A new approach to explicit MPC using self-optimizing control

Size: px
Start display at page:

Download "A new approach to explicit MPC using self-optimizing control"

Transcription

1 28 American Control Conference Westin Seattle Hotel, Seattle, Washington, USA June -3, 28 WeA3.2 A new approach to explicit MPC using self-optimizing control Henrik Manum, Sriharakumar Narasimhan an Sigur Skogesta Abstract Moel preictive control (MPC) is a favore metho for hanling constraine linear control problems. Normally, the MPC optimization problem is solve on-line, but in explicit MPC an explicit piecewise affine feeback law is compute an implemente ]. This approach is similar to self-optimizing control, where the iea is to fin simple pre-compute policies for implementing optimal operation, for example, by keeping selecte controlle variable combinations c constant. The nullspace metho 2] generates optimal variable combinations, which turn out to be equivalent to the explicit MPC feeback laws, that is, c = u Kx, where K is the optimal state feeback matrix in a given region. More importantly, this link gives new insights an also some new results. One is that regions changes may be ientifie by tracking the variables c for neighboring regions. I. INTRODUCTION Consier the general static optimization problem 2]: min J (x,u,) u,x s.t. f i (x,u,) =, i E h i (x,u,), i I, (P) where x R nx are the states, u R nu are the inputs, an D R n are isturbances. By iscretization an reformulation this may also represent some ynamic optimization problems. Usually f is a moel of the physical system, whilst h is a set of inequality constraints that limits the operation (e.g., physical limits on temperature measurements or flow constraints). In aition to (P) we have measurements on the form y = f y (x,u,). () In this work the emphasis is on implementation of the solution to (P). This means that the optimization problem (P) is solve off-line to generate a control policy which is suitable for on-line implementation, with particular emphasis on remaining close to optimal solution when there are unknown isturbances. That is, we search for control policies such that the cost J remains optimal or close to optimal when isturbances occur without the nee to reoptimize. A. Self-optimizing control In our previous work on self-optimizing control we have looke for simple control policies to implement optimal operation, an in particular what shoul we control (choice of controlle variables (CV s)). Using off-line optimization Department of Chemical Engineering, Norwegian University of Science an Technology, N-749 Tronheim, Norway. Author to whom corresponence shoul be aresse. skoge@ntnu.no we may etermine regions where ifferent sets of active constraints are active, an implementation of optimal operation is then in each region to: ) Control the active constraints. 2) For the remaining unconstraine egrees of freeom: Control self-optimizing variables c = Hy which have the property that keeping them constant (c = c s ) inirectly achieves close-to optimal operation (with a small loss), in spite of isturbances. We here allow for linear measurement combinations, c = Hy. There are here two factors that shoul be consiere: a) Disturbances. Ieally, we want the optimal value of c (c opt ) to be inepenent of. b) Measurements errors n y. The loss shoul be insensitive to these. B. Relationship to explicit MPC Consier a simple static optimization problem min u J(u,), where u are the unconstraine egrees of freeom an the states x an the active constraints have been eliminate by substitution. For the quaratic case J(u,) = u ] T Su ] ] Juu J where S = u. J u T J In aition we have available measurements y = G y u+ G. A key result, which is the basis for this paper, is For a quaratic optimization problem there exists (infinitely many) linear measurement combinations c = Hy that are optimally invariant to isturbances. One sees immeiately that there may be some link to explicit MPC, because the iscrete form MPC problem can be written as a static quaratic problem. The link is: If we let y contain the inputs u an the states x, then the selfoptimizing variable combination c = Hy is the same as the explicit MPC feeback law (control policy), i.e. c = u Kx. (This is shown in section III.) Base on this, we provie in this contribution some new ieas on explicit MPC: ) We propose that tracking the variables c (eviation from optimal feeback law) for all regions, may be use as a local metho to etect when to switch between regions. 2) We may use our results to inclue measurement error in y (e.g. in x an u) when eriving the optimal explicit MPC. 3) We may exten the results to output feeback (c = u Ky) by incluing in y present an past outputs (an not present states x). (2) /8/$ AACC. 435

2 Off-line Optimizer c s Feeback Controller u c + n y m n c Measurement combination (H) Process y (G y,g y ) ny Fig.. Block iagram of a feeback control structure incluing an optimization layer 4]. 4) We can also exten the results to the case where only a subset of the states are measure (but in this case there will be a loss, which we can quantify). This may be of interest even in the unconstraine LQ case. In this paper the basic framework an issue () are iscusse. In 3] it is shown how the results can be extene to hanle items (2)-(4), both with theorems an examples. II. RESULTS FROM SELF-OPTIMIZING CONTROL A. Steay state conitions Once the set of active constraints in (P) is known we can form the reuce problem an the unconstraine egrees of freeom u can be etermine. The unconstraine measurements are y = G y u + G y, (3) an y contain information about the present state an isturbances (y may inclue u an, but not the active constraints.) The (measure) value of y m available for implementation is y m = y + n y, (4) where n y represents uncertainty in the measurement of y incluing uncertainty of implementation in u. The following theorem escribes a metho to fin linear invariants that yiels zero loss from optimality when the invariants are controlle at constant setpoint. The theorem is base on the nullspace metho presente in 2]. Figure illustrates how the H matrix is use to linearly combine measurements (an square own the plant). Theorem : (Linear invariants for quaratic optimization problem 4]) Consier an unconstraine quaratic optimization problem in the variables u (input vector of length n u ) an (isturbance vector of length n ) min u J(u,) = u ] Juu J u J u T J ] u ] (5) In aition, there are measurement variables y = G y u + G y. If there exists n y n u + n inepenent measurements (where inepenent means that the matrix G y = G y G y ] has full rank), then the optimal solution to (5) has the property that there exists n c = n u linear variable combinations (constraints) c = Hy that are invariant to the isturbances. The optimal measurement combination matrix H is foun by either: (): Let F = yopt T be the optimal sensitivity matrix evaluate with constant active constraints. Uner the assumptions state above possible to select the matrix H in the left nullspace of F, H N(F T ), such that (2): If n y = n u + n : HF = (6) H = Mn J( G y ), (7) where J ] = Juu /2 Juu /2 J u an G y = G y G y ] is the augmente plant. Mn may be seen as a free parameter. (Note that M n = J cc is the Hessian of the cost with respect to the c-variables; in most cases we select M n = I for convenience.) Remark : The sensitivity F matrix can be obtaine from F = ( G y Juu J u G y ). (8) Remark 2: An equivalent formulation is: Assume that there exists a set of inepenent measurements y an that the (operational) constraint c Hy = c s (where c s is a constant) is ae to the problem. Then there exists an H that oes not change the solution to (5). In terms of operation, this means that zero loss (optimal operation) is obtaine by controlling n c = n u variables c = Hy with a constant set-point policy c = c s, where H is selecte accoring to theorem. Theorem may be extene: Lemma : (Linear invariants for constraine quaratic optimization methos) Consier an optimization problem of the form min J = x u ] S x u u,x s.t. Ax + Bu + C = Ãx + Bu + C, with et(a) an à B] full row rank. Assume that the isturbance space has been partitione into n a critical regions. In each region there are n i u = n u n i A unconstraine egrees of freeom, where ni A n m is the number of optimally active constraints in region i. If there exists a set of inepenent unconstraine measurements y i = (G y ) i u i +(G y )i in each region i, such that n y i n u i + n, the optimal solution to (9) has the property that there exists variable combinations c i = H i y i that are invariant to the isturbances in the critical region i. The corresponing optimal H i may be obtaine from Theorem. (9) 436

