How Do Double Integrals and Polar Coordinates Relate to Symmetry Arguments?

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SUMMARY

The discussion focuses on the relationship between double integrals and polar coordinates in the context of symmetry arguments. The unit disk is defined as S = {(x, y) | x² + y² ≤ 1}, and its transformation into polar coordinates is given by S = { (ρ cos(θ), ρ sin(θ)) | ρ ≤ 1, 0 ≤ θ ≤ 2π }. The integral of the function xy√(x² + y²) over the disk is evaluated using polar coordinates, leading to the conclusion that symmetry can simplify the evaluation of integrals without detailed calculations. The discussion also highlights that the same symmetry argument applies when considering a closed disk with a different center.

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jenc305
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Please help. Thank you.
 

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Alright. The unit disk is

S = \{(x, \ y) | x^2 + y^2 \leq 1 \}

Changing to polar coordinates,

S = \{ (\rho \cos{\theta}, \ \rho \sin{\theta}) | \rho \leq 1, \ 0 \leq \theta \leq 2\pi \}

ie. x = \rho \cos{\theta}, \ y = \rho \sin{\theta}.

Thus

\int \int_S xy\sqrt{x^2 + y^2} dA = \int_0^{2\pi} \int_0^1 \rho \sin{\theta}\rho \cos{\theta} \sqrt{\rho^2 \sin^2{\theta} + \rho^2 \cos^2{\theta}} \ \left|\frac{\partial (x, \ y)}{\partial(\rho, \ \theta)}\right| \ d\rho \ d\theta = \int_0^{2\pi} \int_0^1 \rho^4\cos{\theta}\sin{\theta} \ d\rho \ d\theta

I trust you can work out the rest.

I will note that it is quite easy to evaluate this integral without actually doing any calculations, by appealing to symmetry.
 
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What if D is a closed disk with radius 1 and center (1,0).
That would make the polar coord. x=(r cos(theta)-1) and y=(r sin (theta)).
 
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It's actually still the same answer. You can make the same symmetry argument.

Here's a hint:

Obviously, if f is 2\pi-periodic, then \int_0^{2\pi} f(x)\sin{x} \ dx = \int_{-\pi}^{\pi} f(x)\sin{x} \ dx. Thus if f is an even function, since \sin is odd, then f(x)\sin{x} is odd and

\int_0^{2\pi} f(x)\sin{x} \ dx = 0
 
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