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Let $f(z) = \frac{a_0+a_1z+a_2z^2+a_3z^3+.....+a_{n-1}z^{n-1}}{b_0+b_1z+b_2z^2+b_3z^3+.....+b_{n}z^{n}}$ $b_n \ne0$

Assuming zeroes of denominator to be simple, show that sum of residues of $f(z)$ at it's poles is equal to $\frac{a_{n-1}}{b_n}$

I approached the problem by writing denominator into factors say $(z-c_0)(z-c_1)(z-c_2)....(z-c_n)$

and then adding all residues using $\sum_{i=0}^n\lim \limits_{z\to c_n}{(z-c_n)f(z)}$

However I get stuck with different denominators of each term.

I found a solution where it generalises the formula by showing it true for couple of values of $n$. But this doesn't seem satisfactory enough. Is there a simple way to prove the desired result ?

I tried using Cauchy's integral formula but to no avail as well.

2 Answers2

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The sum of residues is $$\frac1{2\pi i}\int_C f(z)\,dz$$ where $C$ is a large enough circle with centre $0$. Let the radius $R\to\infty$. $$\frac1{2\pi i}\int_C f(z)\,dz=\frac1{2\pi}\int_0^{2\pi} \frac{\cdots+R^{n-1}a_{n-1}e^{i(n-1)t}}{ \cdots+R^nb_ne^{int}}e^{it}R\,dt$$ etc.

Angina Seng
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A slightly different approach which can be very useful e.g. when applying the Egorychev method is to use the fact that for a rational function all residues including the residue at infinity sum to zero. (I don't have a reference ready at this time.) The residue at infinity is given by

$$\mathrm{Res}_{z=\infty} f(z) = - \mathrm{Res}_{z=0} \frac{1}{z^2} f(1/z).$$

This means the sum of the residues at the finite poles is given by

$$\mathrm{Res}_{z=0} \frac{1}{z^2} f(1/z)$$

which in the present case yields

$$\mathrm{Res}_{z=0} \frac{1}{z^2} \frac{a_0+a_1/z+\cdots+a_{n-1}/z^{n-1}}{b_0+b_1/z+\cdots+b_n/z^n} \\ = \mathrm{Res}_{z=0} \frac{1}{z^2} \frac{a_0z^n+a_1z^{n-1}+\cdots+a_{n-1}z}{b_0z^n+b_1z^{n-1}+\cdots+b_n} \\ = \mathrm{Res}_{z=0} \frac{1}{z} \frac{a_0z^{n-1}+a_1z^{n-2}+\cdots+a_{n-1}} {b_0z^n+b_1z^{n-1}+\cdots+b_n}.$$

This is

$$[z^0] \frac{a_0z^{n-1}+a_1z^{n-2}+\cdots+a_{n-1}} {b_0z^n+b_1z^{n-1}+\cdots+b_n}$$

because the denominator is not zero at $z=0$ as per the problem definition. With no pole at zero the constant coefficient can be obtained from the ordinary Taylor series and is equal to

$$\left.\frac{a_0z^{n-1}+a_1z^{n-2}+\cdots+a_{n-1}} {b_0z^n+b_1z^{n-1}+\cdots+b_n}\right|_{z=0} = \frac{a_{n-1}}{b_n}.$$

The rule that residues sum to zero may then be used in a variety of creative ways, for example at this MSE link I where it is applied twice, with the residue at infinity vanishing in the second application as per the integral formula. The same technique is used at this MSE link II. The Egorychev method with a non-zero residue at infinity is applied at this MSE limk III (streamlined proof).

Marko Riedel
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