186 C H A P T E R 3: The Laplace Transform
f(t)=Ae−atu(t)whereain general can be a complex number isF(s)=A
s+aROC:σ >−aThe location of the poles=−aclosely relates to the signal. For instance, ifa=5,f(t)=Ae−^5 tu(t)is
a decaying exponential and the pole ofF(s)is ats=−5 (in left-hands-plane); ifa=−5, we have an
increasing exponential and the pole is ats=5 (in right-hands-plane). The larger the value of|a|the
faster the exponential decays (fora>0) or increases (fora<0); thus,Ae−^10 tu(t)decays a lot faster
thatAe−^5 tu(t), andAe^10 tu(t)grows a lot faster thanAe^5 tu(t).The Laplace transformF(s)= 1 /(s+a)off(t)=e−atu(t), for any real value ofa, has a pole on the real
axisσof thes-plane, and we have the following three cases:n Fora=0, the pole at the origins=0 corresponds to the signalf(t)=u(t), which is constant for
t≥0 (i.e., it does not decay).
n Fora>0, the signal isf(t)=e−atu(t), a decaying exponential, and the poles=−aofF(s)is in
the real axisσof the left-hands-plane. As the pole is moved away from the origin toward the left,
the faster the exponential decays, and as it moves toward the origin, the slower the exponential
decays.
n Fora<0, the poles=−ais on the real axisσof the right-hands-plane, and corresponds to
a growing exponential. As the pole moves to the right the exponential grows faster, and as it is
moved toward the origin it grows at a slower rate—clearly this signal is not useful, as it grows
continuously.The conclusion is that theσaxis of the Laplace plane corresponds to damping. A single pole on this axis
and in the left-hands-plane corresponds to a decaying exponential, and a single pole on this axis and in the
right-hands-plane corresponds to a growing exponential.Suppose then we considerg(t)=Acos( 0 t)u(t)=Aej^0 t
2u(t)+Ae−j^0 t
2u(t)and leta=j 0 to expressg(t)asg(t)=0.5[Aeatu(t)+Ae−atu(t)]Then, by the linearity of the Laplace transform and the previous result we obtainG(s)=A
2
1
s−j 0+
A
2
1
s+j 0=
As
s^2 +^20(3.9)
with a zero ats=0, and the poles are values for whichs^2 +^20 = 0 ⇒s^2 =−^20 or s1,2=±j 0