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082-Engineering-Mathematics-Anthony-Croft-Robert-Davison-Martin-Hargreaves-James-Flint-Edisi-5-2017

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660 Chapter 21 The Laplace transform

G(s). Therefore, forEquation (21.5),

G(s) = 1

1 +s

The concept of a transferfunction isvery usefulinengineering. Itprovides a simple

algebraic relationship between the input and the output. In other words, it allows the

analysisofdynamicsystemsbasedonthedifferentialequationtoproceedinarelatively

straightforward manner. Earlier we noted that it was necessary to assume zero initial

conditions in order to form the transfer function. Without such an assumption, the relationship

between the input and the output would have been more complicated. What

is more, the relationship would vary depending on how much energy is stored in the

system at t = 0. By assuming zero initial conditions, the transfer function depends

purely on the system characteristics. Such an approach, whilst very convenient, does

have its limitations. The transfer function approach is useful for analysing the effect of

aninputtothesystem.However,ifonerequirestheeffectofthecombinationofasystem

inputand initial conditions,thenitisnecessarytocarryoutafullsolution ofthedifferential

equation as we did in Section 21.10. In practice there are many cases where the

simplified treatment provided by the transfer function is perfectly acceptable. An alternativeapproachisprovidedbystate-spacemodels,whichweexaminedinSection20.4.

Theseprovideanaturalwayofhandlinginitialconditions.Inordertosolveastate-space

model wherethereareinitialconditions,allthatisnecessaryistouseanon-zeroinitial

valueofthestatevector.RecallthatinSection20.4weonlysetupthestate-spacemodels

and did not solve them. However, the method for the standard solution of a state-space

model can befound inmany advanced textbooks on control and systems engineering.

Example21.28 Findthetransferfunctionsofthefollowingequationsassumingthat f (t)representsthe

inputandx(t) represents the output:

(a)

(b)

dx(t)

dt

d 2 x(t)

dt 2

−4x(t) =3f(t), x(0) =0

+3 dx(t)

dt

−x(t) = f(t),

dx(0)

dt

=0, x(0)=0

Solution (a) Taking Laplace transforms ofthe differential equation gives

sX(s) −x(0) −4X(s) =3F(s)

(s −4)X(s) =3F(s) asx(0) =0

X(s)

F(s) =G(s) = 3

s −4

(b) Taking Laplace transforms ofthe differential equation gives

s 2 X(s) −sx(0) − dx(0) +3(sX(s) −x(0)) −X(s) =F(s)

dt

(s 2 +3s −1)X(s) =F(s) as dx(0) =0 and x(0)=0

X(s)

F(s) =G(s) = 1

s 2 +3s−1

dt

Whencreatingamathematicalmodelofanengineeringsystemitisoftenconvenientto

thinkofthevariableswithinthesystemassignalsandelementsofthesystemasmeans

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