Problem integrating over a sphere.

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Homework Help Overview

The discussion revolves around the computation of a surface integral over a sphere, specifically integrating the vector field \(\vec{F}\) defined in terms of spherical coordinates. The original poster presents their attempt at the solution, noting a discrepancy between their result and the expected answer.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the form of the integrand and the implications of using spherical coordinates versus Cartesian coordinates. There are inquiries about the correctness of the integration limits and the behavior of specific terms in the integrand.

Discussion Status

Some participants have offered alternative perspectives on the integral, suggesting the use of Stokes' theorem and questioning the original poster's integration limits. There is recognition of the odd nature of certain terms in the integrand, leading to discussions about their contributions to the integral.

Contextual Notes

There is a noted confusion regarding the limits of integration for the variable \(\theta\), with some participants pointing out that the range should be from 0 to \(\pi\) instead of 0 to \(\pi/2\). This discrepancy may affect the evaluation of the integral.

S. Moger
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Homework Statement



Compute \int_S \vec{F} \cdot d\vec{S}

\vec{F} = (xz, yz, z^3/a)

S: Sphere of radius a centered at the origin.

Homework Equations



x = a \sin(\theta) \cos(\varphi)
y = a \sin(\theta) \sin(\varphi)
z = a \cos(\theta)

Phi : 0->2 pi, Theta : 0->pi/2 .

The Attempt at a Solution



\vec{F} = a^2 \cos(\theta) \cdot \{ \sin(\theta) \cos(\varphi), \sin(\theta) \sin(\varphi), \cos(\theta)^2 \}

d\vec{S} = \frac{ \partial{\vec{r} }} {\partial{\theta} } \times \frac{ \partial{\vec{r}}}{\partial{\varphi}} d\theta d\varphi = a^2 \sin(\theta) \cdot \{ \sin(\theta) \cos(\varphi), \sin(\theta) \sin(\varphi), \cos(\theta) \}

\int_S \vec{F} \cdot d\vec{S} = \int_\varphi d\varphi \int_\theta ... d\theta = 2 \pi a^4 \int_\theta ... d\theta = 9 \pi a^4 / 10

While the correct answer is \frac{4}{5} \pi a^4 .I'm relatively sure this isn't a book-keeping issue, I double checked the computations manually and with mathematica. Maybe I'm missing something (or maybe there's an easier way to "see" the answer).
 
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What's the integrand you came up with?
 
Stokes' theorem might lead to an easier integral (didn't test it).
$$\vec{F} = a^2 \cos(\theta) \cdot \{ \sin(\theta) \cos(\varphi), \sin(\theta) \sin(\varphi), \cos(\theta)^2 \}$$
This is still in cartesian coordinates? Then it shouldn't have that prefactor.
 
I got this:
\int_S \vec{F} \cdot d\vec{S}= a^4 \int \int \sin(\theta)^3 \cos(\theta) + \sin(\theta) \cos(\theta)^4 d\varphi d\theta

The phi variable "disappears" ( = 1) because of the trigonometric identity, so I separate its integral from the expression involving theta.

The expression for the F-vector should be valid as it stands (in cartesian coordinates). I inserted the expressions for x y z in theta, phi and a, and extracted z.
 
When you integrate the ##\sin^3\theta \cos\theta## term, it'll vanish because the integrand is odd around ##\theta = \pi/2##. Is that what you found? The final answer pops out from the second integral.
 
Ah right, you have the z everywhere.
 
vela said:
When you integrate the ##\sin^3\theta \cos\theta## term, it'll vanish because the integrand is odd around ##\theta = \pi/2##. Is that what you found? The final answer pops out from the second integral.

If I integrate it from 0 to pi/2 I should get 1/4. (It's just \frac{\sin^4{\theta}}{4}, with theta=0 vanishing, if I'm not mistaken). But makes me think about the range (integration limits, not sure about the word for it). But if I spanned -pi/2 to pi/2 I would get zero in any case
 
Oh, I didn't notice you had written down the wrong limits. ##\theta## does indeed go from 0 to ##\pi##, not ##\pi/2##.
 
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Yes, that's it! Thank you very much.
 

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