3 Within each region, optimality requires that c i c i s = (where c i s is a constant). From continuity of the solution, we have that c i is continuous across the bounary of region i. This implies that the elements in the variable vector c i c i s will change sign or remain zero when crossing into or from a neighboring region. Proof: See internal report 5]. B. Implementation of optimal solution For the case of no measurement error, n y =, Theorem shows that for the solution to quaratic optimization problems, variable combinations c = Hy that are invariant to the isturbances can be foun. In section III this insight will be use as a new approach to the explicit MPC problem. III. APPLICATION TO EXPLICIT MPC We will now look at the moel preictive control problem (MPC) with constraints on inputs an outputs. For a iscussion on MPC in a unifie theoretical framework see 6]. The following iscrete MPC formulation is base on 7]. Consier the state-space representation of a given process moel: x(t + ) = Ax(t) + Bu(t) () subject to the following constraints: y (t) = Cx(t), () y min y (t) y max (2) u min u(t) u max, (3) where x(t) R n, u(t) R m, an y(t) R p are the state, input an output vectors, respectively, subscripts min an max enote the lower an upper bouns, respectively, an (A,B) is stabilizable. MPC problems for regulating to the origin can then be pose as the following optimization problem: min J(U,x(t)) = x t+n T y y Px U t+ny t+ + N y k= xt+k t T Qx t+k t + u t+k T Ru t+k ] s.t. y min y t+k t y max, u min u t+k u max, x t t = x(t) k =,...,N c k =,,...,N c x t+k+ t = Ax t+k t + Bu t+k, k y t+k t = Cx t+k t, k u t+k = Kx t+k t, N u k N y where U {u t,...,u t+nu }, Q = Q T, R = R T >, P, N y N u, an K is some feeback gain. 7] show that by substitution of the moel equations, the problem can be rewritten on the form min U 2 U T HU + x(t) T FU + 2 x(t)t Y x(t) s.t. GU W + Ex(t) (4) The MPC control law is base on the following iea: At time t, compute the optimal solution U (t) = {u t,...,u t+n u } an apply u(t) = u t ]. Remark 3: The trae-off between robustness an performance is inclue in the weights in the MPC cost function an in the constraints. If we let the initial state x(t) be treate as a isturbance, (4) can be written as: min U 2 U T T] H F F Y s.t. GU W + E, ] ] U (5) an we observe that (5) is on the same form as (9), where the moel equations f(x,u,) = have alreay been substitute into the objective function. A property of the solution to (5) is that the isturbance space (initial state space) is ivie into critical regions. In the i th critical region there are n i u = n U n i A unconstraine egrees of freeom, where n i A is the number of active constraints in region i. As we iscuss in section III-A, a possible set of measurements y is the current state an the inputs, y T = x T u T]. We further note that causality is not an issue here, as we have the information at the current time. A. Exact measurements of all states (state feeback) The following theorem is well known, but we will here prove the theorem using the nullspace metho. Theorem 2: (Optimal state feeback ]) The control law u(t) = f(x(t)), f : R n R m, efine by the MPC problem, is continuous an piecewise affine f(x) = K i x + g i if H i x k i, i =,...,N mpc (6) { where the polyheral sets H i x k i}, i =,...,N mpc N r are a partition of the given set of states X. In this case causality is not a problem an from Theorem the optimal solution is simply u = Kx + g (i.e. c = u (Kx g)). Note that n = n x in this case. Proof: We consier the explicit MPC formulation as in (5). First we consier the unconstraine case. Let y = (U,x) be the set of caniate measurements. With this choice of measurements an isturbances on the present state, we form the process moel: y = G y U + G y (7) ] G y nx (n = un u) R (nx+nunu) (nunu) (8) I (nun u) (n un ] u) G y = Inx n x R (nx+nunu) nx. (9) (nun u) n x 437

4 We then get the optimal sensitivity as F = yopt T = ( G y Juu J u G y ) = (2) ( ] ]) nx (n un u) Inx n (Juu x (2) J u ) (nun u) n x (nun ] u) n x Inx n = x Juu (22) J u We now search for a matrix H that gives a non-trivial solution to HF = : ] ] I (H ) (nun u) n x (H 2 ) nx n x (nun u) (n un u) Juu = (23) J u ( ) = H H 2 J uu J u = (24) To ensure a non-trivial solution we can for example choose H 2 = I (nun u) n un u. Then we must have H = Juu J u, an hence the optimal combination c of x an U becomes c = Hy = J uu J u x + U = R (nunu) (25) In the internal report by 5] it is shown how the affine term in (6) enters as a function of the active constraints. Remark 4: (Comparison with previous results on unconstraine MPC) In (25) the state feeback gain matrix is given as Juu J u. This is gives the same result as conventional MPC, see equation (3) in 8]. Remark 5: These are not new results but the alternative proof leas to some new insights. The most important is probably that the self-optimizing variables c i = u (K i x+ g i ) which are optimally zero in region i, may be use for ientifying when to switch between regions (Theorem 3) rather than using a centralize approach, for example base on a state tree structure search. This seems to be new. Another insight is to unerstan why a simple feeback solution must exist in the first place. A thir is to allow for new extensions. Theorem 3: (Optimal region for explicit MPC etection using feeback law) The variables c = u k (Kx k + g) can be use to ientify region changes. Proof: See report by 5]. Remark 6: Neighboring regions with the same feeback law (incluing regions where the feeback law is to keep the input saturate) can be merge (provie that the regions remain convex or if the crossings insie a non-convex region ue to the optimal irection of the process in close loop only occurs in the convex part of the region). This may greatly reuce the number of regions compare to presently use enumeration schemes. Note that the number of c-variables that nee to be tracke to etect region changes is only equal to the number of inputs n u times the number of istinct merge regions. Because of the merging of regions, this may be a small number even with a large input or control horizon an with output (state) constraints. We present a simple example from ] that confirms that our switching policy base on tracking the sign of the c- variables works in practice. Algorithm Detect current region an calculate u k Require: CR k, i.e. the region of the last sample time, an x k : u k = K(CR k ) + g(cr k ) 2: Regions,α] = Neighbors(CR k ) 3: for i = to length(regions) o 4: c k (i) = α i (u k (K(Regions(i)) + g(regions(i)))) 5: en for 6: if sign(c k (i) ) then 7: CR k = Regions(i) 8: else 9: CR k = CR k : en if : return u k = K(CR k )x k + g(cr k ), CR k Example 3. (Optimal switching): This example is taken from ] (with correction), an is inclue here to emonstrate optimal switching using the sign change of c = u Kx as the criterion. The system is: y(t) = 2 s 2 + 3s + 2 u(t). With a sampling time T =. secons the following statespace representation is obtaine: ] ] x(t + ) = x(t) + u(t) y(t) =.442 ] x(t) One observes that only the last state is measure, but it will be assume that both states are known (measure) in the remainer of this example. The task is to regulate the system to the origin while fulfilling the input constraint 2 u(t) 2. (26) The objective function to be minimize is minx t+2 t T Px t+2 t + k= T xt+k t x t+k t +.u 2 ] t+k (27) subject to the constraints an x t t = x(t). P solves the Lyapunov equation P = A T PA + Q, where Q = I in this case. The optimal control problem can be solve for example using the MPT toolbox 9]. The P -matrix is numerically: ] P = To illustrate ieas a simulation from x = (,) was one. State space trajectories an inputs are shown in figures 2 an 3. As long as the state is in the input-constraine region where u opt = 2, the linear combination c = u k Kx k remains positive. One chooses to leave the input-constraine region when c k becomes zero. As one observes, this happens at time instant 8, where the process inee is on the bounary between the input-saturate region an the center region. 438

