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Four particles (one of charge q,one of charge 3q,and two of charge -2q)are placed as shown in Fig. 3.31, each a distance from the origin. Find a

simple approximate formula for the potential, valid at points far from the origin.

(Express your answer in spherical coordinates.)

Short Answer

Expert verified

The potential at the origin for the point charge is V=12πε02qacosθr2.

Step by step solution

01

Define function

The dipole moment is the product of charge and distance of separation charge from the origin.

Write the expression for dipole moment.

p=∑i=1nqiri ……. (1)

Here, is the charge of ithparticle,ri is the distance of separation charge form the origin.

02

Given data

The position of particle is shown in figure.

It consist of charges as q ,3q-2q,-2q. The separation between the charges denoted by a.

03

Determine potential

Write the expression for the total dipole moment due to four charges.

P=3qaz^-qaz^+-2qay^+-2qa-y^=2qaz^+2qay^+2qay^.........(2)=2qaz^

Write the expression for the position of the point in spherical coordinates.

x=rsinθcosθq=rsinθsinθz=rcosθ

The scalar product of dipole P and position vector r^is,

P.r^ ......(3)

Substitute 2qaz^ for P in equation (3).

P.r^=2qaz^.r^=2qaz^.r^=2qar^cosθ.r^

Substitute r^.r^=1

Thus,

P.r^=2qacosθ.......(4)

Write the equation for potential at distance rdue to point charge q.

V=14πε0P.r^r2......(5)

Substitute 2qacosθ for P .r^, in equation (5)

V=14πε02qacosθr2

Thus, the potential at the origin for the point charge is V=14πε2qacosθr2.

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Most popular questions from this chapter

Two long, straight copper pipes, each of radius R, are held a distance

2d apart. One is at potential V0, the other at -V0(Fig. 3.16). Find the potential

everywhere. [Hint: Exploit the result of Prob. 2.52.]

Three point charges are located as shown in Fig. 3.38, each a distance

afrom the origin. Find the approximate electric field at points far from the origin.

Express your answer in spherical coordinates, and include the two lowest orders in the multi-pole expansion.

(a) Show that the average electric field over a spherical surface, due to charges outside the sphere, is the same as the field at the center.

(b) What is the average due to charges inside the sphere?

In Prob. 2.25, you found the potential on the axis of a uniformly charged disk:

V(r,0)=σ2ε0(r2+R2-r)

(a) Use this, together with the fact that PI(1)=1, to evaluate the first three terms

in the expansion (Eq. 3.72) for the potential of the disk at points off the axis, assuming r>R.

(b) Find the potential for r<Rby the same method, using Eq. 3.66. [Note: You

must break the interior region up into two hemispheres, above and below the

disk. Do not assume the coefficientsAIare the same in both hemispheres.]

Two semi-infinite grounded conducting planes meet at right angles. In the region between them, there is a point chargeq, situated as shown in Fig. 3.15. Set up the image configuration, and calculate the potential in this region. What charges do you need, and where should they be located? What is the force onq? How much Work did it take to bringqin from infinity? Suppose the planes met at some angle other than; would you still be able to solve the problem by the method of images? If not, for what particular anglesdoesthe method work?

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