Finding surface charge densities and potential (metal cylinder)

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Homework Help Overview

The discussion revolves around a solid metal cylinder surrounded by a coaxial metal shell, focusing on finding surface charge densities and electric potential. The problem involves concepts from electrostatics, particularly related to charge distribution and electric fields in conductors.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the calculation of surface charge densities at various radii and the potential at the center of the configuration. There are attempts to clarify the relationship between potential and electric field, as well as the correct integration variables for the equations presented.

Discussion Status

Some participants have provided guidance on correcting the integration approach and clarifying the relationship between potential and electric field. There are ongoing questions regarding the assumptions made about the potential inside the conductor and the correct signs for surface charge densities.

Contextual Notes

Participants note potential misunderstandings regarding the integration variables and the implications of charge distribution within the conductor. There is also mention of the need to consider the behavior of potential in conductive materials.

ghostfolk
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Homework Statement



A solid metal cylinder of radius ##R## and length ##L##, carrying a charge ##Q##, is surrounded by a thick coaxial metal shell of inner radius ##a## and outer radius ##b##. The shell carries no net charge.
a) Find the surface charge desnities ##\sigma## at ##R##, at ##a##, and at ##b##.
b) Find the potential at the center using ##r=b## as the reference point.

Homework Equations


##\sigma=q/A##, ##A_{cyl}=2\pi rh##, ##V(r)=-\int_{r_1}^{r_2} \frac{\sigma}{r} da##

The Attempt at a Solution


a) ##\sigma_R=\frac{Q}{2\pi RL}## ##\sigma_a=\frac{Q}{2\pi aL}## ##\sigma_b=\frac{Q}{2\pi bL}##

b) ##V=-\int_b^a \frac{\sigma_b}{r}da-\int_a^R \frac{\sigma_a}{r}da-\int_R^0 \frac{\sigma_R}{r}da##
##da=2\pi RLdr##
 
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ghostfolk said:

Homework Statement



A solid metal cylinder of radius ##R## and length ##L##, carrying a charge ##Q##, is surrounded by a thick coaxial metal shell of inner radius ##a## and outer radius ##b##. The shell carries no net charge.
a) Find the surface charge desnities ##\sigma## at ##R##, at ##a##, and at ##b##.
b) Find the potential at the center using ##r=b## as the reference point.

Homework Equations


##\sigma=q/A##, ##A_{cyl}=2\pi rh##, ##V(r)=-\int_{r_1}^{r_2} \frac{\sigma}{r} da##

The last equation is not correct. How are the potential function V(r) and the electric field E(r) related ?

You should integrate with respect to the variable the integrand depends on. If you integrate a function depending on r , write it as ##\int f(r)dr ## instead of ##\int f(r) da##. If you use fixed boundaries in the integral for r the result can not depend on r .
Moreover, a means the inner radius of the shell, do not use it as an integrating variable.

ghostfolk said:

The Attempt at a Solution


a) ##\sigma_R=\frac{Q}{2\pi RL}## ##\sigma_a=\frac{Q}{2\pi aL}## ##\sigma_b=\frac{Q}{2\pi bL}##

b) ##V=-\int_b^a \frac{\sigma_b}{r}da-\int_a^R \frac{\sigma_a}{r}da-\int_R^0 \frac{\sigma_R}{r}da##
##da=2\pi RLdr##
The surface charge densities are all right, but the sign of the surface charge density at a is not correct.
I do not understand what you tried to say with line b). Does the potential change inside a conductor?

ehild
 
ehild said:
The last equation is not correct. How are the potential function V(r) and the electric field E(r) related ?
You should integrate with respect to the variable the integrand depends on. If you integrate a function depending on r , write it as ##\int f(r)dr ## instead of ##\int f(r) da##. If you use fixed boundaries in the integral for r the result can not depend on r .
Moreover, a means the inner radius of the shell, do not use it as an integrating variable.
I should've made it made it more clear that ##da## is the normal vector of the surface area of the cylinder so that ##d\vec{a}=2 \pi RLdr\hat{r}##

ehild said:
The surface charge densities are all right, but the sign of the surface charge density at a is not correct.
I do not understand what you tried to say with line b). Does the potential change inside a conductor?
Yeah I forgot the minus sign. Also the potential does not change in the conductor so I should remove the integral that goes from 0 to ##R##
 
Last edited:
ghostfolk said:
I should've made it made it more clear that ##da## is the normal vector of the surface area of the cylinder so that ##d\vec{a}=2 \pi RLdr\hat{r}##
Note that the potential is line integral of the negative electric field instead of a surface integral.

ghostfolk said:
Yeah I forgot the minus sign. Also the potential does not change in the conductor so I should remove the integral that goes from 0 to ##R##

That is right, but it is zero also somewhere else.

ehild
 

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