MHB Using Residue Calculus For a General Cosine Angle

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The discussion focuses on using residue calculus to evaluate the integral of the form $$\int_{0}^{2\pi}\frac{1}{a+b\cos( \theta) } \mathrm{d}\theta$$ for the condition |b|<|a|. The integral is transformed using the substitution $$z=\exp(i\theta)$$, leading to a contour integral representation. Participants discuss the factorization of the polynomial $$bz^2 + 2az + b = 0$$ to identify the roots and their locations relative to the unit circle. The final evaluation of the integral hinges on determining the residues at the poles inside the contour, with the conclusion that the integral evaluates to $$\frac{2\pi}{\sqrt{a^2 - b^2}}$$ when the conditions are satisfied. The conversation emphasizes the importance of correctly identifying poles and their contributions to the integral.
shen07
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Hi, I am supposed to use residue calculus to do the following integral

$$\int_{0}^{2\pi}\frac{1}{a+b\cos( \theta) } \mathrm{d}\theta$$ for
|b|<|a|​

i have paremetrise it on $$\gamma(0;1)$$ that is $$z=\exp(i\theta), 0\leq\theta\leq2\pi$$ and obtain the following

$$\int_{0}^{2\pi}\frac{1}{a+b\cos( \theta) } \mathrm{d}\theta=\frac{2}{i}\int_{\gamma(0;1)}\frac{1}{bz^2+2az+b}\mathrm{d}z$$

Now i have to factorise it so that i know where the roots are holomorphic,

i.e i have to solve $$bz^2+2az+b=0$$

Please help me, I am stuck.
 
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shen07 said:
Hi, I am supposed to use residue calculus to do the following integral

$$\int_{0}^{2\pi}\frac{1}{a+b\cos( \theta) } \mathrm{d}\theta$$ for
|b|<|a|​

i have paremetrise it on $$\gamma(0;1)$$ that is $$z=\exp(i\theta), 0\leq\theta\leq2\pi$$ and obtain the following

$$\int_{0}^{2\pi}\frac{1}{a+b\cos( \theta) } \mathrm{d}\theta=\frac{2}{i}\int_{\gamma(0;1)}\frac{1}{bz^2+2az+b}\mathrm{d}z$$

Now i have to factorise it so that i know where the roots are holomorphic,

i.e i have to solve $$bz^2+2az+b=0$$

Please help me, I am stuck.

$\displaystyle \begin{align*} b\,z^2 + 2a\,z + b &= 0 \\ z &= \frac{-2a \pm \sqrt{\left( 2a \right) ^2 - 4 \left( b \right) \left( b \right) }}{2b} \\ z &= \frac{-2a \pm \sqrt{ 4a^2 - 4b^2 }}{2b} \\ z &= \frac{-2a \pm 2\sqrt{ a^2 - b^2} }{2b} \\ z &= \frac{ -a \pm \sqrt{ a^2 - b^2 } }{b} \end{align*}$
 
Prove It said:
$\displaystyle \begin{align*} b\,z^2 + 2a\,z + b &= 0 \\ z &= \frac{-2a \pm \sqrt{\left( 2a \right) ^2 - 4 \left( b \right) \left( b \right) }}{2b} \\ z &= \frac{-2a \pm \sqrt{ 4a^2 - 4b^2 }}{2b} \\ z &= \frac{-2a \pm 2\sqrt{ a^2 - b^2} }{2b} \\ z &= \frac{ -a \pm \sqrt{ a^2 - b^2 } }{b} \end{align*}$

I tried this out but then which root lied inside $$\gamma(0;1)$$ and how do i evaluate the residue using this expression. Or should i simply do a Laurent Series to Obtain the coefficient of $$C_{-1}$$
 
shen07 said:
Hi, I am supposed to use residue calculus to do the following integral

$$\int_{0}^{2\pi}\frac{1}{a+b\cos( \theta) } \mathrm{d}\theta$$ for
|b|<|a|​

i have paremetrise it on $$\gamma(0;1)$$ that is $$z=\exp(i\theta), 0\leq\theta\leq2\pi$$ and obtain the following

$$\int_{0}^{2\pi}\frac{1}{a+b\cos( \theta) } \mathrm{d}\theta=\frac{2}{i}\int_{\gamma(0;1)}\frac{1}{bz^2+2az+b}\mathrm{d}z$$

Now i have to factorise it so that i know where the roots are holomorphic,

i.e i have to solve $$bz^2+2az+b=0$$

Please help me, I am stuck.

Very well!... if the integral is...

$\displaystyle \int_{0}^{2\ \pi} \frac{d \theta}{a + b\ \cos \theta}\ (1)$

... then the substitution $\displaystyle z= e^{i\ \theta}\ \implies d \theta = \frac{d z}{i\ z}, \cos \theta= \frac{z+ \frac{1}{z}}{2}$ leads to...