5 x u = 2 u = Kx u = x Fig. 2. Partition of state space for first input. (Example 3..) States x(t) Input u(t) c k = u k (Kx k ) Fig. 3. Close loop MPC with region etection using u k (Kx k ). (Example 3..) After the switching the controller for the center region is implemente. The state trajectory is the same as in ]. The reason for why c never becomes negative is because both states are assume measure at the present time an hence optimal switching is achieve. This can be unerstoo from the algorithm, where we show how the current critical region (CR k ) is tracke an how the current input u k is calculate. Example 3.2 (Double integrator): Consier the ouble integrator isusse by ], y(t) = /s 2 u(t), an its equivalent iscrete-time state-space representation, ] ] x k+ = x k + u k, y k = ] x k, which is obtaine by setting ÿ(t) = (ẏ(t + T s ) ẏ(t))/t s, x u = x 7 u = 8 9 Fig. 4. Regions for ouble integrator example (Example 3.2). ẏ(t) = (y(t + T s ) y(t))/t s, T s =. The control objective is to regulate the system to the origin while minimizing the quaratic cost funcion J = t= y(t)t y(t) + u2 subject to the input constraint u(t). The infinite horizion control problem can be converte to a finite horizion problem by solving ], ]: K LQ = (R + B T PB) B T PA, P = (A + BK LQ ) T P(A + BK LQ ) + K LQ T RK LQ + Q to obtain the unconstraine feeback gain K LQ an the final state weight matrix P (see example 3.). In this case we get K LQ = ] ] an P = For emonstration purposes we choose N u = 6, an by solving the paramteric program we get 73 regions initially. In this case there are regions of unsaturate control actions, which agrees with the general result of (2N u ) regions given in ]. Merging all regions where the first optimal input is the same, leaves us with the unsaturate regions, an two regions for which the optimal input is either at the high or low constraint. The final partitioning with 3 regions is shown in figure 4. We note that ] fin 57 regions after their merging scheme. Consiering figure 4 one observes that the input-saturate regions are non-convex. However, optimally, this process moves clockwise in the state space, an we observe that the non-convex crossings will not occur in practise. The remaing bounaries then form convex regions (inicate by the ashe lines in the figure.) Figure 5 shows the evolution of the invariants c i in each region when we start the simulation at x = (, 3) an close the loop by using the optimal inputs. We start in the input-saturate region u =, an nee to track the invariants for regions,2,3,4,5, an 6 to etermine optimal switching. We shoul switch to unsaturate control when one the variables c to c 6 becomes zero or changes sign. As one sees, this happens for c 3 at t = 6, so we change to this region. After using the feeback law for region 3 for one 439

6 c c 2 c 7 c 3 c c 4 c c 5 c 5 5 c 6 c Fig. 5. Invariants for ouble integrator example. sample time, we reach the other input constraint u = at t = 8. Now, to ecie when to leave this constraine region we track the invariants for regions,7,8,9,,, an we observe that at t = 9 the invariant for the center region becomes zero, hence we switch control to this region. Note that in this example, where we have only input constraine regions, the challenge is to ecie when to leave the input constraints. Note that the converse crossing can also be tracke using their invariants on the form c k = u k g. The iea of using irectionality (clockwise movement in this case) to reuce the number of reigons in explicit MPC can be generalize by using the irectional erivative of the process uner optimal control, (A BK i ), together with the normal vectors to the bounaries of the regions, an by some normalization scheme we remove all bounaries for which crossings uner optimal control will not occur. Here K i is the optimal feeback gain for region i. u regions, but we note that for some processes irectionality of the process in close loops implies that the non-convex crossings may be ignore. In a forthcoming contribution 3] we show how the results can be extene to output feeback an how to fin invariants that give minimal loss when controlle at constant set points also when we have noisy measurements. We further show how we one choose the orer of the controller an we show by examples that the resulting controller will have performance in the orer of magnitue of LQG controllers. The most important problem of using results from steay state self-optimizing control is causality, in steay state optimization all measurements are available at the current time (i.e. t ), but in ynamic optimization we may nee to fin invariants between measurements at current an future times an then switch the invariants back to get a casual controller, but this controller will be non-optimal by construction. Also this is iscusse in more etail in 3]. REFERENCES ] A. Bempora, M. Morari, V. Dua, an E. N. Pistikopoulos, The explicit linear quaratic regulator for constraine systems, Automatica, vol. 38, pp. 3 2, 22, see also corrigenum 39(23), pages ] V. Alsta an S. Skogesta, Null space metho for selecting optimal measurement combinations as controlle variables, In. Eng. Chem. Res, vol. 46, pp , 27. 3] H. Manum, S. Narasimhan, an S. Skogesta, Explicit MPC with output feeback using self-optimizing control, in Proceeings of IFAC Worl Conference, Seoul, Korea, 28. 4] V. Alsta, S. Skogesta, an E. Hori, Optimal measurement combinations as controlle variables, 28, in Press: Journal of Process Control, oi:.6/j.jprocont ] H. Manum, S. Narasimhan, an S. Skogesta, A new approach to explicit MPC using self-optimizing control, 27, avaliable at: 6] K. R. Muske an J. B. Rawlings, Moel preictive control with linear moels, AIChE Journal, vol. 39, pp , February ] E. N. Pistikopoulos, V. Dua, N. A. Bozinis, A. Bempora, an M. Morari, On-line optimization via off-line parametric optimization tools, Computers an Chemical Engineering, vol. 26, pp , 22. 8] J. B. Rawlings an K. R. Muske, The stability of constraine receing-horizon control, in IEEE Transactions on Automatic Control, vol. 38, 993, pp ] M. Kvasnica, P. Grieer, an M. Baotić, Multi-Parametric Toolbox (MPT), 24. Online]. Available: mpt/ ] D. Chmielewski an V. Manousiouthakis, On constraine infinitetime linear quaratic optimal control, Systems an Control Letters, vol. 29, pp. 2 29, 996. IV. DISCUSSION In this paper we have escribe the link between selfoptimizing control an explicit MPC. This link has been use to propose a new metho for etecting region changes. This new metho lets us reuce the number of regions by merging all regions for which the first input is the same. In its simple form presente in this paper, it oes not hanle non-convex 44

Nested Saturation with Guaranteed Real Poles 1

Nested Saturation with Guaranteed Real Poles 1 Neste Saturation with Guarantee Real Poles Eric N Johnson 2 an Suresh K Kannan 3 School of Aerospace Engineering Georgia Institute of Technology, Atlanta, GA 3332 Abstract The global stabilization of asymptotically

