Control Systems I. Lecture 2: Modeling. Suggested Readings: Åström & Murray Ch. 23, Guzzella Ch Emilio Frazzoli


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1 Control Systems I Lecture 2: Modeling Suggested Readings: Åström & Murray Ch. 23, Guzzella Ch. 23 Emilio Frazzoli Institute for Dynamic Systems and Control DMAVT ETH Zürich September 29, 2017 E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
2 Tentative schedule # Date Topic 1 Sept. 22 Introduction, Signals and Systems 2 Sept. 29 Modeling, Linearization 3 Oct. 6 Analysis 1: Time response, Stability 4 Oct. 13 Analysis 2: Diagonalization, Modal coordinates 5 Oct. 20 Transfer functions 1: Definition and properties 6 Oct. 27 Transfer functions 2: Poles and Zeros 7 Nov. 3 Analysis of feedback systems: internal stability, root locus 8 Nov. 10 Frequency response 9 Nov. 17 Analysis of feedback systems 2: the Nyquist condition 10 Nov. 24 Specifications for feedback systems 11 Dec. 1 Loop Shaping 12 Dec. 8 PID control 13 Dec. 15 Implementation issues 14 Dec. 22 Robustness E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
3 Today s learning objectives After today s lecture, you should be able to: Describe the benefits of using control systems to another student Understand the difference between the main control architectures. Can use the concept of state to model a system Write the model of a LTI system with A, B, C, D matrices. Understands the notion of equilibrium points and can calculate them. The student is able to linearize a nonlinear system at an appropriately chosen equilibrium point to derive an approximate LTI system with A, B,C, D matrices E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
4 Control objectives Stabilization: make sure the system does not blow up (i.e., it stays within normal operating conditions). Regulation: Maintain a desired operating point in spite of disturbances. Tracking: follow a reference trajectory that changes over time, as closely as possible. E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
5 Basic control architectures: FeedForward r F u P y Basic idea: given r, attempt to compute what should be the control input u that would make y = r. Essentially, F should be an inverse of P. Relies on good knowledge of P sensitive to modeling errors. Cannot alter the dynamics of P, i.e., cannot make an unstable system stable. E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
6 Basic control architectures: Feedback r e C u P y Basic idea: given the error r y, compute u such that the error is small. Intuition: the bigger C, the smaller the error e will be, regardless of P (under some assumption, e.g., closedloop stability). Does not require a precise knowledge of P robust to modeling errors. Can stabilize unstable systems. But can also make stable systems unstable (!). Needs an error to develop in order to figure out the appropriate control. E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
7 Basic control architectures: two degrees of freedom F r e C u P y Basic idea: given r, compute a guess for the control input u that would make y = r; correct this guess based on the measurement of the error e, so that the error is minimized. Combines the main advantages of feedforward and feedback architectures. Ensures stability, robustness, but can also speed up tracking/regulation. E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
8 Benefits/dangers of feedback Feedforward control relies on a precise knowledge of the plant, and does not change its dynamics. Feedback control allows one to Stabilize an unstable system; Handle uncertainties in the system; Reject external disturbances. However, feedback can introduce instability, even in an otherwise stable system! feed sensor noise into the system. Two degrees of freedom (feedforward + feedback) allow better transient behavior, e.g., can yield good tracking of rapidlychanging reference inputs. E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
9 Causality revisited An inputoutput system Σ is causal if, for any t T, the output at time t depends only on the values of the input on (, t]. In other words, an inputoutput system Σ is causal if P T ΣP T = P T Σ, T T. E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
10 State of a system We know that, if a system is causal, in order to compute its output at a given time t 0, we need to know only the input signal over (, t 0 ]. This is a lot of information. Can we summarize it with something more manageable? Definition (state) The state x(t 1 ) of a causal system at time t 1 is the information needed, together with the input u between times t 1 and t 2, to uniquely predict the output at time t 2, for all t 2 t 1. In other words, the state of the system at a given time t summarizes the whole history of the past inputs over (, t), for the purpose of predicting the output at future times. Usually, the state of a system is a vector in some Euclidean space R n. E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
11 Water tank example Suppose that the input is u = u + u (i.e., net flow of water into the tank). Is there a way to summarize the effect of all past inputs until time T? E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
12 Dimension of a system The choice of a state for a system is not unique (in fact, there are infinite choices, or realizations). However, there are come choices of state which are preferable to others; in particular, we can look at minimal realizations. Definition (Dimension of a system) We define the dimension of a causal system as the minimal number of variables sufficient to describe the system s state (i.e., the dimension of the smallest state vector). We will deal mostly with finitedimensional systems, i.e., systems which can be described with a finite number of variables. E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