$\displaystyle \int_{0}^{2\ \pi} \frac{d \theta}{a + b\ \cos \theta} = \frac{2}{i}\ \int_{\gamma} \frac{z\ d z}{b\ z^{2} + 2\ a\ z + b}\ (3)$

Kind regards

$\chi$ $\sigma$
 
On closer inspection, it appears you're missing quite a lot. What is your contour? To perform contour integration you need a closed contour, all you have is an arc...
 
Prove It said:
On closer inspection, it appears you're missing quite a lot. What is your contour? To perform contour integration you need a closed contour, all you have is an arc...

No, i don't agree with you. when You Paremetrise $$\theta$$ on $$\gamma(0;1)$$ you have a circle centre 0 and radius 1.

- - - Updated - - -

chisigma said:
Very well!... if the integral is...
$\displaystyle \int_{0}^{2\ \pi} \frac{d \theta}{a + b\ \cos \theta} = \frac{2}{i}\ \int_{\gamma} \frac{z\ d z}{b\ z^{2} + 2\ a\ z + b}\ (3)$

Kind regards

$\chi$ $\sigma$

there is a z surplus in ur Numerator.. its $$ \frac{2}{i}\ \int_{\gamma} \frac{\ d z}{b\ z^{2} + 2\ a\ z + b}\$$
 
shen07 said:
No, i don't agree with you. when You Paremetrise $$\theta$$ on $$\gamma(0;1)$$ you have a circle centre 0 and radius 1.

Ah I see, I interpreted this as something else...
 
I'm assuming that $a$ and $b$ are positive parameters.

$$ \frac{2}{i} \int_{|z|=1} \frac{1}{bz^{2}+2az+b} \ dz = \frac{2}{i} \int_{|z|=1} \frac{1}{b(z+\frac{a}{b} - \frac{\sqrt{a^{2}-b^{2}}}{b})(z+ \frac{a}{b} + \frac{\sqrt{a^{2}-b^{2}}}{b})} $$

$$ = \frac{2}{ib} \int_{|z|=1} \frac{1}{(z+r-\sqrt{r^{2}-1})(z+r+\sqrt{r^{2}-1})}$$

where $r=\frac{a}{b}$If $r < 1$, both $|r- \sqrt{r^{2}-1}|$ and $|r+\sqrt{r^{2}-1}|$ equal 1. So there are poles on the unit circle and the integral doesn't converge.If $ r >1$, $|r- \sqrt{r^{2}-1}| <1$ and $|r+\sqrt{r^{2}-1}| >1$. So the only pole inside of the unit circle is at $z=-r+\sqrt{r^{2}-1}$.So for $r>1$ (i.e., for $a>b$),

$$\frac{2}{i} \int_{|z|=1} \frac{1}{bz^{2}+2az+b} \ dz = 2 \pi i \lim_{z \to \ -r + \sqrt{r^{2}-1}} \frac{2}{ib} \frac{1}{z+r+\sqrt{r^{2}-1}}$$

$$= \frac{4 \pi}{b} \frac{1}{2\sqrt{r^{2}-1}} = \frac{2 \pi}{\sqrt{a^{2}-b^{2}}} $$
 
Last edited:
Random Variable said:
I'm assuming that $a$ and $b$ are positive parameters.

$$ \frac{2}{i} \int_{|z|=1} \frac{1}{bz^{2}+2az+b} \ dz = \frac{2}{i} \int_{|z|=1} \frac{1}{b(z+\frac{a}{b} - \frac{\sqrt{a^{2}-b^{2}}}{b})(z+ \frac{a}{b} + \frac{\sqrt{a^{2}-b^{2}}}{b})} $$

$$ = \frac{2}{ib} \int_{|z|=1} \frac{1}{(z+r-\sqrt{r^{2}-1})(z+r+\sqrt{r^{2}-1})}$$

where $r=\frac{a}{b}$If $r < 1$, both $|r- \sqrt{r^{2}-1}|$ and $|r+\sqrt{r^{2}-1}|$ equal 1. So there are poles on the unit circle and the integral doesn't converge.If $ r >1$, $|r- \sqrt{r^{2}-1}| <1$ and $|r+\sqrt{r^{2}-1}| >1$. So the only pole inside of the unit circle is at $z=-r+\sqrt{r^{2}+1}$.So for $r>1$ (i.e., for $a>b$),

$$\frac{2}{i} \int_{|z|=1} \frac{1}{bz^{2}+2az+b} \ dz = 2 \pi i \lim_{z \to \ -r + \sqrt{r^{2}+1}} \frac{2}{ib} \frac{1}{z+r+\sqrt{r^{2}-1}}$$

$$= \frac{4 \pi}{b} \frac{1}{2\sqrt{r^{2}-1}} = \frac{2 \pi}{\sqrt{a^{2}-b^{2}}} $$
Ahh that's exactly what i was looking for as answer, Thanks a lot.
 

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