More information

BEYOND THE CONSTRUCTION OF OPTIMAL SWITCHING SURFACES FOR AUTONOMOUS HYBRID SYSTEMS. Mauro Boccadoro Magnus Egerstedt Paolo Valigi Yorai Wardi

BEYOND THE CONSTRUCTION OF OPTIMAL SWITCHING SURFACES FOR AUTONOMOUS HYBRID SYSTEMS. Mauro Boccadoro Magnus Egerstedt Paolo Valigi Yorai Wardi BEYOND THE CONSTRUCTION OF OPTIMAL SWITCHING SURFACES FOR AUTONOMOUS HYBRID SYSTEMS Mauro Boccaoro Magnus Egerstet Paolo Valigi Yorai Wari {boccaoro,valigi}@iei.unipg.it Dipartimento i Ingegneria Elettronica

More information

Calculus of Variations

Calculus of Variations 16.323 Lecture 5 Calculus of Variations Calculus of Variations Most books cover this material well, but Kirk Chapter 4 oes a particularly nice job. x(t) x* x*+ αδx (1) x*- αδx (1) αδx (1) αδx (1) t f t

More information

Experimental Robustness Study of a Second-Order Sliding Mode Controller

Experimental Robustness Study of a Second-Order Sliding Mode Controller Experimental Robustness Stuy of a Secon-Orer Sliing Moe Controller Anré Blom, Bram e Jager Einhoven University of Technology Department of Mechanical Engineering P.O. Box 513, 5600 MB Einhoven, The Netherlans

More information

Math Notes on differentials, the Chain Rule, gradients, directional derivative, and normal vectors

Math Notes on differentials, the Chain Rule, gradients, directional derivative, and normal vectors Math 18.02 Notes on ifferentials, the Chain Rule, graients, irectional erivative, an normal vectors Tangent plane an linear approximation We efine the partial erivatives of f( xy, ) as follows: f f( x+

More information

Systems & Control Letters

Systems & Control Letters Systems & ontrol Letters ( ) ontents lists available at ScienceDirect Systems & ontrol Letters journal homepage: www.elsevier.com/locate/sysconle A converse to the eterministic separation principle Jochen

More information

Optimal Variable-Structure Control Tracking of Spacecraft Maneuvers

Optimal Variable-Structure Control Tracking of Spacecraft Maneuvers Optimal Variable-Structure Control racking of Spacecraft Maneuvers John L. Crassiis 1 Srinivas R. Vaali F. Lanis Markley 3 Introuction In recent years, much effort has been evote to the close-loop esign

More information

Exponential Tracking Control of Nonlinear Systems with Actuator Nonlinearity

Exponential Tracking Control of Nonlinear Systems with Actuator Nonlinearity Preprints of the 9th Worl Congress The International Feeration of Automatic Control Cape Town, South Africa. August -9, Exponential Tracking Control of Nonlinear Systems with Actuator Nonlinearity Zhengqiang

More information

6 General properties of an autonomous system of two first order ODE

6 General properties of an autonomous system of two first order ODE 6 General properties of an autonomous system of two first orer ODE Here we embark on stuying the autonomous system of two first orer ifferential equations of the form ẋ 1 = f 1 (, x 2 ), ẋ 2 = f 2 (, x

More information

19 Eigenvalues, Eigenvectors, Ordinary Differential Equations, and Control

19 Eigenvalues, Eigenvectors, Ordinary Differential Equations, and Control 19 Eigenvalues, Eigenvectors, Orinary Differential Equations, an Control This section introuces eigenvalues an eigenvectors of a matrix, an iscusses the role of the eigenvalues in etermining the behavior

More information

Total Energy Shaping of a Class of Underactuated Port-Hamiltonian Systems using a New Set of Closed-Loop Potential Shape Variables*

Total Energy Shaping of a Class of Underactuated Port-Hamiltonian Systems using a New Set of Closed-Loop Potential Shape Variables* 51st IEEE Conference on Decision an Control December 1-13 212. Maui Hawaii USA Total Energy Shaping of a Class of Uneractuate Port-Hamiltonian Systems using a New Set of Close-Loop Potential Shape Variables*

More information

Math 342 Partial Differential Equations «Viktor Grigoryan

Math 342 Partial Differential Equations «Viktor Grigoryan Math 342 Partial Differential Equations «Viktor Grigoryan 6 Wave equation: solution In this lecture we will solve the wave equation on the entire real line x R. This correspons to a string of infinite

More information

Predictive Control of a Laboratory Time Delay Process Experiment

Predictive Control of a Laboratory Time Delay Process Experiment Print ISSN:3 6; Online ISSN: 367-5357 DOI:0478/itc-03-0005 Preictive Control of a aboratory ime Delay Process Experiment S Enev Key Wors: Moel preictive control; time elay process; experimental results

More information

Diagonalization of Matrices Dr. E. Jacobs

Diagonalization of Matrices Dr. E. Jacobs Diagonalization of Matrices Dr. E. Jacobs One of the very interesting lessons in this course is how certain algebraic techniques can be use to solve ifferential equations. The purpose of these notes is

More information

Optimal Control of Spatially Distributed Systems

Optimal Control of Spatially Distributed Systems Optimal Control of Spatially Distribute Systems Naer Motee an Ali Jababaie Abstract In this paper, we stuy the structural properties of optimal control of spatially istribute systems. Such systems consist

More information

Computing Exact Confidence Coefficients of Simultaneous Confidence Intervals for Multinomial Proportions and their Functions

Computing Exact Confidence Coefficients of Simultaneous Confidence Intervals for Multinomial Proportions and their Functions Working Paper 2013:5 Department of Statistics Computing Exact Confience Coefficients of Simultaneous Confience Intervals for Multinomial Proportions an their Functions Shaobo Jin Working Paper 2013:5

More information

Design A Robust Power System Stabilizer on SMIB Using Lyapunov Theory

Design A Robust Power System Stabilizer on SMIB Using Lyapunov Theory Design A Robust Power System Stabilizer on SMIB Using Lyapunov Theory Yin Li, Stuent Member, IEEE, Lingling Fan, Senior Member, IEEE Abstract This paper proposes a robust power system stabilizer (PSS)

More information

Switching Time Optimization in Discretized Hybrid Dynamical Systems

Switching Time Optimization in Discretized Hybrid Dynamical Systems Switching Time Optimization in Discretize Hybri Dynamical Systems Kathrin Flaßkamp, To Murphey, an Sina Ober-Blöbaum Abstract Switching time optimization (STO) arises in systems that have a finite set

More information

Adaptive Predictive Control with Controllers of Restricted Structure

Adaptive Predictive Control with Controllers of Restricted Structure Aaptive Preictive Control with Controllers of Restricte Structure Michael J Grimble an Peter Martin Inustrial Control Centre University of Strathclye 5 George Street Glasgow, G1 1QE Scotlan, UK Abstract

More information

State observers and recursive filters in classical feedback control theory

State observers and recursive filters in classical feedback control theory State observers an recursive filters in classical feeback control theory State-feeback control example: secon-orer system Consier the riven secon-orer system q q q u x q x q x x x x Here u coul represent

More information

Linear First-Order Equations

Linear First-Order Equations 5 Linear First-Orer Equations Linear first-orer ifferential equations make up another important class of ifferential equations that commonly arise in applications an are relatively easy to solve (in theory)

More information

Separation Principle for a Class of Nonlinear Feedback Systems Augmented with Observers

Separation Principle for a Class of Nonlinear Feedback Systems Augmented with Observers Proceeings of the 17th Worl Congress The International Feeration of Automatic Control Separation Principle for a Class of Nonlinear Feeback Systems Augmente with Observers A. Shiriaev, R. Johansson A.