13 LTI Statespace model It can be shown that any finitedimensional LTI system can be described by a statespace model of the form: Definition (Continuoustime StateSpace Models) d x(t) dt = Ax(t) + Bu(t); y(t) = Cx(t) + Du(t); The state x represents the memory of the system. The state x is an internal variable that cannot be accessed directly, but only controlled though the input x and observed through the output y. The order of the system is the dimension of the state x. A system is memoryless if the dimension of the state is zero (i.e., there is no need to keep a state, or memory) A system is strictly causal if the feedthrough term D is zero. E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
14 Water Tank (Integrator) Notation: Flow: u = u + u, Water level: h, Tank crosssection area: S, Dynamic model: d h dt = 1 S u Statespace model, with y = x = h: [ ] [ ] A B 0 1 = S C D 1 0 E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
15 Temperature Control (1st order system) Notation: Heat Flow: u, Temperature: T, Outside Temperature: T e, Thermal Conductivity: c Thermal Capacity: m Dynamic model: m d T dt = c(t e T ) + u Equilibrium (T, u) = (T e, u). Statespace model, with y = x = T T e : [ ] [ A B c = m C D m ] E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
16 Nonlinear systems Unfortunately, most realworld systems are nonlinear. Finitedimensional, timeinvariant, causal nonlinear control systems, with input u and output y can typically be modeled using a set of differential equations as follows: Definition (Continuoustime Nonlinear StateSpace Models) ẋ(t) := d x(t) dt = f (x(t), u(t)), y(t) = g(x(t), u(t)); Can we construct an LTI approximation of this system, so that we can apply the techniques designed for LTI systems? Remarkably, control systems designed for the LTI approximation will work very well for the nonlinear system. E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
17 Pendulum (2ndorder nonlinear system) Notation: Angular position: θ, Torque input: u, Pendulum length: L, Pendulum mass: m, Viscous damping coefficient: c Dynamic model: ml 2 θ = c θ mgl sin θ + u. Define x 1 := θ, and x 2 := θ. Then one can write ẋ 1 = x 2, ẋ 2 = c ml 2 x 2 g L sin(x 1) + u. E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
18 Equilibrium point The pendulum is a nonlinear system. How can we construct an approximate model which is linear? The key idea is that of constructing an approximation that is valid near some special operating condition, e.g., equilibrium points. Definition (Equilibrium point) A system described by an ODE ẋ(t) = f (x(t), u(t)) has an equilibrium point (x e, u e ) if f (x e, u e ) = 0. Clearly, if x(0) = x e, and u(t) = u e for all t 0, then x(t) = x(0) = x e, for all t 0. E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
19 Equilibria for a pendulum What would be an equilibrium for the pendulum? We need to solve for ẋ 1 = x 2 = 0, ẋ 2 = c ml 2 x 2 g L sin(x 1) + u = 0. There are two solutions: x e = (0, 0), u e = 0, and x e = (π, 0), u e = 0. The first equilibrium is stable, the second unstable; we will make these notions more precise. E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
20 (Jacobian) Linearization procedure Given an equilibrium point (x e, u e ), with output y e = g(x e, u e ), a linearized model is obtained by setting x x e + δx, u u e + δu, y y e + δy, and then neglecting all terms of second (or higher) order in δx, δu, and δy in the (nonlinear) dynamics model. Note that since x e is a constant, ẋ = δẋ. The resulting model would be a good approximation of the original nonlinear model when near the equilibrium point, i.e., for δx << 1, δu << 1, and δy << 1. E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
21 Linearization about the stable equilibrium Susbstituting as in the previous slide, with x e = (0, 0) and u e = 0, δẋ 1 = 0 + δx 2, δẋ 2 = c ml 2 (0 + δx 2) g L (0 + δx 1) + 1 (0 + δu), ml2 δy = δx 1. The above can be rewritten in the statespace form as δẋ = Aδx + Bδu, δy = Cδx + Dδu, where [ ] [ ] A = g/l c/(ml 2, B = ) 1/(mL 2. ) C = [ 1 0 ], D = 0. E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
22 Linearization about the unstable equilibrium Susbstituting x e = (π, 0) and u e = 0, δẋ 1 = π + δx 2, δẋ 2 = c ml 2 (0 + δx 2) g L (0 δx 1) + 1 (0 + δu), ml2 δy = δx 1. The above can be rewritten in the statespace form as δẋ = Aδx + Bδu, δy = Cδx + Dδu, where [ ] [ ] A = +g/l c/(ml 2, B = ) 1/(mL 2. ) C = [ 1 0 ], D = 0. E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
23 Some remarks on infinitedimensional systems Even though we will not address infinitedimensional systems in detail, some examples are very useful: Timedelay systems: Consider the very simple time delay S T, defined as a continuoustime system such that its input and outputs are related by y(t) = u(t T ). In order to predict the output at times after t, the knowledge of the input for all times in (t T, t] is necessary. PDEdriven systems: Many systems in engineering, arising, e.g., in structural control and flow control applications, can only be described exactly using a continuum of state variables (stress, displacement, pressure, temperature, etc.). These are infinitedimensional systems. In order to deal with infinitedimensional systems, approximate discrete models are often used to reduce the dimension of the state. E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
24 Today s learning objectives After today s lecture, you should be able to: Describe the benefits of using control systems to another student Understand the difference between the main control architectures. Can use the concept of state to model a system Write the model of a LTI system with A, B, C, D matrices. Understand the notion of equilibrium points. Linearize a nonlinear system at an appropriately chosen equilibrium point to derive an approximate LTI system with A, B,C, D matrices E. Frazzoli (ETH) Lecture 2: Control Systems I 09/29/ / 24
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