/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Q29P Four particles (one of charge q,... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

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.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

A circular ring in thexy plane (radius R , centered at the origin) carries a uniform line charge λ. Find the first three terms(n=0,1,2) in the multi pole expansion for V(r,θ).

A uniform line charge λis placed on an infinite straight wire, a distanced above a grounded conducting plane. (Let's say the wire runs parallel to the x-axis and directly above it, and the conducting plane is the xyplane.)

  1. Find the potential in the region above the plane. [Hint: Refer to Prob. 2.52.]
  2. Find the charge density σ induced on the conducting plane.

Two infinite parallel grounded conducting planes are held a distanceapart. A point chargeqis placed in the region between them, a distance xfromone plate. Find the force on q20Check that your answer is correct for the special

cases a→∞and x=a2.

You can use the superposition principle to combine solutions obtained by separation of variables. For example, in Prob. 3.16 you found the potential inside a cubical box, if five faces are grounded and the sixth is at a constant potential V0; by a six-fold superposition of the result, you could obtain the potential inside a cube with the faces maintained at specified constant voltages . V1,V2,......V6In this way, using Ex. 3.4 and Prob. 3.15, find the potential inside a rectangular pipe with two facing sides (x=±b)at potential V0, a third (y=a)at V1. and the last at(y=a) grounded.

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)=1to 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 coefficients A1are the same in both hemispheres.]

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.