulations and mesh adaptation : exercise sessions Charles Dapogny Pascal Frey 2 Yannick Privat 2 The purpose of this exercise session is to give an overview of several aspects of scientific
More informationSOR- and Jacobi-type Iterative Methods for Solving l 1 -l 2 Problems by Way of Fenchel Duality 1
SOR- and Jacobi-type Iterative Methods for Solving l 1 -l 2 Problems by Way of Fenchel Duality 1 Masao Fukushima 2 July 17 2010; revised February 4 2011 Abstract We present an SOR-type algorithm and a
More informationA few words about the MTW tensor
A few words about the Ma-Trudinger-Wang tensor Université Nice - Sophia Antipolis & Institut Universitaire de France Salah Baouendi Memorial Conference (Tunis, March 2014) The Ma-Trudinger-Wang tensor
More information