How can I find this surface integral in cylindrical coordina

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SUMMARY

The discussion focuses on calculating the surface integral of a vector field $\vec F$ defined in cylindrical coordinates, specifically through the closed surface bounded by the cylinders $\rho = a$ and $\rho = 2a$, and the planes $z = \pm \frac{a\pi}{2}$. The vector field is expressed as $\vec F = \frac{F_0 \rho}{a} \cos(\lambda z) \hat{\rho} + F_0 \sin(\lambda z) \hat{k}$. Participants seek clarity on representing the unit normal vector and infinitesimal area elements for the surface integral, and whether to compute four separate integrals for the inner and outer surfaces as well as the caps. The divergence theorem is also suggested for evaluating the integral.

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John004
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Homework Statement


A vector field $\vec F$ is defined in cylindrical polar coordinates $\rho , \theta , z$ by

$\vec F = F_0(\frac{xcos (\lambda z)}{a}\hat i \ + \frac{ycos(\lambda z)}{a}\hat j \ + sin(\lambda z)\hat k) \ \equiv \frac{F_0 \rho}{a}cos(\lambda z)\hat \rho \ + F_0sin(\lambda z)\hat k $

where $\hat i$ , $\hat j$ , and $\hat k$ are the unit vectors along the cartesian axes and $\hat \rho$ is the unit vector $\frac{x}{\rho}\hat i \ + \frac{y}{\rho}\hat j$.

(a) Calculate, as a surface integral, the flux of $\vec F$ through the closed surface bounded by the cylinders $\rho = a$ and $\rho = 2a$ and the planes $z =\pm \frac{a\pi}{2} $.

(b) Evaluate the same integral using the divergence theorem.

So I am pretty lost on how to even begin part (a). I sketched a picture of the situation and am I kinda confused as to how to represent the unit normal vector, as well as the infinitesimal area elements. Am I supposed to take four separate integrals and sum them afterwards, one for the inner and outer curved surfaces, and one for the upper and lower caps?
 
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I see that this is marked solved, so I haven't commented. I just fixed the text to make it readable. @John004: use ## instead of $ to delimit inline Latex.

John004 said:

Homework Statement


A vector field ##\vec F## is defined in cylindrical polar coordinates ##\rho , \theta , z## by

$$\vec F = F_0(\frac{xcos (\lambda z)}{a}\hat i \ + \frac{ycos(\lambda z)}{a}\hat j \ + sin(\lambda z)\hat k) \ \equiv \frac{F_0 \rho}{a}cos(\lambda z)\hat \rho \ + F_0sin(\lambda z)\hat k $$

where ##\hat i## , ##\hat j## , and ##\hat k## are the unit vectors along the cartesian axes and ##\hat \rho## is the unit vector ##\frac{x}{\rho}\hat i \ + \frac{y}{\rho}\hat j##.

(a) Calculate, as a surface integral, the flux of ##\vec F## through the closed surface bounded by the cylinders ##\rho = a## and ##\rho = 2a## and the planes ##z =\pm \frac{a\pi}{2} ##.

(b) Evaluate the same integral using the divergence theorem.

So I am pretty lost on how to even begin part (a). I sketched a picture of the situation and am I kinda confused as to how to represent the unit normal vector, as well as the infinitesimal area elements. Am I supposed to take four separate integrals and sum them afterwards, one for the inner and outer curved surfaces, and one for the upper and lower caps?
 

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