Spherical surface area element

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Homework Help Overview

The discussion revolves around understanding the expression for the area element on a spherical surface, specifically the term Rdθ.2∏Rsinθ. Participants are exploring the geometric interpretation of this expression in the context of surface area and charge density calculations.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants are attempting to break down the expression into its components, questioning the meaning of Rdθ as the width of a strip and 2∏Rsinθ as the length. There are discussions about the arc length and the relationship between the variables involved. Some participants express confusion regarding the setup and the definitions used, particularly concerning the radius and the surface charge density.

Discussion Status

The discussion is ongoing, with participants seeking clarification on the geometric and physical interpretations of the terms involved. Some have provided insights into the area element and its integration, while others are still grappling with the foundational concepts and definitions. There is no explicit consensus yet, as different interpretations and understandings are being explored.

Contextual Notes

There are mentions of potential ambiguities in the definitions of variables, particularly regarding the surface charge density and the angle θ. Participants are also noting the need for clearer statements of the problem being solved to facilitate better understanding.

binbagsss
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See image attached.

(I've had a google but can't find anything).

I am trying to understand the expression : Rdθ.2∏Rsinθ



Here are my thoughts so far:

Rdθ is the width of a strip, θ being the variable changing/to integrate over, giving arise to the elements.

2∏Rsinθ must then be the length. However I don't understand this expression.

I think I understand Rdθ - it is the arc length.

Here are my length thoughts: From the triangle sin θ =(l/2)/R, where l is the length we are after, and l/2, because this triangle only gives half of the length we are after.

Ofc this must be wrong, as I have a ∏ unexplained.


Many thanks to anyone who can help shed some light on this, greatly appreciated !
 

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binbagsss said:
See image attached.

(I've had a google but can't find anything).

I am trying to understand the expression : Rdθ.2∏Rsinθ
Here are my thoughts so far:

Rdθ is the width of a strip, θ being the variable changing/to integrate over, giving arise to the elements.

2∏Rsinθ must then be the length. However I don't understand this expression.

I think I understand Rdθ - it is the arc length.

Here are my length thoughts: From the triangle sin θ =(l/2)/R, where l is the length we are after, and l/2, because this triangle only gives half of the length we are after.

Ofc this must be wrong, as I have a ∏ unexplained.Many thanks to anyone who can help shed some light on this, greatly appreciated !

It would help if you give us a statement of what problem is being solved. Also, in the figure it doesn't appear that R is the radius of the circle. Or maybe it is, just overwritten on the vertical strip.
 
I am given a surface change densiity σ = P.[itex]\hat{n}[/itex] = P cos θ, where P is a constant, and am multiplying this by the area element to find the total charge.
(I am then going to apply Coulomb's law to find the total electric field).

Does this help?

My apologies, R is the radius of the circle
 
It doesn't help me. I don't see what you are doing. I don't see any spherical dS element and I don't understand the problem. Maybe someone else will stop by.
 
anyone?
 
binbagsss said:
See image attached.

(I've had a google but can't find anything).

I am trying to understand the expression : Rdθ.2∏Rsinθ
Here are my thoughts so far:

Rdθ is the width of a strip, θ being the variable changing/to integrate over, giving arise to the elements.

2∏Rsinθ must then be the length. However I don't understand this expression.

I think I understand Rdθ - it is the arc length.

[itex]r\,d\theta[/itex] is the arclength in the direction of increasing [itex]\theta[/itex] (with [itex]\phi[/itex] and [itex]r[/itex] fixed). Arclength in the direction of increasing [itex]\phi[/itex] (with [itex]\theta[/itex] and [itex]r[/itex] fixed) is [itex]r\sin\theta\,d\phi[/itex]. The area of the surface corresponding to [itex][\theta, \theta + \delta\theta]\times[\phi,\phi + \delta\phi][/itex] with [itex]r = R[/itex] constant is then approximately [itex](R\delta\theta)(R \sin (\theta)\delta\phi) = R^2 \sin (\theta)\delta\theta\delta\phi[/itex]. Thus the integral of [itex]\sigma[/itex] over the sphere [itex]r = R[/itex] is
[tex] \int_{r = R} \sigma\,dS = \int_0^{2\pi} \int_0^{\pi} \sigma R^2 \sin \theta\,d\theta\,d\phi[/tex] and if [itex]\sigma[/itex] is independent of [itex]\phi[/itex] this reduces to
[tex] R^2\left(\int_0^{2\pi}\,d\phi\right)\int_0^\pi \sigma\sin \theta\,d\theta = 2\pi R^2 \int_0^\pi \sigma\sin\theta\,d\theta.[/tex]

binbagsss said:
I am given a surface change densiity σ = P.[itex]\hat{n}[/itex] = P cos θ, where P is a constant,

Are you given that [itex]\sigma = P \cos \theta[/itex] for constant [itex]P[/itex], or are you given [itex]\sigma = \mathbf{P} \cdot \hat{\mathbf{n}}[/itex] for constant [itex]\mathbf{P}[/itex]? I can't tell whether [itex]\mathbf{P} \cdot \hat{\mathbf{n}} = P\cos\theta[/itex] is something you were given or the reflex action of calling the angle in the definition of the dot product "[itex]\theta[/itex]". But that angle might not be equal to the coordinate [itex]\theta[/itex], so should be given a different name.

Assuming [itex]\hat{\mathbf{n}}[/itex] is the outward normal to the sphere, you have [itex]\hat{\mathbf{n}} = \hat{\mathbf{r}}[/itex], so [itex]\mathbf{P} \cdot \hat{\mathbf{n}}[/itex] is the radial component of [itex]\mathbf{P}[/itex]. But if [itex]\mathbf{P}[/itex] is constant then its radial component is not constant but depends on both [itex]\theta[/itex] and [itex]\phi[/itex].
 
Last edited:

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