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EE 380 Fall 2014 Lecture 4. EE 380 Linear Control Systems Lecture 4 Professor Jeffrey Schiano Department of Electrical Engineering 1

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EE 380 Fall 2014Lecture 4.

EE 380

Linear Control Systems

Lecture 4

Professor Jeffrey SchianoDepartment of Electrical Engineering

1

EE 380 Fall 2014Lecture 4.

Lecture 4 Topics

• State-Space Representation– Advantages– Definitions– Transfer function from State-Space Matrices

• Example

2

EE 380 Fall 2014Lecture 4.

Advantages• Facilitates the use of linear algebra tools in the design and

analysis of feedback control systems– Nonlinear systems– Time-varying systems

• Easily represents multiple-input multi-output (MIMO) systems

• Provides a complete internal model of the plant dynamics– Pole-zero cancellations in the transfer function

(input/output ) description may hide poorly damped (oscillatory) or unstable modes

3

EE 380 Fall 2014Lecture 4.

Terminology• The state of a system is the smallest number of n variables

x1(t), x2(t),…,xn(t), called state variables, such that the initial values xi(to) of these variables and the m system inputs u1(t), u2(t),…,um(t), are sufficient to uniquely describe the system’s future response for t ≥ t0

• The set of state variables xi(t) represents the components of the n-dimensional state vector that specifies the system behavior for any t ≥ t0

4

1

n

x tx t

x t

EE 380 Fall 2014Lecture 4.

Terminology• State space defines an n-dimensional space in which the

components of the state vector represent its coordinate axis

• State trajectory defines the path of the state vector x(t) as it evolves with time. State space and state trajectory in the two-dimensional case (n=2) are referred to as the phase plane and phase trajectory

• The state equations are a coupled set of n first-order differential equations expressed in terms of the state variables

5

EE 380 Fall 2014Lecture 4.

State Equations• The state equations are represented as

• Let

then

6

1 1 1 2, , 1 2, , ,

1 2, , 1 2, , ,

, , ,

, , ,

n m

n n n m

x f x x x u u u t

x f x x x u u u t

, ,x f x u t

1 1 1 1 , ,, , , ( , , )

, ,n n m n

x x u f x u tx x u f x u t

x x u f x u t

EE 380 Fall 2014Lecture 4.

Output Equations• The output equations are represented as

• Let

then

7

1 1 1 2, , 1 2, , ,

1 2, , 1 2, , ,

, , ,

, , ,

n m

r r n m

y g x x x u u u t

y g x x x u u u t

, ,y g x u t

1 1 , ,, ( , , )

, ,r r

y g x u ty g x u t

y g x u t

EE 380 Fall 2014Lecture 4.

State-Space Representation• General Case

• Time-Invariant Systems

8

, ,

, ,

x f x u t

y g x u t

,

,

x f x u

y g x u

EE 380 Fall 2014Lecture 4.

Linear System• Linear Time-Varying Systems

• Linear Time-Invariant Systems

• Dimensions

9

x F t x G t u

y H t x J t u

x Ax Buy Cx Du

1 1 1, ,n m rx u y

x A t x B t u

y C t x D t u

x Fx Guy Hx Ju

, , ,n n n m r n r mA B C D , , ,n n n m r n r mF G H J

EE 380 Fall 2014Lecture 4.

Transfer Function Representation• For a LTI system represented by the state-space model

the transfer function representation is

10

,x Fx Guy Hx Ju

1

transfer function

Y s H sI F G J U s

,x Ax Buy Cx Du

1

transfer function

Y s C sI A B D U s

EE 380 Fall 2014Lecture 4.

Example• Determine the transfer function and state-space

representation of a single-input single-output (SISO) system represented by the ordinary differential equation

11

2y y y u u

EE 380 Fall 2014Lecture 4.

Solution

12

EE 380 Fall 2014Lecture 4.

Solution

13

EE 380 Fall 2014Lecture 4.

Solution

14

EE 380 Fall 2014Lecture 4.

EE 380

Linear Control Systems

Lecture 4

Professor Jeffrey SchianoDepartment of Electrical Engineering

1

EE 380 Fall 2014Lecture 4.

Lecture 4 Topics

• State-Space Representation– Advantages– Definitions– Transfer function from State-Space Matrices

• Example

2

EE 380 Fall 2014Lecture 4.

Advantages• Facilitates the use of linear algebra tools in the design and

analysis of feedback control systems– Nonlinear systems– Time-varying systems

• Easily represents multiple-input multi-output (MIMO) systems

• Provides a complete internal model of the plant dynamics– Pole-zero cancellations in the transfer function

(input/output ) description may hide poorly damped (oscillatory) or unstable modes

3

EE 380 Fall 2014Lecture 4.

Terminology• The state of a system is the smallest number of n variables

x1(t), x2(t),…,xn(t), called state variables, such that the initial values xi(to) of these variables and the m system inputs u1(t), u2(t),…,um(t), are sufficient to uniquely describe the system’s future response for t ≥ t0

• The set of state variables xi(t) represents the components of the n-dimensional state vector that specifies the system behavior for any t ≥ t0

4

EE 380 Fall 2014Lecture 4.

Terminology• State space defines an n-dimensional space in which the

components of the state vector represent its coordinate axis

• State trajectory defines the path of the state vector x(t) as it evolves with time. State space and state trajectory in the two-dimensional case (n=2) are referred to as the phase plane and phase trajectory

• The state equations are a coupled set of n first-order differential equations expressed in terms of the state variables

5

EE 380 Fall 2014Lecture 4.

State Equations• The state equations are represented as

• Let

then

6

EE 380 Fall 2014Lecture 4.

Output Equations• The output equations are represented as

• Let

then

7

EE 380 Fall 2014Lecture 4.

State-Space Representation• General Case

• Time-Invariant Systems

8

EE 380 Fall 2014Lecture 4.

Linear System• Linear Time-Varying Systems

• Linear Time-Invariant Systems

• Dimensions

9

EE 380 Fall 2014Lecture 4.

Transfer Function Representation• For a LTI system represented by the state-space model

the transfer function representation is

10

EE 380 Fall 2014Lecture 4.

Example• Determine the transfer function and state-space

representation of a single-input single-output (SISO) system represented by the ordinary differential equation

11

EE 380 Fall 2014Lecture 4.

Solution

12

EE 380 Fall 2014Lecture 4.

Solution

13

EE 380 Fall 2014Lecture 4.

Solution

14