Maximum charge on a spherical capacitor

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Homework Help Overview

The discussion revolves around determining the maximum charge on a spherical capacitor, focusing on the relationship between electric field, potential, and charge in the context of capacitors with a dielectric material.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the use of electric potential versus electric field in determining maximum charge, questioning the relevance of potential in this context. There is a focus on where the electric field is maximized and how that relates to the charge.

Discussion Status

Some participants have offered guidance on the relationship between the electric field and maximum charge, while others are questioning the assumptions made regarding the use of potential. Multiple interpretations of the problem are being explored, particularly concerning the conditions under which the electric field is maximized.

Contextual Notes

There appears to be a lack of consensus on the approach to take regarding the use of potential versus electric field, with some participants emphasizing the importance of the electric field's maximum value in the analysis.

lorenz0
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Homework Statement
A spherical capacitor has internal radius ##R_1## and external radius ##R_2##.
Between the spheres there is a dielectric with constant ##\varepsilon_r##.
If the maximum electric field that can be applied without electrical discharges occurring is ##E_{max}##, find the corresponding maximum charge that can be put on the plates.
Relevant Equations
##\Delta V=\int \vec{E}\cdot d\vec{l}##
The electric field is the one generated by the charge ##+Q## on the inner sphere of the capacitor, which generates a radial electric field ##\vec{E}=\frac{1}{4\pi\varepsilon_0}\frac{Q}{r^2}\hat{r}## which, due to the presence of the dielectric, become ##\vec{E}_d=\frac{1}{4\pi\varepsilon_0\varepsilon_r}\frac{Q}{r^2}\hat{r}## so ##\Delta V=\int \vec{E}_d\cdot d\vec{l}=\int_{R_1}^{R_2}\frac{1}{4\pi\varepsilon_0\varepsilon_r}\frac{Q}{r^2}\hat{r}\cdot d\vec{l}=\frac{Q}{4\pi\varepsilon_0\varepsilon_r}\frac{R_2-R_1}{R_1R_2}.##

So, ##E=\frac{\Delta V}{R_2-R_1}=\frac{Q}{4\pi\varepsilon_0\varepsilon_r}\frac{1}{R_1R_2}\leq E_{max}\Rightarrow \frac{Q_{max}}{4\pi\varepsilon_0\varepsilon_r}\frac{1}{R_1R_2}= E_{max}\Leftrightarrow Q_{max}=E_{max}4\pi\varepsilon_0\varepsilon_rR_1R_2##.

Does this make sense? Thanks
 
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Why are you using the potential at all? The limit is given in terms of the E field.
Where is it biggest?
 
hutchphd said:
Why are you using the potential at all? The limit is given in terms of the E field.
Where is it biggest?
##E## is biggest on the surface of the inner sphere so ##E_{max}=E(R_1)=\frac{Q_{max}}{4\pi\varepsilon_0\varepsilon_r R_1^2}\Leftrightarrow Q_{max}=4\pi\varepsilon_0\varepsilon_r R_1^2 E_{max}##. Is this correct?
 
Yes.
 
t
hutchphd said:
Yes.
Thank you.
 
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