Finding surface charge densities and potential (metal cylinder)

AI Thread Summary
The discussion focuses on calculating the surface charge densities and electric potential for a solid metal cylinder surrounded by a coaxial shell. The surface charge densities at the cylinder and shell surfaces are correctly identified as σ_R = Q/(2πRL), σ_a = Q/(2πaL), and σ_b = Q/(2πbL), although the sign for σ_a is noted to be incorrect. The potential calculation involves integrating the electric field, but there are errors in the integration boundaries and variable usage that need correction. It is emphasized that the potential does not change within a conductor, leading to the removal of certain integrals in the potential calculation.
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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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