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State Space Analysis-1

The document discusses state space analysis and the state space approach. It provides definitions of key concepts like state, state variable, state vector and state space. It also discusses the representation and analysis of systems using state equations and output equations in matrix form.
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0% found this document useful (0 votes)
34 views52 pages

State Space Analysis-1

The document discusses state space analysis and the state space approach. It provides definitions of key concepts like state, state variable, state vector and state space. It also discusses the representation and analysis of systems using state equations and output equations in matrix form.
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
Available Formats
Download as PDF, TXT or read online on Scribd
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STATE SPACE ANALYSIS

 The transfer function is the classical approach using the frequency domain
technique deals with input and output only.
 It is unable to give any information about the internal condition.
 On the modern control theory based on the state variable approach.
 It is a time-domain technique.
 It is include the initial conditions in the system.
 It is used as a mathematical tool to solve linear, non-linear, time-varying
and time-varying control problems.
 In this approach to analysis of control system with basic knowledge of
matrix algebra.

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Limitations of Classical or Transfer Function Approach

 It is based on transfer functions derived from linear differential equations


with constant coefficients.
 Analysis and design of linear time-invariant SISO control systems.
 Not applicable to nonlinear, time-varying and MIMO systems.
 The initial conditions are are set to zero.
 Initial conditions cannot be included.
 Does not give any information about the internal variables.
 The test signals like unit impulse, step, ramp and unit parabolic inputs.

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Advantages of the State Space Method

1. Applicable to be linear, nonlinear, time-invariant and time varying systems


2. MIMO systems can be represented and analyzed
3. Initial conditions are incorporated
4. It is based on certain internal variables in a system, and these variables, at
any time, can be known.
5. Discrete-time model is obtained which can be analyzed using a digital
computer.

Disadvantages of the State Space Method

1. This technique is complex over the conventional methods.


2. In this techniques many computations are required.

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Concept of State Space Response
 Consider a linear time-invariant continuous time system with an input u(t) and output response
y(t) as shown in Figure l.

Figure 1 : Input-output relationship in a LTI system


 The output response y(t) is given by the convolution integral 1
t
y (t )   h (t   )u ( ) d 1

where h(t) is the impulse response of the system.
 Consider that the input is applied at time t = 0, then the response can be written as
0 t
y (t )   h(t   )u ( ) d   h(t   )u ( ) d
 0

 The first term on the right hand side is the response of the system at t = 0, and this is the initial
condition of the system.
 Then y(t) can be written as
t
y (t )  y (0)   h (t   )u ( ) d
0
 The output y(t) can be determined completely for a given input u(t), if the initial condition y(0) is
known.
 Given the initial states at t = to and the inputs for t ≥ to, it is possible to determine the system
response completely for any time t > to.
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Basic Concept of State Space Response
 Consider the system defined by following differential equation
a 
y (t )  b y (t )  c y (t )  du (t ) (1)

where y is the output and u is input of the system.


 This system is of second order.
 This means that the system involves two integrators.
 Let us define state variables x1 and x2 as
x1  y
and x2  x1  y
 Then equation (2) can be written as
ax2  bx2  cx1  d u

Now, x1  x2 (2)

and x2   ac x1  ba x2  da u (3)


 We can write this two equations (2) and (3) in vector-matrix form as
 x1   0 1   x1   0 
 x    c b     d u (4)
 2    a  a   x2   a 
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Concept of State Space Response

 The output equation is

 x1 
y  x1   1 0   
(5)
 x2 
 Equation (4) and (5) are in the standard form:

x  Ax  B u (6)
and y  Cx  D u (7)

 0 1 0
A c b ; B  d ; C  1 0 ; and D = [ 0 ]
  a  a   a 

 Equation (6) is a state equation and equation (7) is an output equation of the system.

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State Model for Linear System

 Consider a third-order linear time-invariant system, which is described by a third-order


differential equation.
 Let the state variables are x1 (t ), x2 (t ) and x3 (t ) and two inputs r1 (t ) and r2 (t ) and
two outputs y1 (t ) and y2 (t ) .
 A set of three first-order differential equations can be written in the form

x1  a11 x1 (t )  a12 x2 (t )  a13 x3 (t )  b11 r1 (t )  b12 r2 (t ) (1)


x2  a21 x1 (t )  a22 x2 (t )  a23 x3 (t )  b21 r1 (t )  b22 r2 (t ) (2)
x3  a31 x1 (t )  a32 x2 (t )  a33 x3 (t )  b31 r1 (t )  b32 r2 (t ) (3)

 The state equations (1), (2) and (3) can be written in matrix form as

 x1   a11 a12 a13   x1 (t )   b11 b12 


 x    a  r (t ) 
 2   21 a22 a23   x2 (t )   b21 b22   1 
 r2 (t ) 
 x3   a31 a32 a33   x3 (t )  b31 b32 

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State Model for Linear System

 The output equations are


y1 (t )  c11 x1 (t )  c12 x2 (t )  c13 x3 (t )  d11 r1 (t )  d12 r2 (t ) (5)
y2 (t )  c21 x1 (t )  c22 x2 (t )  c23 x3 (t )  d 21 r1 (t )  d 22 r2 (t ) (6)

 The output equations (5) and (6) can be expressed in matrix form as
 x (t ) 
 y1 (t )   c11 c12 c13   1   d11 d12   r1 (t ) 
 y (t )    c  x2 (t )   
 2   21 c22 c23   d d 22   r2 (t ) 
 x3 (t )   21

 The two equations (4) and (7) together are said to be the state model of the system.

 In general, these are written as,


x  Ax  B u - state equation
and y  Cx  Du - output equation

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Definitions concerning state space approach
State
The state of a dynamical system is the minimal amount of information required, together
with initial conditions at t ≥ t0 and input excitation, to completely determine the behaviour
of the system for any time t ≥ t0.
State Variable
The state variables of a dynamical system are the smallest set of variables which determine
the state of the dynamic system. If at least n variables, x1, x2, x3, … , xn, are needed to
completely describe the function behaviour of the system, together with the initial state and
input excitation, then these n variables x1, x2, x3, … , xn, are a set of state variables. Note that
the state variable need not be physically measurable or observable quantities.
State Vector
The n state variables can be considered the n state variables can be considered the n
components of a state vector x(t), described in n-dimensional vector-space. Such a vector is
called a state vector. A state vector is thus a vector that determines uniquely the system
state x(t) for any time t ≥ t0, once the state at t = t0 is given and the input u(t) for t ≥ t0, is
specified.
State Space
The n-dimension space whose coordinate axes consist of the x1-axis, x2-axis, x3-axis, . . . , xn-
axis, where x1, x2, x3, … , xn, are state variables; is called a state space. Any state can be
represented by a point in the state space.
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Block Diagram Representation of State and Output Equations

 The state space representation of multiple inputs multiple outputs (MIMO) system
are given by the state and the output equations:
x  Ax  B u
and y  Cx  Du

 The block diagram of the system based on state and the output equations are shown
in Fig. 2 below:

Fig. 2 : Block diagram representation of the state space equations.

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Electromechanical System

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