Calculating mass by double integral

Sami Lakka
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Homework Statement


The distribution of mass on the hemispherical shell z=(R2 - x2 -y2)1/2 is given by
\sigma= (\sigma0/R2)*(x2+y2)
where \sigma0 is constant. Find an expression in terms of \sigma0 and R for the total mass of the shell


Homework Equations


The mass is given by double integral over hemispherical shell


The Attempt at a Solution



\int\int\sigma0/R2(x2+y2)dS
Switch to polar coordinates: x2+y2=r2

\int\int\sigma0/R2*r2*r*dr*d0

After the iterated integral over region 0->2\Pi and 0->R I get answer:
Mass = (\Pi*R2*\sigma0)/2

However the book that I'm studying (Div,Grad,Curl and all that, problem II-6) says that right answer is: (4*\Pi*R2*\sigma0)/3

What goes wrong?
 
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In spherical coordinates, with \rho= R x= R cos(\theta)sin(\phi) and y= R sin(\theta)sin(\phi) so x^2+ y^2= R^2 sin^2(\phi)[/math] and your density function is given by <br /> \frac{\sigma_0}{R}\R^2 sin^2(\phi)<br /> <br /> Since the integration is over the upper half spherical shell, the integration is for \theta from 0 to 2\pi and for \phi from 0 to [math]\pi/2[/math]. <br /> <br /> Finally, the &quot;differential of surface area&quot; for a sphere, of radius R, is [math]R^2 sin(\phi) d\theta d\phi[/math]. <br /> <br /> So the mass of the shell is given by <br /> \frac{\sigma_0}{R}\R^2 \int_{\theta= 0}^{2\pi}\int_{\phi= 0}^{\pi/2} sin^2(\phi)(R^2 sin^2(\phi) d\theta d\phi<br /> = \sigma_0\int_{\theta= 0}^{2\pi}\int_{\phi= 0}^{\pi/2} sin^4(\phi)d\theta d\phi<br /> since the &quot;R<sup>2</sup>&quot; terms cancel out.
 
There are two things I don't understand about this problem. First, when finding the nth root of a number, there should in theory be n solutions. However, the formula produces n+1 roots. Here is how. The first root is simply ##\left(r\right)^{\left(\frac{1}{n}\right)}##. Then you multiply this first root by n additional expressions given by the formula, as you go through k=0,1,...n-1. So you end up with n+1 roots, which cannot be correct. Let me illustrate what I mean. For this...
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