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LAPLACE TRANSFORM AND CONTINUOUS-TIME LTI SYSTEMS                  [CHAP. 3



                       where a,,,  equals the maximum real part of  any of  the poles of  X(s). Thus, the ROC is
                       a half-plane to the right of  the vertical line  Reb) = a,,,  in  the s-plane and thus to the
                       right of  all of  the poles of  Xb).
           Property 4:  If  x(t) is  a left-sided  signal, that  is, x(t) = O  for  t > t,  > -=,  then the ROC is of  the
                       form



                       where a,,,  equals the minimum real part of  any of the poles of X(s). Thus, the ROC is
                       a half-plane to the left of  the vertical line Re(s) =amin in the s-plane and thus to the left
                       of  all of  the poles of  X(s).
           Property  5:  If  x(t) is  a  two-sided  signal, that  is,  x(t) is  an  infinite-duration signal  that  is  neither
                       right-sided nor left-sided, then the ROC is of  the form



                       where a, and a, are the real parts of  the two poles of  X(s). Thus, the ROC is a vertical
                       strip in  the s-plane between the vertical lines Re(s) = a, and Re(s) = a,.
               Note  that  Property  1 follows immediately  from  the  definition  of  poles;  that  is,  X(s) is
           infinite at a pole.  For verification  of  the other properties see Probs. 3.2 to 3.7.



           33  LAPLACE TRANSFORMS OF SOME COMMON SIGNALS

           A.  Unit Impulse Function  S( t ):
                 Using Eqs. (3.3) and (1.20), we obtain


                                     J[s(t)] = /- s(t)e-"  dt = 1       all s
                                                 - m

           B.  Unit Step Function u(t 1:










           where O+ = lim, , + €1.
                             "(0

           C.  Laplace Transform Pairs for Common Signals:

                 The Laplace transforms of some common signals are tabulated  in Table 3-1. Instead of
             having  to reevaluate  the  transform of  a  given signal, we  can  simply refer  to such  a  table
             and read out the desired transform.



           3.4  PROPERTIES OF THE LAPLACE TRANSFORM
                 Basic properties of  the Laplace transform are presented in  the following. Verification
             of  these properties is given in  Probs. 3.8 to 3.16.
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