1540470959-Boundary_Value_Problems_and_Partial_Differential_Equations__Powers

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372 Chapter 6 Laplace Transform


The algebraic determination of theA’s is very tedious, but notice that


(s−r 1 )q(s)
p(s)

=A 1 +A 2 s−r^1
s−r 2

+···+Aks−r^1
s−rk

.

Ifsis set equal tor 1 , the right-hand side is justA 1. The left-hand side becomes
0 /0, but L’Hôpital’s rule gives


slim→r
1

(s−r 1 )q(s)
p(s)

=slim→r
1

(s−r 1 )q′(s)+q(s)
p′(s)

=q(r^1 )
p′(r 1 )

.

ThereforeA 1 and all the otherA’s are given by


Ai=

q(ri)
p′(ri).

Consequently, our rational function takes the form


q(s)
p(s)=

q(r 1 )
p′(r 1 )

1

s−r 1 +···+

q(rk)
p′(rk)

1

s−rk.

From this point we can easily obtain the inverse transform, as expressed in the
conclusion of the following theorem.


Theorem 1.Let p and q be polynomials, q of lower degree than p, and let p have
only simple roots, r 1 ,r 2 ,...,rk.Then


L−^1

(q(s)
p(s)

)

=

q(r 1 )
p′(r 1 )exp(r^1 t)+···+

q(rk)
p′(rk)exp(rkt). (2)

(Equation(2)is known as Heaviside’s formula.) 


Let us apply the theorem to the example in whichq(s)=s+4,p(s)=s^2 +
3 s+2,p′(s)= 2 s+3. Then


L−^1

(

s+ 4
s^2 + 3 s+ 2

)

= −^1 +^4

2 (− 1 )+ 3

e−t+ −^2 +^4
2 (− 2 )+ 3

e−^2 t= 3 e−t− 2 e−^2 t.

In nonhomogeneous differential equations also, the Laplace transform is a
useful tool. To solve the problem


u′+au=f(t), u( 0 )=u 0 ,

we again transform the entire equation, obtaining


sU−u 0 +aU=F(s),
U(s)= u^0
s+a

+^1

s+a

F(s).
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