Gradient in spherical coordinates problem

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The discussion centers on understanding the gradient of a scalar field in spherical coordinates, specifically the terms involving \(\frac{1}{r}\) and \(\frac{1}{r \sin(\theta)}\). The user initially presents a gradient expression that lacks these terms, leading to confusion. It is clarified that these factors arise from the conversion of Cartesian coordinates to spherical coordinates using the chain rule. The gradient operator in spherical coordinates incorporates these terms to accurately represent changes in the scalar field. The conversation emphasizes the importance of properly applying the chain rule for accurate calculations in spherical coordinates.
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Hello,

I need help. The topic is a gradient in spherical coordinates. In cartesian it is clear but in spherical coordinates I have two terms which I don't understand from where they come.

Okay, I have a scalar field in spherical coordinates:

\Phi = \Phi(r, \theta, \phi)

I thought that this is the gradient but it is wrong and I don't know why :(

grad \Phi = \frac{\partial \phi}{\partial r} \vec{e}_{r} + \frac{\partial \phi}{\partial \theta} \vec{e}_{\theta} + \frac{\partial \phi}{\partial \phi} \vec{e}_{\phi}

My mathbook tells me that this is the gradient in spherical coordinates but I don't understand the terms \frac{1}{r} and \frac{1}{r \sin(\theta)}

grad \Phi = \frac{\partial \phi}{\partial r} \vec{e}_{r} + \frac{1}{r} ~ \frac{\partial \phi}{\partial \theta} \vec{e}_{\theta} + \frac{1}{r \sin(\theta)} ~ \frac{\partial \phi}{\partial \phi} \vec{e}_{\phi}


I would be thank you for helping :)

greetings

P.S.
Sorry for my bad english. I will practice and learn grammar for better english in the future ;)
 
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In Cartesian coordinates
\grad \phi= \frac{\partial \phi}{\partial x}\vec{i}+ \frac{\partial \phi}{\partial y}\vec{j}+ \frac{\partial \phi}{\partial z}\vec{k}
Now you have to use the chain rule to convert those derivatives to spherical coordinates:
\frac{\partial\Phi}{\partial x}= \frac{\partial \Phi}{\partial \rho}\frac{\partial \rho}{\partial x}+ \frac{\partial \Phi}{\partial \theta}\frac{\partial \theta}{\partial x}+ \frac{\partial \Phi}{\partial \phi}\frac{\partial \phi}{\partial x}
It's tedious but doable.
 
HallsofIvy said:
Now you have to use the chain rule to convert those derivatives to spherical coordinates:

This is what I don't saw. Thank you :)
 
you can define the gradient operator such that :

d \Phi = \left< grad \Phi , d\vec{r}\right >

knowing that in spherical coordinates :

d\vec{r}\right = \vec{e}_{r} dr + \vec{e}_{\theta} \cdot r d\theta + \vec{e}_{\phi} \cdot r \cdot sin(\theta) d\phi

then you should find what you want.
 

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