Posting a Divergence Theorem problem shortly.
Is n just the surface normal of the given solid, or what exactly is n?
Okay, and dS is just the surface differential, right?
Okay, so this is just a section of a cone.
How do I find the normal vector in this situation?
Oh! Do I take the gradient vector of the surface and divide it by its magnitude?
\[\triangledown S=\frac{2x i+2yj-2zk}{?}\]I'd get something like rho in spherical coordinates in the denominator when I took the magnitude, how do I deal with that?
(?)
@Kainui
Well the normal vector is just a radial vector. You can always convert to spherical coordinates, which is probably your best bet. Sorry I'm reading a book so I'm not really all here right now.
No problem, I've got three hours before my final and then I'll be in the immediate timeframe done with worrying over this, I just need to remember and figure out enough prior.
Well, it's close to a good conversion, but not quite because of the minus sign in there; I'm wondering if anybody else has a good idea. @zepdrix
Wait you said this was a cone?
Yeah, it's a cone when graphed, x^2+y^2=z^2; I think I figured out n, the denominator will be a constant when the constraints are involved
nevermind, I'm still not really sure about n..
Oh sorry my bad I misread it and though it as a sphere. You're better off in cylindrical coordinates.
|dw:1418211510984:dw| I don't know if this picture helps, but essntially the downward component is constant while the other one changes direction as you change angle.
I'm just trying to figure out the meaningful math behind that; both the k and j component are constant, I read it as, but I don't know how to translate that into math, right now.
So the z component is constant, while the x and y components are not.
So find the slope of a line perpendicular to the surface of the cone, normalize it, and allow the component in the xy plane to be spread out with sintheta and cos theta.
So it'll look like this I think. I think I might have it pointing in the wrong direction, so add some negative signs in there or whatever to fix it \[\large \bar n = \frac{\sqrt{2}}{2}\cos \theta \ \hat i+\frac{\sqrt{2}}{2}\sin \theta \ \hat j+\frac{\sqrt{2}}{2} \hat k\]
(Lord help me jesus)
This exam is about to be a lot of not-good if I can't figure out a systematic way to find n prior.
Thank you for helping me so far.
You're thinking too had about the integrals when really you should be visualizing the objects and concepts. I mean, I can't really help you there, but I find it too difficult to try to do it how you're thinking. I mean, a cone is truly something independent of a coordinate system. You just have to choose whatever coordinate system has the most symmetry in common with your object of interest.
Yeah, I know that's not what you want to be reading lol sorry.
No problem, I understand that cylindrical coordinate systems would be fantastic for this, I just need to learn how to *SYSTEMATICALLY FIND N* regardless of what that is, lol. I think I'm going to go sulk in a corner/use the bathroom for like 10 minutes.
You can take the cross product to find the normal vector, and then divide by the magnitude.
BAM
See, that makes sense to me, lol. What two vectors should I be taking the cross product of?
?
hey still stuck on this ?
Focusing purely on conceptuals now. If you want to take a shot, go for it, one hour and a half prior to my exam.
part a or part b ?
il give you the solution may be if it helps
Yeah, that would help, right now I'm trying my best not to do problems but run through a ton of worked problems and observe how they were done.
part b : \[\vec{v} = \langle yz,-xz,z^2\rangle\] \[\mathrm{div}(\vec{v}) = 0+0+2z = 2z\] \[\begin{align}\iint_S \vec{v}\cdot \vec{n}dS &= \iiint_D 2z ~dV\\~\\ &= \int\limits_{0}^{2\pi}\int\limits_0^{\pi/4}\int\limits_{\sec\phi}^{2\sec\phi } 2\rho \cos\phi ~\rho^2\sin\phi d\rho d\phi d\theta\\~\\ &= \int\limits_{0}^{2\pi}\int\limits_0^{\pi/4}\int\limits_{\sec\phi}^{2\sec\phi } ~\rho^3 \sin(2\phi ) d\rho d\phi d\theta\\~\\ &= \frac{15\pi}{2} \end{align} \]
see if that makes more or less sense (dont wry about evaluating the integral for now, just see if you're comfortable with the setup)
part a : S1 = curved surface \[f(x,y,z) = x^2+y^2-z^2\] \[\hat{n}dS =-\dfrac{\langle 2x,2y,-2z \rangle }{\langle 2x,2y,-2z \rangle \cdot\langle 0,0,1\rangle } = \dfrac{\langle x,y,-z\rangle }{z} ~dxdy\] \[\begin{align}\iint_S \vec{v}\cdot \vec{n}dS &= \iint_S \langle yz,-xz,z^2\rangle \cdot \dfrac{\langle x,y,-z\rangle }{z} ~dxdy\\~\\ &=\iint_S -z^2 ~dxdy\\~\\ &=-\iint_S x^2+y^2 ~dxdy\\~\\ &=-\int\limits_0^{2\pi}\int\limits_{1}^2 r^2~rdrd\theta \\~\\ &= - \frac{15\pi}{2} \end{align} \]
part a : S2 = bottom plane ( z = 1) \[\hat{n}dS = \langle 0,0,-1\rangle ~dxdy\] \[\begin{align}\iint_S \vec{v}\cdot \vec{n}dS &= \iint_S \langle yz,-xz,z^2\rangle \cdot \langle 0,0,-1\rangle ~dxdy\\~\\ &=\iint_S -z^2 ~dxdy\\~\\ &=-\iint_S 1 ~dxdy\\~\\ &=-\pi \end{align} \]
part a : S3 = top plane ( z = 2) \[\hat{n}dS = \langle 0,0,1\rangle ~dxdy\] \[\begin{align}\iint_S \vec{v}\cdot \vec{n}dS &= \iint_S \langle yz,-xz,z^2\rangle \cdot \langle 0,0,1\rangle ~dxdy\\~\\ &=\iint_S z^2 ~dxdy\\~\\ &=\iint_S 2^2 ~dxdy\\~\\ &=16\pi \end{align} \]
total flux out of closed surface = S1 + S2 + S3 \[-\frac{15\pi}{2} -\pi + 16\pi = \frac{15\pi}{2}\] which checks out with the part a so we are good!
Ignore messages in this thread. I'm using OpenStudy's built-in LaTeX editor for the moment for other purposes.
okie.. there is another freindly editor online which i dont like but i see many ppl using it here http://www.codecogs.com/latex/eqneditor.php
Yeah, I'm aware of that one, I don't like it either, heh. Ended up just waiting until TeX studio and MiKTeX were up and running.
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