Page 33 - 4811
P. 33

Properties of Laplace Transform


               immediately recognizable as the Laplace transform of some elementary

               function, such as
                                                                   1
                                                  F(s) =                     ,
                                                            (s − 2)(s − 3)
               for s confined to some region Ω (e.g., Re(s) > α). Just as in calculus (for s real),

               where the goal is to integrate such a function, the procedure required here is to
               decompose the function into partial fractions.
                   There are several different ways for computing constants in partial fractions
               decomposition:
                  1. Method of undetermined coefficients;

                  2. Plug in particular values method;
                  3. Cover up method.
                   The last method is a quick way to determine the coefficients in a partial

               fraction decomposition. The cover up method was popularized by the English

               electrical engineer Oliver Heaviside (1850 - 1925).
                   Recall that to use partial fractions the degree of the polynomial in the
               numerator must be strictly less than the degree of the polynomial in the
               denominator. If it is not then you must first use long division to obtain a quotient

               polynomial and a rational function remainder; the remainder will certainly have
               a denominator of higher degree than the numerator and so partial fractions can
               be used on it.
                   We will be concerned with the quotient of two polynomials, namely a rational

               function
                                                                 P(s)
                                                       F(s) =          ,
                                                                 Q(s)
               where the degree of Q(s) is greater than the degree of P(s), and P(s) and Q(s)
               have no common factors. Then F(s) can be expressed as a finite sum of partial
               fractions.

                  (i) For each linear factor of the form as + b of Q(s), there corresponds a partial
                     fraction of the form
                                                          A
                                                               , A constant.
                                                       as + b
                                                                                     n
                 (ii) For each repeated linear factor of the form (as + b) , there corresponds a
                     partial fraction of the form

                                              A 1          A 2                   A n
                                                     +             + · · · +            ,
                                            as + b      (as + b) 2           (as + b)  n

                     A , A , . . . , A constants.
                            2
                       1
                                      n
                                                                    2
                (iii) For every quadratic factor of the form as +bs+c, there corresponds a partial
                     fraction of the form
                                                    As + b
                                                                , A, B constants.
                                                    2
                                                 as + bs + c
                                                              32
   28   29   30   31   32   33   34   35   36   37   38