[Mathematical physics] - Integral problem

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The integral problem involves calculating the surface integral of a vector field over a sphere. The correct expression for the surface element is derived using the cross product of partial derivatives, which defines the unit normal vector. The second term in the integrand does not contribute to the integral, and the divergence theorem may be relevant but is not required for this calculation. Confusion arises regarding the normal vector and the application of integral theorems. A clear understanding of the surface element and the properties of the vector field is essential for solving the problem.
Mulz
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Homework Statement


Calculate the integral

\int_{S} (\frac{A}{r^2}\hat{r} + B\hat{z}) \cdot d\vec{S}

Where S is the sphere with r = a.

2. The attempt at a solution

I have no clue how to solve this problem. I have thought of introducing spherical coordinates and somehow finding a connection but I don't think that works.

I tried breaking out d\vec{S} = \frac{\partial \vec{r}}{\partial u} \cdot \frac{\partial \vec{r}}{\partial v } dudv

using the formula above but not sure on how the dot product works. What confuses me with the integrand with the z and r. The answer is 4πA.
 
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Mulz said:
d\vec{S} = \frac{\partial \vec{r}}{\partial u} \cdot \frac{\partial \vec{r}}{\partial v } dudv
This is not the correct expression for the surface element. The correct expression is
$$
d\vec S = \frac{\partial \vec r}{\partial u} \times \frac{\partial \vec r}{\partial v} du\, dv.
$$
This is equal to ##\vec n \, dS##, where ##\vec n## is a unit normal and ##dS## the area spanned by the tangent vectors on the sphere. What is the unit normal to the unit sphere?

Also, the second term does not contribute to the integral. Do you know of some integral theorem that you can invoke to come to this conclusion?
 
Ask yourself, what is the vector ## d \vec S ##?
 
Orodruin said:
This is not the correct expression for the surface element. The correct expression is
$$
d\vec S = \frac{\partial \vec r}{\partial u} \times \frac{\partial \vec r}{\partial v} du\, dv.
$$
This is equal to ##\vec n \, dS##, where ##\vec n## is a unit normal and ##dS## the area spanned by the tangent vectors on the sphere. What is the unit normal to the unit sphere?

Also, the second term does not contribute to the integral. Do you know of some integral theorem that you can invoke to come to this conclusion?

I might be completely lost but isn't the normal of a surface given by \nabla = \frac{\partial}{\partial x} + \frac{\partial}{\partial y} + \frac{\partial}{\partial z}? It should be ⊥ to the tangentvector.

Or maybe the position vector \vec{r} = x\hat{x} + y\hat{y} + z\hat{z}? I think this one simply desribes the coordinates of a sphere as opposed to a normal.

The don't know if the book covered the relevant integral theroem since I read it 4 times.
 
The ##\nabla## operator in itself is a differential operator, not a vector. Acting on a scalar field, it becomes the gradient, which is normal to the level surfaces of the field.

The integral theorem is the divergence theorem. You can do without as well, but it helps.
 
Orodruin said:
The ##\nabla## operator in itself is a differential operator, not a vector. Acting on a scalar field, it becomes the gradient, which is normal to the level surfaces of the field.

The integral theorem is the divergence theorem. You can do without as well, but it helps.
I don't think I'm supposed to use the divergence theorem since it's not discussed in this chapter.
 
As I already said, it helps, but it is not necessary.
 
Orodruin said:
As I already said, it helps, but it is not necessary.
How should I begin to solve it? I'm not sure how to start. Feels like I'm missing a lot of knowledge even when repeaditely reading the chapter.
 

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