More information

1 dx. where is a large constant, i.e., 1, (7.6) and Px is of the order of unity. Indeed, if px is given by (7.5), the inequality (7.

1 dx. where is a large constant, i.e., 1, (7.6) and Px is of the order of unity. Indeed, if px is given by (7.5), the inequality (7. Lectures Nine an Ten The WKB Approximation The WKB metho is a powerful tool to obtain solutions for many physical problems It is generally applicable to problems of wave propagation in which the frequency

More information

θ x = f ( x,t) could be written as

θ x = f ( x,t) could be written as 9. Higher orer PDEs as systems of first-orer PDEs. Hyperbolic systems. For PDEs, as for ODEs, we may reuce the orer by efining new epenent variables. For example, in the case of the wave equation, (1)

More information

APPPHYS 217 Thursday 8 April 2010

APPPHYS 217 Thursday 8 April 2010 APPPHYS 7 Thursay 8 April A&M example 6: The ouble integrator Consier the motion of a point particle in D with the applie force as a control input This is simply Newton s equation F ma with F u : t q q

More information

inflow outflow Part I. Regular tasks for MAE598/494 Task 1

inflow outflow Part I. Regular tasks for MAE598/494 Task 1 MAE 494/598, Fall 2016 Project #1 (Regular tasks = 20 points) Har copy of report is ue at the start of class on the ue ate. The rules on collaboration will be release separately. Please always follow the

More information

Real-time economic optimization for a fermentation process using Model Predictive Control

Real-time economic optimization for a fermentation process using Model Predictive Control Downloae from orbit.tu.k on: Nov 5, 218 Real-time economic optimization for a fermentation process using Moel Preictive Control Petersen, Lars Norbert; Jørgensen, John Bagterp Publishe in: Proceeings of

More information

Survey Sampling. 1 Design-based Inference. Kosuke Imai Department of Politics, Princeton University. February 19, 2013

Survey Sampling. 1 Design-based Inference. Kosuke Imai Department of Politics, Princeton University. February 19, 2013 Survey Sampling Kosuke Imai Department of Politics, Princeton University February 19, 2013 Survey sampling is one of the most commonly use ata collection methos for social scientists. We begin by escribing

More information

UNIFYING PCA AND MULTISCALE APPROACHES TO FAULT DETECTION AND ISOLATION

UNIFYING PCA AND MULTISCALE APPROACHES TO FAULT DETECTION AND ISOLATION UNIFYING AND MULISCALE APPROACHES O FAUL DEECION AND ISOLAION Seongkyu Yoon an John F. MacGregor Dept. Chemical Engineering, McMaster University, Hamilton Ontario Canaa L8S 4L7 yoons@mcmaster.ca macgreg@mcmaster.ca

More information

Robustness and Perturbations of Minimal Bases

Robustness and Perturbations of Minimal Bases Robustness an Perturbations of Minimal Bases Paul Van Dooren an Froilán M Dopico December 9, 2016 Abstract Polynomial minimal bases of rational vector subspaces are a classical concept that plays an important

More information

Adaptive Gain-Scheduled H Control of Linear Parameter-Varying Systems with Time-Delayed Elements

Adaptive Gain-Scheduled H Control of Linear Parameter-Varying Systems with Time-Delayed Elements Aaptive Gain-Scheule H Control of Linear Parameter-Varying Systems with ime-delaye Elements Yoshihiko Miyasato he Institute of Statistical Mathematics 4-6-7 Minami-Azabu, Minato-ku, okyo 6-8569, Japan

More information

The Exact Form and General Integrating Factors

The Exact Form and General Integrating Factors 7 The Exact Form an General Integrating Factors In the previous chapters, we ve seen how separable an linear ifferential equations can be solve using methos for converting them to forms that can be easily

More information

The Levitation Controller Design of an Electromagnetic Suspension Vehicle using Gain Scheduled Control

The Levitation Controller Design of an Electromagnetic Suspension Vehicle using Gain Scheduled Control Proceeings of the 5th WSEAS Int. Conf. on CIRCUIS, SYSEMS, ELECRONICS, CONROL & SIGNAL PROCESSING, Dallas, USA, November 1-3, 6 35 he Levitation Controller Design of an Electromagnetic Suspension Vehicle

More information

SYNCHRONOUS SEQUENTIAL CIRCUITS

SYNCHRONOUS SEQUENTIAL CIRCUITS CHAPTER SYNCHRONOUS SEUENTIAL CIRCUITS Registers an counters, two very common synchronous sequential circuits, are introuce in this chapter. Register is a igital circuit for storing information. Contents

More information

ELEC3114 Control Systems 1

ELEC3114 Control Systems 1 ELEC34 Control Systems Linear Systems - Moelling - Some Issues Session 2, 2007 Introuction Linear systems may be represente in a number of ifferent ways. Figure shows the relationship between various representations.

More information

From Local to Global Control

From Local to Global Control Proceeings of the 47th IEEE Conference on Decision an Control Cancun, Mexico, Dec. 9-, 8 ThB. From Local to Global Control Stephen P. Banks, M. Tomás-Roríguez. Automatic Control Engineering Department,

More information

Dissipativity for dual linear differential inclusions through conjugate storage functions

Dissipativity for dual linear differential inclusions through conjugate storage functions 43r IEEE Conference on Decision an Control December 4-7, 24 Atlantis, Paraise Islan, Bahamas WeC24 Dissipativity for ual linear ifferential inclusions through conjugate storage functions Rafal Goebel,

More information

Table of Common Derivatives By David Abraham

Table of Common Derivatives By David Abraham Prouct an Quotient Rules: Table of Common Derivatives By Davi Abraham [ f ( g( ] = [ f ( ] g( + f ( [ g( ] f ( = g( [ f ( ] g( g( f ( [ g( ] Trigonometric Functions: sin( = cos( cos( = sin( tan( = sec

More information

NOTES ON EULER-BOOLE SUMMATION (1) f (l 1) (n) f (l 1) (m) + ( 1)k 1 k! B k (y) f (k) (y) dy,

NOTES ON EULER-BOOLE SUMMATION (1) f (l 1) (n) f (l 1) (m) + ( 1)k 1 k! B k (y) f (k) (y) dy, NOTES ON EULER-BOOLE SUMMATION JONATHAN M BORWEIN, NEIL J CALKIN, AND DANTE MANNA Abstract We stuy a connection between Euler-MacLaurin Summation an Boole Summation suggeste in an AMM note from 196, which

More information

The Optimal Steady-State Control Problem

The Optimal Steady-State Control Problem SUBMITTED TO IEEE TRANSACTIONS ON AUTOMATIC CONTROL. THIS VERSION: OCTOBER 31, 218 1 The Optimal Steay-State Control Problem Liam S. P. Lawrence Stuent Member, IEEE, John W. Simpson-Porco, Member, IEEE,

