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Linear%20Time%20Invariant%20systems

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Use linearity, and a some table entries to conclude: Sign{ } growth or decay ... Use table entries (as before) to conclude: Reformulate y(t) in terms of and. Where: ... – PowerPoint PPT presentation

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Title: Linear%20Time%20Invariant%20systems


1
Linear Time Invariant systems
  • definitions,
  • Laplace transform,
  • solutions,
  • stability

2
Ready to GO !?
  • Disclaimer the following slides are a quick
    review of Linear, Time Invariant systems
  • If you feel a bit disoriented think
  • I can easily read up on it (references will be
    given)
  • Its VERY simple if youve seen it before (i.e.
    intuitive).
  • This part will be over soon.

3
Lumpedness and causality
  • Definition a system is lumped if it can be
    described by a state vector of finite dimension.
    Otherwise it is called distributed.Examples
  • distributed system y(t)u(t-? t)
  • lumped system (mass and spring with friction)
  • Definition a system is causal if its current
    state is not a function of future events (all
    real physical systems are causal)

4
Linearity and Impulse Response description of
linear systems
  • Definition a function f(x) is linear if(this
    is known as the superposition property)
  • Impulse response
  • Suppose we have a SISO (Single Input Single
    Output) system system as follows
  • where
  • y(t) is the systems response (i.e. the observed
    output) to the control signal, u(t) .
  • The system is linear in x(t) (the systems state)
    and in u(t)

5
Linearity and Impulse Response description of
linear systems
  • Define the systems impulse response, g(t,?), to
    be the response, y(t) of the system at time t, to
    a delta function control signal at time ? (i.e.
    u(t)?t,t) given that the system state at time ?
    is zero (i.e. x(?)0 )
  • Then the system response to any u(t) can be found
    by solving
  • Thus, the impulse response contains all the
    information on the linear system

6
Time Invariance
  • A system is said to be time invariant if its
    response to an initial state x(t0) and a control
    signal u is independent of the value of t0.
  • So g(t,?) can be simply described as g(t)g(t,0)
  • A time linear time invariant system is said to be
    causal if
  • A system is said to be relaxed at time 0 if x(0)
    0
  • A linear, causal, time invariant (SISO) system
    that is relaxed at time 0 can be described by

7
LTI - State-Space Description
Fact (instead of using the impulse response
representation..)
  • Every (lumped, noise free) linear, time invariant
    (LTI) system can be described by a set of
    equations of the form

8
What About nth Order Linear ODEs?
  • Can be transformed into n 1st order ODEs
  • Define new variable
  • Then

Dx/dt A
x B
u y I 0 0 ? 0 x

9
Using Laplace Transform to Solve ODEs
  • The Laplace transform is a very useful tool in
    the solution of linear ODEs (i.e. LTI systems).
  • Definition the Laplace transform of f(t)
  • It exists for any function that can be bounded by
    ae?t (and sgta ) and it is unique
  • The inverse exists as well
  • Laplace transform pairs are known for many useful
    functions (in the form of tables and Matlab
    functions)
  • Will be useful in solving differential equations!

10
Some Laplace Transform Properties
  • Linearity (superposition)
  • Differentiation
  • Convolution
  • Integration

11
Some specific Laplace Transforms (good to know)
  • Constant (or unit step)
  • Impulse
  • Exponential
  • Time scaling

12
Using Laplace Transform to Analyze a 2nd Order
system
  • Consider the unforced (homogenous) 2nd order
    system
  • To find y(t)
  • Take the Laplace transform (to get an algebraic
    equation in s)
  • Do some algebra
  • Find y(t) by taking the inverse transform

13
2nd Order system - Inverse Laplace
  • The solution of the inverse depends on the nature
    of the roots ?1,?2 of the characteristic
    polynomial p(s)as2bsc
  • real distinct, b2gt4ac
  • real equal, b24ac
  • complex conjugates b2lt4ac
  • In shock absorber exampleam, bdamping coeff.,
    cspring coeff.
  • We will see Re?? exponential effectIm??
    Oscillatory effect

14
Real Distinct roots (b2gt4ac)
  • Some algebra helps fit the polynomial to Laplace
    tables.
  • Use linearity, and a table entry To conclude
  • Sign? ? growth or decay
  • ? ? rate of growth/decay

15
Real Equal roots (b24ac)
  • Some algebra helps fit the polynomial to Laplace
    tables.
  • Use linearity, and a some table entries to
    conclude
  • Sign? ? growth or decay
  • ? ? rate of growth/decay

16
Complex conjugate roots (b2lt4ac)
  • Some algebra helps fit the polynomial to Laplace
    tables.
  • Use table entries (as before) to conclude
  • Reformulate y(t) in terms of ? and ?Where

17
Complex roots (b2lt4ac)
  • For p(s)s20.35s1 and initial condition
    y(0)1,y(0)0
  • The roots are ??i?-0.175i0.9846
  • The solution has formand the constants
    areA?1.0157r0.5-i0.0889?arctan(Im(r)/Re(r
    )) -0.17591
  • We see the solution is an exponentially
    decaying oscillation where the decay is
    governed by ? and the oscillation by ?.

18
The Roots of a Response
19
(Optional) Reading List
  • LTI systems
  • Chen, 2.1-2.3
  • Laplace
  • http//www.cs.huji.ac.il/control/handouts/laplace
    _Boyd.pdf
  • Also, Chen, 2.3
  • 2nd order LTI system analysis
  • http//www.cs.huji.ac.il/control/handouts/2nd_ord
    er_Boyd.pdf
  • Linear algebra (matrix identities and eigenstuff)
  • Chen, chp. 3
  • Stengel, 2.1,2.2
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