Spherical Coordinates to Rectangular Coordinates

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Homework Help Overview

The discussion revolves around the conversion of forces expressed in spherical coordinates, specifically focusing on a particle moving in a central potential, V(r). Participants are examining how to express the force vector in terms of spherical coordinates and the implications of the gradient operator in this context.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the expression of the force vector using spherical coordinates and question the application of Cartesian coordinates. There are discussions about the gradient operator and its implications in spherical coordinates, with some participants expressing uncertainty about their understanding of gradients.

Discussion Status

The discussion is ongoing, with participants providing insights and hints to each other. Some have suggested that the force should depend solely on the radial component, while others are clarifying the need to consider all components of the force vector in spherical coordinates. There is a mix of understanding and confusion regarding the gradient and its application.

Contextual Notes

Some participants indicate a lack of experience with gradients and spherical coordinates, which may be influencing their interpretations and attempts to solve the problem. There is an emphasis on ensuring that the force vector is expressed correctly in terms of the spherical coordinate system.

Domnu
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A particle of mass [tex]m[/tex] moves in a "central potential," [tex]V(r),[/tex] where [tex]r[/tex] denotes the radial displacement of the particle from a fixed origin.

a) What is the (vector) force on the particle? Use spherical coordinates.

We have

[tex]F = -\nabla V = -\frac{\partial V}{\partial x} \hat{i} - \frac{\partial V}{\partial y} \hat{j} - \frac{\partial V}{\partial z} \hat{k}[/tex]

Now, note that

[tex]\frac{\partial V}{\partial x} = \frac{\partial V}{\partial r} \frac{\partial r} \partial x},[/tex]

since [tex]V is only dependent on [tex]r[/tex] (and not [tex]\theta[/tex] or [tex]\phi[/tex]). Since [tex]x = r \sin \theta \cos \phi[/tex], we have that<br /> <br /> [tex]\frac{\partial r}{\partial x} = \frac{1}{\sin \theta \cos \phi},[/tex]<br /> <br /> so finally,<br /> <br /> [tex]F = -\frac{dV}{dr} \cdot \frac{1}{\sin \theta \cos \phi}[/tex][/tex]
 
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Domnu said:
A particle of mass [tex]m[/tex] moves in a "central potential," [tex]V(r),[/tex] where [tex]r[/tex] denotes the radial displacement of the particle from a fixed origin.

a) What is the (vector) force on the particle? Use spherical coordinates.

[tex]F = -\frac{dV}{dr} \cdot \frac{1}{\sin \theta \cos \phi}[/tex]

Hi Domnu! :smile:

Nooo … the force has to depend only on r, doesn't it?

Try again! (hint: what "is" gradient?) :smile:
 
Domnu said:
Use spherical coordinates.

We have

[tex]F = -\nabla V = -\frac{\partial V}{\partial x} \hat{i} - \frac{\partial V}{\partial y} \hat{j} - \frac{\partial V}{\partial z} \hat{k}[/tex]
You were asked to use spherical coordinates. So why did you use cartesian coordinates?

One reasonable answer is that you have not been taught how to compute the gradient in spherical coordinates. If that is the case, you have only computed one of the three cartesian elements of the force vector. The force will have y and z components as well as an x component.
 
Hmm... I haven't really had a whole lot of experience with gradients, etc. Let's say we have a function F, and we take the gradient of it. Would the resulting gradient just be the vector (after substituting x,y,z points) which lies on the plane which is tangent to F?
 
Hmm... well I see that

[tex]F = - \nabla V = -\frac{\partial V}{\partial r} \hat{r}[/tex]

only... the dv/dtheta and dv/dphi terms are both zero, causing the theta-hat and phi-hat terms to be zero. So, would this just be the answer? It is only in terms of r, since V is only a function of r.
 
Domnu said:
Hmm... well I see that

[tex]F = - \nabla V = -\frac{\partial V}{\partial r} \hat{r}[/tex]

only... the dv/dtheta and dv/dphi terms are both zero, causing the theta-hat and phi-hat terms to be zero. So, would this just be the answer? It is only in terms of r, since V is only a function of r.

That's it! :smile:

Once you know that the gradient is in a particular direction, it's just the directional derivative in that direction. :wink:
 
Yay :) I think I finally get the conversion between spherical/cylindrical coordinates. Awesome =)
 
That is the correct answer. You probably need to show that this is the right answer.
 

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