More information

The canonical controllers and regular interconnection

The canonical controllers and regular interconnection Systems & Control Letters ( www.elsevier.com/locate/sysconle The canonical controllers an regular interconnection A.A. Julius a,, J.C. Willems b, M.N. Belur c, H.L. Trentelman a Department of Applie Mathematics,

More information

F 1 x 1,,x n. F n x 1,,x n

F 1 x 1,,x n. F n x 1,,x n Chapter Four Dynamical Systems 4. Introuction The previous chapter has been evote to the analysis of systems of first orer linear ODE s. In this chapter we will consier systems of first orer ODE s that

More information

12.11 Laplace s Equation in Cylindrical and

12.11 Laplace s Equation in Cylindrical and SEC. 2. Laplace s Equation in Cylinrical an Spherical Coorinates. Potential 593 2. Laplace s Equation in Cylinrical an Spherical Coorinates. Potential One of the most important PDEs in physics an engineering

More information

JUST THE MATHS UNIT NUMBER DIFFERENTIATION 2 (Rates of change) A.J.Hobson

JUST THE MATHS UNIT NUMBER DIFFERENTIATION 2 (Rates of change) A.J.Hobson JUST THE MATHS UNIT NUMBER 10.2 DIFFERENTIATION 2 (Rates of change) by A.J.Hobson 10.2.1 Introuction 10.2.2 Average rates of change 10.2.3 Instantaneous rates of change 10.2.4 Derivatives 10.2.5 Exercises

More information

Sliding mode approach to congestion control in connection-oriented communication networks

Sliding mode approach to congestion control in connection-oriented communication networks JOURNAL OF APPLIED COMPUTER SCIENCE Vol. xx. No xx (200x), pp. xx-xx Sliing moe approach to congestion control in connection-oriente communication networks Anrzej Bartoszewicz, Justyna Żuk Technical University

More information

Calculus and optimization

Calculus and optimization Calculus an optimization These notes essentially correspon to mathematical appenix 2 in the text. 1 Functions of a single variable Now that we have e ne functions we turn our attention to calculus. A function

More information

Control of a PEM Fuel Cell Based on a Distributed Model

Control of a PEM Fuel Cell Based on a Distributed Model 21 American Control Conference Marriott Waterfront, Baltimore, MD, USA June 3-July 2, 21 FrC1.6 Control of a PEM Fuel Cell Base on a Distribute Moel Michael Mangol Abstract To perform loa changes in proton

More information

Lectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs

Lectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs Lectures - Week 10 Introuction to Orinary Differential Equations (ODES) First Orer Linear ODEs When stuying ODEs we are consiering functions of one inepenent variable, e.g., f(x), where x is the inepenent

More information

Lecture 2 Lagrangian formulation of classical mechanics Mechanics

Lecture 2 Lagrangian formulation of classical mechanics Mechanics Lecture Lagrangian formulation of classical mechanics 70.00 Mechanics Principle of stationary action MATH-GA To specify a motion uniquely in classical mechanics, it suffices to give, at some time t 0,

More information

An Introduction to Event-triggered and Self-triggered Control

An Introduction to Event-triggered and Self-triggered Control An Introuction to Event-triggere an Self-triggere Control W.P.M.H. Heemels K.H. Johansson P. Tabuaa Abstract Recent evelopments in computer an communication technologies have le to a new type of large-scale

More information

Kou Yamada 1, Takaaki Hagiwara 2, Iwanori Murakami 3, Shun Yamamoto 4, and Hideharu Yamamoto 5, Non-members

Kou Yamada 1, Takaaki Hagiwara 2, Iwanori Murakami 3, Shun Yamamoto 4, and Hideharu Yamamoto 5, Non-members Achievement of low-sensitivity characteristics an robust stability conition for multi-variable systems having an uncertain number of right half plane poles67 Achievement of low-sensitivity characteristics

More information

Laplacian Cooperative Attitude Control of Multiple Rigid Bodies

Laplacian Cooperative Attitude Control of Multiple Rigid Bodies Laplacian Cooperative Attitue Control of Multiple Rigi Boies Dimos V. Dimarogonas, Panagiotis Tsiotras an Kostas J. Kyriakopoulos Abstract Motivate by the fact that linear controllers can stabilize the

More information

Adaptive Optimal Path Following for High Wind Flights

Adaptive Optimal Path Following for High Wind Flights Milano (Italy) August - September, 11 Aaptive Optimal Path Following for High Win Flights Ashwini Ratnoo P.B. Sujit Mangal Kothari Postoctoral Fellow, Department of Aerospace Engineering, Technion-Israel

More information

A Globally Stabilizing Receding Horizon Controller for Neutrally Stable Linear Systems with Input Constraints 1

A Globally Stabilizing Receding Horizon Controller for Neutrally Stable Linear Systems with Input Constraints 1 A Globally Stabilizing Receding Horizon Controller for Neutrally Stable Linear Systems with Input Constraints 1 Ali Jadbabaie, Claudio De Persis, and Tae-Woong Yoon 2 Department of Electrical Engineering

More information

Introduction to variational calculus: Lecture notes 1

Introduction to variational calculus: Lecture notes 1 October 10, 2006 Introuction to variational calculus: Lecture notes 1 Ewin Langmann Mathematical Physics, KTH Physics, AlbaNova, SE-106 91 Stockholm, Sween Abstract I give an informal summary of variational

More information

Online Appendix for Trade Policy under Monopolistic Competition with Firm Selection

Online Appendix for Trade Policy under Monopolistic Competition with Firm Selection Online Appenix for Trae Policy uner Monopolistic Competition with Firm Selection Kyle Bagwell Stanfor University an NBER Seung Hoon Lee Georgia Institute of Technology September 6, 2018 In this Online

More information

Path-By-Path Output Regulation of Switched Systems With a Receding Horizon of Modal Knowledge

Path-By-Path Output Regulation of Switched Systems With a Receding Horizon of Modal Knowledge 24 American Control Conference (ACC) June 4-6, 24. Portlan, Oregon, USA Path-By-Path Output Regulation of Switche Systems With a Receing Horizon of Moal Knowlege Ray Essick Ji-Woong Lee Geir Dulleru Abstract

More information

'HVLJQ &RQVLGHUDWLRQ LQ 0DWHULDO 6HOHFWLRQ 'HVLJQ 6HQVLWLYLW\,1752'8&7,21

'HVLJQ &RQVLGHUDWLRQ LQ 0DWHULDO 6HOHFWLRQ 'HVLJQ 6HQVLWLYLW\,1752'8&7,21 Large amping in a structural material may be either esirable or unesirable, epening on the engineering application at han. For example, amping is a esirable property to the esigner concerne with limiting

More information

ECE 422 Power System Operations & Planning 7 Transient Stability

ECE 422 Power System Operations & Planning 7 Transient Stability ECE 4 Power System Operations & Planning 7 Transient Stability Spring 5 Instructor: Kai Sun References Saaat s Chapter.5 ~. EPRI Tutorial s Chapter 7 Kunur s Chapter 3 Transient Stability The ability of

More information

II. First variation of functionals

II. First variation of functionals II. First variation of functionals The erivative of a function being zero is a necessary conition for the etremum of that function in orinary calculus. Let us now tackle the question of the equivalent

