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Partial Fraction Expansion via Differentiation

Module by: Steven Cox

Summary: (Blank Abstract)

Introduction and Terminology

With the tools of complex functions we may produce complex polynomials:

fz=zm+ c m - 1 zm-1++ c 1 z+ c 0 f z z m c m - 1 z m 1 c 1 z c 0 (1)
We say that such an ff is of order mm. We shall often find it convenient to represent polynomials as the product of their factors, namely:
fz=z- λ 1 d 1 z- λ 2 d 2 z- λ h d h f z z λ 1 d 1 z λ 2 d 2 z λ h d h (2)
Each λ j λ j is a root of degree d j d j . Here hh is the number of distinct roots of ff. We call λ j λ j a simple root when d j =1 d j 1 . We can observe the appearance of ratios of polynomials or so called rational functions. Suppose qz=fzgz q z f z g z is rational, that f f is of order at most m-1 m 1 while g g is of order m m with the simple roots λ 1 λ m λ 1 λ m .

Simple Roots

It should come as no surprise that such a q q should admit a Partial Fraction Expansion

qz=j=1m q k z- λ j q z j 1 m q k z λ j (3)

One uncovers the q j q j by first multiplying each side by z- λ j z λ j and then letting z z tend to λ j λ j . For example, if

1z2+1= q 1 z+i+ q 2 z-i 1 z 2 1 q 1 z i q 2 z i (4)
then multiplying each side by z+i z i produces
1z-i= q 1 + q 2 z+iz-i 1 z i q 1 q 2 z i z i (5)
Now, in order to isolate q 1 q 1 it is clear that we should set z=-i z i . So doing we find q 1 =i2 q 1 i 2 . In order to find q 1 q 1 we multiply the above equality by z-i z i and then set z=i z i . So doing we find q 2 =-i2 q 2 i 2 , and so
1z2+1=i2z+i+-i2z-i 1 z 2 1 i 2 z i i 2 z i (6)
Returning to the general case, we encode the above in the simple formula
q j =limz λ j z- λ j qz q j z λ j z λ j q z (7)
You should be able to use this to confirm that
zz+12=1/2z+1+1/2z-1 z z 1 2 12 z 1 12 z 1 (8)

Multiple Roots

q 1 , 1 q 1 , 1 and q 1 , 2 q 1 , 2 in the expansion

z+2z+12= q 1 , 1 z+1+ q 1 , 2 z+12 z 2 z 1 2 q 1 , 1 z 1 q 1 , 2 z 1 2 (9)
Arguing as above it seems wise to multiply through by z+12 z 1 2 and so arrive at
z+2= q 1 , 1 z+1+ q 1 , 2 z 2 q 1 , 1 z 1 q 1 , 2 (10)
On setting z=-1 z -1 this gives q 1 , 2 =1 q 1 , 2 1 . With q 1 , 2 q 1 , 2 computed the previous equation takes the simple form
z+1= q 1 , 1 z+1 z 1 q 1 , 1 z 1 (11)
and so q 1 , 1 =1 q 1 , 1 1 as well. Hence:
z+2z+12=1z+1+1z+12 z 2 z 1 2 1 z 1 1 z 1 2 (12)

This latter step grows more cumbersome for roots of higher degree. Let us consider

z+22z+13= q 1 , 1 z+1+ q 1 , 2 z+12+ q 1 , 3 z+13 z 2 2 z 1 3 q 1 , 1 z 1 q 1 , 2 z 1 2 q 1 , 3 z 1 3 (13)
The first step is still correct: multiply through by the factor at its highest degree, here 3 3. This leaves us with
z+22= q 1 , 1 z+12+ q 1 , 2 z+1+ q 1 , 3 z 2 2 q 1 , 1 z 1 2 q 1 , 2 z 1 q 1 , 3 (14)
Setting z=-1 z -1 again produces the last coefficient, here q 1 , 3 =1 q 1 , 3 1 . We are left however with one equation in two unknowns. Well, not really one equation, for the previous equation is to hold for all z z. We exploit this by taking two derivatives, with respect to z z, of this equation. This produces
2z+2=2 q 1 , 1 z+1+ q 1 , 2 2 z 2 2 q 1 , 1 z 1 q 1 , 2 (15)
and
2= q 1 , 1 2 q 1 , 1 (16)
The latter of course needs no comment. We derive q 1 , 2 q 1 , 2 from the former by setting z=-1 z -1 . This example will permit us to derive a simple expression for a partial fraction expansion.
Definition 1: Partial Fraction Expansion
The partial fraction expansion of a general proper rational function q=fg q f g where g g has h h distinct roots λ 1 λ h λ 1 λ h of respective degrees d 1 d h d 1 d h can be written as qz=j=1hk=1 d j q j , k z- λ j k q z j 1 h k 1 d j q j , k z λ j k and it can be noted, as above, that q j , k q j , k is the coefficient of z- λ j d j -k z λ j d j k in the rational function r j zqzz- λ j d j r j z q z z λ j d j . Hence, q j , k q j , k may be computed by setting z= λ j z λ j in the ratio of the d j -k d j k th derivative of r j r j to d j -k! d j k . That is, q j , k =limz λ j 1 d j -k!d d j -kdz d j -kz- λ j d j qz q j , k z λ j 1 d j k z d j k z λ j d j q z .

Connection to Residues

With respect to the previous definition observe that if we choose r j r j so small that λ j λ j is the only zero of g g encircled by R j C λ j r j R j C λ j r j then by Cauchy's Theorem

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