For the infinite slot (Ex. 3.3), determine the charge density σ(y)on

the strip at x=0, assuming it is a conductor at constant potential V0.

Short Answer

Expert verified

Answer

The equation for the charge density on the strip at x=0is σy=4ε0V0an=1,3,5...sinnπya.

Step by step solution

01

Define functions

Write the expression for the potential V(x,y)in the infinite slot.

V(x,y)=4V0πn=1,3,5...1ne-nπxasin(nπya) …… (1)

Here, V0is the constant potential along the conductor, xis the x-coordinate, yis the y-coordinate, and nis the positive integer.

02

Determine the charge density

Derive the charge density in terms of electric potential.

σ=-e0Vnσy=-e0Vxx=0 …… (2)

Substitute 4V0πn=1,3,5...1ne-nπxasinnπyafor Vx,yin equation (2).

σy=ε0x4V0π1nenπxasinnπyax=0=ε04V0πx1nenπxasinnπyax=0=ε04V0π1n-nxaenπxasinnπyax=0=ε04V0π1nnxa1nenπxasinnπyax=0

σy=4ε0V0an=1,3,5...sinnπya

Hence, the equation for the charge density on the strip at x=0is σy=4ε0V0an=1,3,5...sinnπya.

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Most popular questions from this chapter

(a) Using the law of cosines, show that Eq. 3.17 can be written as follows:

V(r,θ)=14πε0[qr2+a22racosθqR2+(ra/R)22racosθ]

Whererand θare the usual spherical polar coordinates, with the zaxis along the

line through q. In this form, it is obvious thatV=0on the sphere, localid="1657372270600" r=R.

(a) Find the induced surface charge on the sphere, as a function of θ. Integrate this to get the total induced charge . (What should it be?)

(b) Calculate the energy of this configuration.

A stationary electric dipole p=pz^is situated at the origin. A positive

point charge q(mass m) executes circular motion (radius s) at constant speed

in the field of the dipole. Characterize the plane of the orbit. Find the speed, angular momentum and total energy of the charge.

Charge density

σ(ϕ)=asin(5ϕ)

(whereais a constant) is glued over the surface of an infinite cylinder of radiusR

(Fig. 3.25). Find the potential inside and outside the cylinder. [Use your result from Prob. 3.24.]

Prove that the field is uniquely determined when the charge density ρ

is given and either V or the normal derivative a V/n is specified on each boundary surface. Do not assume the boundaries are conductors, or that V is constant over any given surface.

RFind the average potential over a spherical surface of radius Rdue to

a point charge qlocated inside (same as above, in other words, only with z<R).(In this case, of course, Laplace's equation does not hold within the sphere.) Show that, in general,

role="math" localid="1657706668993" Vave=Vcenter+Qenc4πε0R

where Vcenteris the potential at the center due to all the external charges, andQenc is the total enclosed charge.

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