More information

Assignment 1. g i (x 1,..., x n ) dx i = 0. i=1

Assignment 1. g i (x 1,..., x n ) dx i = 0. i=1 Assignment 1 Golstein 1.4 The equations of motion for the rolling isk are special cases of general linear ifferential equations of constraint of the form g i (x 1,..., x n x i = 0. i=1 A constraint conition

More information

Balancing Expected and Worst-Case Utility in Contracting Models with Asymmetric Information and Pooling

Balancing Expected and Worst-Case Utility in Contracting Models with Asymmetric Information and Pooling Balancing Expecte an Worst-Case Utility in Contracting Moels with Asymmetric Information an Pooling R.B.O. erkkamp & W. van en Heuvel & A.P.M. Wagelmans Econometric Institute Report EI2018-01 9th January

More information

State-Space Model for a Multi-Machine System

State-Space Model for a Multi-Machine System State-Space Moel for a Multi-Machine System These notes parallel section.4 in the text. We are ealing with classically moele machines (IEEE Type.), constant impeance loas, an a network reuce to its internal

More information

Permanent vs. Determinant

Permanent vs. Determinant Permanent vs. Determinant Frank Ban Introuction A major problem in theoretical computer science is the Permanent vs. Determinant problem. It asks: given an n by n matrix of ineterminates A = (a i,j ) an

More information

Conservation laws a simple application to the telegraph equation

Conservation laws a simple application to the telegraph equation J Comput Electron 2008 7: 47 51 DOI 10.1007/s10825-008-0250-2 Conservation laws a simple application to the telegraph equation Uwe Norbrock Reinhol Kienzler Publishe online: 1 May 2008 Springer Scienceusiness

More information

Lie symmetry and Mei conservation law of continuum system

Lie symmetry and Mei conservation law of continuum system Chin. Phys. B Vol. 20, No. 2 20 020 Lie symmetry an Mei conservation law of continuum system Shi Shen-Yang an Fu Jing-Li Department of Physics, Zhejiang Sci-Tech University, Hangzhou 3008, China Receive

More information

A simplified macroscopic urban traffic network model for model-based predictive control

A simplified macroscopic urban traffic network model for model-based predictive control Delft University of Technology Delft Center for Systems an Control Technical report 9-28 A simplifie macroscopic urban traffic network moel for moel-base preictive control S. Lin, B. De Schutter, Y. Xi,

More information

EE 370L Controls Laboratory. Laboratory Exercise #7 Root Locus. Department of Electrical and Computer Engineering University of Nevada, at Las Vegas

EE 370L Controls Laboratory. Laboratory Exercise #7 Root Locus. Department of Electrical and Computer Engineering University of Nevada, at Las Vegas EE 370L Controls Laboratory Laboratory Exercise #7 Root Locus Department of Electrical an Computer Engineering University of Nevaa, at Las Vegas 1. Learning Objectives To emonstrate the concept of error

More information

Polynomial Inclusion Functions

Polynomial Inclusion Functions Polynomial Inclusion Functions E. e Weert, E. van Kampen, Q. P. Chu, an J. A. Muler Delft University of Technology, Faculty of Aerospace Engineering, Control an Simulation Division E.eWeert@TUDelft.nl

More information

ON THE OPTIMALITY SYSTEM FOR A 1 D EULER FLOW PROBLEM

ON THE OPTIMALITY SYSTEM FOR A 1 D EULER FLOW PROBLEM ON THE OPTIMALITY SYSTEM FOR A D EULER FLOW PROBLEM Eugene M. Cliff Matthias Heinkenschloss y Ajit R. Shenoy z Interisciplinary Center for Applie Mathematics Virginia Tech Blacksburg, Virginia 46 Abstract

More information

How the potentials in different gauges yield the same retarded electric and magnetic fields

How the potentials in different gauges yield the same retarded electric and magnetic fields How the potentials in ifferent gauges yiel the same retare electric an magnetic fiels José A. Heras a Departamento e Física, E. S. F. M., Instituto Politécnico Nacional, México D. F. México an Department

More information

Damage identification based on incomplete modal data and constrained nonlinear multivariable function

Damage identification based on incomplete modal data and constrained nonlinear multivariable function Journal of Physics: Conference Series PAPER OPEN ACCESS Damage ientification base on incomplete moal ata an constraine nonlinear multivariable function To cite this article: S S Kourehli 215 J. Phys.:

More information

Power Systems Control Prof. Wonhee Kim. Ch.3. Controller Design in Time Domain

Power Systems Control Prof. Wonhee Kim. Ch.3. Controller Design in Time Domain Power Systems Control Prof. Wonhee Kim Ch.3. Controller Design in Time Domain Stability in State Space Equation: State Feeback t A t B t t C t D t x x u y x u u t Kx t t A t BK t A BK x t x x x K shoul

More information

A Path Planning Method Using Cubic Spiral with Curvature Constraint

A Path Planning Method Using Cubic Spiral with Curvature Constraint A Path Planning Metho Using Cubic Spiral with Curvature Constraint Tzu-Chen Liang an Jing-Sin Liu Institute of Information Science 0, Acaemia Sinica, Nankang, Taipei 5, Taiwan, R.O.C., Email: hartree@iis.sinica.eu.tw

More information

Applications of the Wronskian to ordinary linear differential equations

Applications of the Wronskian to ordinary linear differential equations Physics 116C Fall 2011 Applications of the Wronskian to orinary linear ifferential equations Consier a of n continuous functions y i (x) [i = 1,2,3,...,n], each of which is ifferentiable at least n times.

More information

Equilibrium in Queues Under Unknown Service Times and Service Value

Equilibrium in Queues Under Unknown Service Times and Service Value University of Pennsylvania ScholarlyCommons Finance Papers Wharton Faculty Research 1-2014 Equilibrium in Queues Uner Unknown Service Times an Service Value Laurens Debo Senthil K. Veeraraghavan University

More information

Criteria for Global Stability of Coupled Systems with Application to Robust Output Feedback Design for Active Surge Control

Criteria for Global Stability of Coupled Systems with Application to Robust Output Feedback Design for Active Surge Control Criteria for Global Stability of Couple Systems with Application to Robust Output Feeback Design for Active Surge Control Shiriaev, Anton; Johansson, Rolf; Robertsson, Aners; Freiovich, Leoni 9 Link to

More information

IERCU. Institute of Economic Research, Chuo University 50th Anniversary Special Issues. Discussion Paper No.210

IERCU. Institute of Economic Research, Chuo University 50th Anniversary Special Issues. Discussion Paper No.210 IERCU Institute of Economic Research, Chuo University 50th Anniversary Special Issues Discussion Paper No.210 Discrete an Continuous Dynamics in Nonlinear Monopolies Akio Matsumoto Chuo University Ferenc

More information

On Characterizing the Delay-Performance of Wireless Scheduling Algorithms

On Characterizing the Delay-Performance of Wireless Scheduling Algorithms On Characterizing the Delay-Performance of Wireless Scheuling Algorithms Xiaojun Lin Center for Wireless Systems an Applications School of Electrical an Computer Engineering, Purue University West Lafayette,

More information

IPA Derivatives for Make-to-Stock Production-Inventory Systems With Backorders Under the (R,r) Policy

IPA Derivatives for Make-to-Stock Production-Inventory Systems With Backorders Under the (R,r) Policy IPA Derivatives for Make-to-Stock Prouction-Inventory Systems With Backorers Uner the (Rr) Policy Yihong Fan a Benamin Melame b Yao Zhao c Yorai Wari Abstract This paper aresses Infinitesimal Perturbation

