Electric potential of a conical surface

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Homework Help Overview

The problem involves calculating the electric potential difference between two points on a conical surface with a uniform surface charge. The specific points of interest are the vertex of the cone and the center of the top, with the context rooted in electrostatics.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the integration process for calculating potential at different points on the cone and question how the direction of integration affects the reference points used in the calculations.

Discussion Status

Some participants have offered clarifications regarding the integration limits and the reference point for potential, while others express confusion about the implications of these limits on the calculations. The discussion is exploring different interpretations of the integration process without reaching a consensus.

Contextual Notes

There is an ongoing examination of the reference points used in the potential calculations, particularly concerning the definitions and assumptions about the limits of integration in relation to the geometry of the cone.

davon806
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Homework Statement


(From Griffiths problem 2.26) :
A conical surface (an empty ice-cream cone) carries a uniform surface charge σ. The height of the cone is h, and the radius of the top is R. Find the potential difference between points a (the vertex) and b (the center of the top).

Homework Equations

The Attempt at a Solution


Solution to this problem: (EXAMPLE 4 of the page)
http://www.physicspages.com/2011/10/10/electric-potential-from-charges-examples-1/

Whenever we are talking about electric potential,we need to specify the reference point.
i.e.
V(r) \equiv -\int_O^\mathbf{r} \mathbf{E \cdot} d \mathbf{l}\

Where O is some standard reference point s.t. V = 0 at that point.In most circumstance we regard infinity as the reference point.

If you picture an inverted cone in your mind, and follow the solution in the above link, then for V(0),
you integrate from the base of cone to the tip of the cone.
While for V(R) ( the base of the cone), you integrate from the tip of the cone up to the base of the cone).

But this two directions are exactly opposite, so how can we have two different reference point when calculating the potential difference V(R) - V(0) ?
 
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davon806 said:
If you picture an inverted cone in your mind, and follow the solution in the above link, then for V(0),
you integrate from the base of cone to the tip of the cone.
While for V(R) ( the base of the cone), you integrate from the tip of the cone up to the base of the cone).
Not when I read it:
For zv=0 they add all the contributions from the rings from z = 0 to z = R to find the potential V(0).
For zv=R they add all the contributions from the rings from z = 0 to z = R to find the potential V(R).
 
BvU said:
Not when I read it:
For zv=0 they add all the contributions from the rings from z = 0 to z = R to find the potential V(0).
For zv=R they add all the contributions from the rings from z = 0 to z = R to find the potential V(R).

Yes, but since these two points are located at the limit of integration (z = 0 and z = R). For z = 0, the tip is at bottom,and all the contributions are above of the tip;
But for z = R, all the contributions are below of the centre of base . I am a bit confused,does this invert the upper and lower limit of integration? And using the definition of V = V(r) \equiv -\int_O^\mathbf{r} \mathbf{E \cdot} d \mathbf{l}\ , does the tip and centre of base have the same reference point ? I mean, because of "invert the upper and lower limit of integration" , I think the reference points in a and b are different as well. Sorry, I am very confused :nb)
 
davon806 said:
does this invert the upper and lower limit of integration?
No. The integral runs in the same direction in each case, from 0 to h.
davon806 said:
does the tip and centre of base have the same reference point ?
Yes. The reference point in both cases is zero potential at infinity. This is built into equation (16). Consider what happens to the expression for dV there as zv tends to infinity.
 

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