Finding da_x in Spherical Coordinates

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SUMMARY

This discussion focuses on converting differential area elements in spherical coordinates, specifically finding da_x in terms of spherical coordinates. The user provides the expression da=R^{2}sin(g)dgdh \hat{r} and seeks to express da_x=dydz \hat{i} using spherical coordinates. Key calculations involve the parameterization of the spherical surface and the differentiation of the position vector, resulting in the differential surface area being sin(φ)dφdθ. The fundamental vector product, represented as the cross product of the derivative vectors, is crucial for determining the differential area.

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I want to integrate something in spherical coordinates
I have da=R^{2}sin(g)dgdh \hat{r} with g and h angles
and \hat{r}=sin(g)cos(h) \hat{i}+sin(g)sin(h) \hat{j}+cos(g) \hat{k}

But what is now da_{x}=dydz \hat{i} in spherical coordinates?
So I have the expression in ordinary coordinates and need to find it in spherical coordinates


thanks
 
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On a spherical surface of radius 1, \vec{r}= sin(\phi)cos(\theta)\vec{i}+ sin\phi)sin(\theta)\vec{j}+ cos(\phi)\vec{k} as you say.

Differentiating with respect to each variable,
\vec{r}_\theta= -sin(\phi)cos(\theta)\vec{i}+ sin(\phi)cos(\theta)\vex{j}
\vec{r}_\phi= cos(\phi)cos(\theta)\vec{i}+ cos(\phi)sin(\theta)\vec{j}- sin(\phi)\vec{k}

The "fundamental vector product" of a surface is the cross product of those two derivative vectors:
\left|\begin{array}\vec{i} & \vec{j} & \vec{k} \\ -sin(\phi)sin(\theta) & sin(\phi)cos(\theta) & 0 \\ cos(\phi)cos(\theta) & cos(\phi)sin(\theta) & -sin(\phi)\end{array}\right|= -sin^2(\phi)cos(\theta)\vec{i}- sin^2(\phi)sin(\theta)\vec{j}- sin(\phi)cos(\phi)\vec{k}
has length sin(\phi) so the differential of surface area is sin(\phi)d\phi d\theta.

(In general if a surface is given by \vec{r}(u, v) with parameters u and v, then the differential of surface area is \left|\vec{r}_u\times\vec{r}_v|dudv. Thats's worth knowing! In fact, the "vector differential" \vec{r}_u\times\vec{r}_v du dv is a vector having the differential of surface area as length, normal to the surface and can be used to integrate vector fields over the surface.)
 
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