More information

Designing Information Devices and Systems II Fall 2017 Note Theorem: Existence and Uniqueness of Solutions to Differential Equations

Designing Information Devices and Systems II Fall 2017 Note Theorem: Existence and Uniqueness of Solutions to Differential Equations EECS 6B Designing Information Devices an Systems II Fall 07 Note 3 Secon Orer Differential Equations Secon orer ifferential equations appear everywhere in the real worl. In this note, we will walk through

More information

Connections Between Duality in Control Theory and

Connections Between Duality in Control Theory and Connections Between Duality in Control heory an Convex Optimization V. Balakrishnan 1 an L. Vanenberghe 2 Abstract Several important problems in control theory can be reformulate as convex optimization

More information

On the Aloha throughput-fairness tradeoff

On the Aloha throughput-fairness tradeoff On the Aloha throughput-fairness traeoff 1 Nan Xie, Member, IEEE, an Steven Weber, Senior Member, IEEE Abstract arxiv:1605.01557v1 [cs.it] 5 May 2016 A well-known inner boun of the stability region of

More information

Minimum-time constrained velocity planning

Minimum-time constrained velocity planning 7th Meiterranean Conference on Control & Automation Makeonia Palace, Thessaloniki, Greece June 4-6, 9 Minimum-time constraine velocity planning Gabriele Lini, Luca Consolini, Aurelio Piazzi Università

More information

Implicit Differentiation

Implicit Differentiation Implicit Differentiation Thus far, the functions we have been concerne with have been efine explicitly. A function is efine explicitly if the output is given irectly in terms of the input. For instance,

More information

Chapter 6: Energy-Momentum Tensors

Chapter 6: Energy-Momentum Tensors 49 Chapter 6: Energy-Momentum Tensors This chapter outlines the general theory of energy an momentum conservation in terms of energy-momentum tensors, then applies these ieas to the case of Bohm's moel.

More information

Least-Squares Regression on Sparse Spaces

Least-Squares Regression on Sparse Spaces Least-Squares Regression on Sparse Spaces Yuri Grinberg, Mahi Milani Far, Joelle Pineau School of Computer Science McGill University Montreal, Canaa {ygrinb,mmilan1,jpineau}@cs.mcgill.ca 1 Introuction

More information

Closed and Open Loop Optimal Control of Buffer and Energy of a Wireless Device

Closed and Open Loop Optimal Control of Buffer and Energy of a Wireless Device Close an Open Loop Optimal Control of Buffer an Energy of a Wireless Device V. S. Borkar School of Technology an Computer Science TIFR, umbai, Inia. borkar@tifr.res.in A. A. Kherani B. J. Prabhu INRIA

More information

Power Generation and Distribution via Distributed Coordination Control

Power Generation and Distribution via Distributed Coordination Control Power Generation an Distribution via Distribute Coorination Control Byeong-Yeon Kim, Kwang-Kyo Oh, an Hyo-Sung Ahn arxiv:407.4870v [math.oc] 8 Jul 204 Abstract This paper presents power coorination, power

More information

Metzler Matrix Transform Determination using a Nonsmooth Optimization Technique with an Application to Interval Observers

Metzler Matrix Transform Determination using a Nonsmooth Optimization Technique with an Application to Interval Observers Downloae 4/7/18 to 148.251.232.83. Reistribution subject to SIAM license or copyright; see http://www.siam.org/journals/ojsa.php Metzler Matrix Transform Determination using a Nonsmooth Optimization Technique

More information

Linear Model Predictive Control via Multiparametric Programming

Linear Model Predictive Control via Multiparametric Programming 3 1 Linear Model Predictive Control via Multiparametric Programming Vassilis Sakizlis, Konstantinos I. Kouramas, and Efstratios N. Pistikopoulos 1.1 Introduction Linear systems with input, output, or state

More information

Summary: Differentiation

Summary: Differentiation Techniques of Differentiation. Inverse Trigonometric functions The basic formulas (available in MF5 are: Summary: Differentiation ( sin ( cos The basic formula can be generalize as follows: Note: ( sin

More information

Thermal conductivity of graded composites: Numerical simulations and an effective medium approximation

Thermal conductivity of graded composites: Numerical simulations and an effective medium approximation JOURNAL OF MATERIALS SCIENCE 34 (999)5497 5503 Thermal conuctivity of grae composites: Numerical simulations an an effective meium approximation P. M. HUI Department of Physics, The Chinese University

More information

Some Remarks on the Boundedness and Convergence Properties of Smooth Sliding Mode Controllers

Some Remarks on the Boundedness and Convergence Properties of Smooth Sliding Mode Controllers International Journal of Automation an Computing 6(2, May 2009, 154-158 DOI: 10.1007/s11633-009-0154-z Some Remarks on the Bouneness an Convergence Properties of Smooth Sliing Moe Controllers Wallace Moreira

More information

Consider for simplicity a 3rd-order IIR filter with a transfer function. where

Consider for simplicity a 3rd-order IIR filter with a transfer function. where Basic IIR Digital Filter The causal IIR igital filters we are concerne with in this course are characterie by a real rational transfer function of or, equivalently by a constant coefficient ifference equation

More information

Mathcad Lecture #5 In-class Worksheet Plotting and Calculus

Mathcad Lecture #5 In-class Worksheet Plotting and Calculus Mathca Lecture #5 In-class Worksheet Plotting an Calculus At the en of this lecture, you shoul be able to: graph expressions, functions, an matrices of ata format graphs with titles, legens, log scales,

More information

Agmon Kolmogorov Inequalities on l 2 (Z d )

Agmon Kolmogorov Inequalities on l 2 (Z d ) Journal of Mathematics Research; Vol. 6, No. ; 04 ISSN 96-9795 E-ISSN 96-9809 Publishe by Canaian Center of Science an Eucation Agmon Kolmogorov Inequalities on l (Z ) Arman Sahovic Mathematics Department,

More information

A Novel Unknown-Input Estimator for Disturbance Estimation and Compensation

A Novel Unknown-Input Estimator for Disturbance Estimation and Compensation A Novel Unknown-Input Estimator for Disturbance Estimation an Compensation Difan ang Lei Chen Eric Hu School of Mechanical Engineering he University of Aelaie Aelaie South Australia 5005 Australia leichen@aelaieeuau

More information

ANALYSIS OF A GENERAL FAMILY OF REGULARIZED NAVIER-STOKES AND MHD MODELS

ANALYSIS OF A GENERAL FAMILY OF REGULARIZED NAVIER-STOKES AND MHD MODELS ANALYSIS OF A GENERAL FAMILY OF REGULARIZED NAVIER-STOKES AND MHD MODELS MICHAEL HOLST, EVELYN LUNASIN, AND GANTUMUR TSOGTGEREL ABSTRACT. We consier a general family of regularize Navier-Stokes an Magnetohyroynamics

More information

u t v t v t c a u t b a v t u t v t b a

u t v t v t c a u t b a v t u t v t b a Nonlinear Dynamical Systems In orer to iscuss nonlinear ynamical systems, we must first consier linear ynamical systems. Linear ynamical systems are just systems of linear equations like we have been stuying

More information