Three charges are situated at the comers of a square ,as shown in Fig. 2.41.

  1. How much work does it take to bring in another charge, +q,from far away and place it in the fourth comer?
  2. How much work does it take to assemble the whole configuration of four charges?

Short Answer

Expert verified

(a)Theworkittaketobringinanothercharge,+qfromfarawayandplaceitinthefourthcomerisw=q24π012-2.(b)Theworkdoesittaketoassemblethewholeconfigurationoffourchargesisw=14π0q2a2-4.

Step by step solution

01

Determine the expression for the potential.

Write the expression for the potential is,

V(r)=q4π0r

Here, qis the charge, r is the distance and Vis the volume.

Consider the figure for the charges.

The figure consist the distribution of charged as shown above.

Consider the distance of the charge at point Aform the charge +qis the diagonal of the square and the value is,

r=a2+a2=2a2=2a

02

Determine the potential at point

(a)

Now write the expression for potential at point A,

VA=14πε0-qa+qa2-qaSolvingforV(A),VA=14πε0a12-2Thus,workdoneinbringingthefourthcharge+qatfrominfinity.Let'sassume,V()=0is,w=qVr-VNowsolvingforVrbysubstituting2aforrinequationVr=q4πε0r.Vr=q4πε0a2SubstitutethefortherintheequationVr=q4πε0r.Vr=q4πε0=0Substitute0forVandVrintheequationw=qvr-v.w=q24πε0a12-2Therefore,therequiredworkisw=q24πε0a12-2.

03

Determine the work required to assemble the whole configuration of the four charges.

(b)

At point ,

Write the expression for amount of work done in bringing the charge,

W=q4πε0-q+-q+1a2+-q+1a2-q

Thus, the work done in assembling the whole configuration is,

w=14πε0q2a-1+-1+12+-q+1a2-1

Solve as further,

w=14πε0q2a2-4Therefore,theworkneedtobedoneisw=14πε0q2a2-4.

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Most popular questions from this chapter

Imagine that new and extraordinarily precise measurements have revealed an error in Coulomb's law. The actual force of interaction between two point charges is found to be

F=14πε0q1q2r2(1+rλ)e(rλ)r^

where λ is a new constant of nature (it has dimensions of length, obviously, and is a huge number—say half the radius of the known universe—so that the correction is small, which is why no one ever noticed the discrepancy before). You are charged with the task of reformulating electrostatics to accommodate the new discovery. Assume the principle of superposition still holds.

a. What is the electric field of a charge distribution ρ (replacing Eq. 2.8)?

b. Does this electric field admit a scalar potential? Explain briefly how you reached your conclusion. (No formal proof necessary—just a persuasive argument.)

c. Find the potential of a point charge q—the analog to Eq. 2.26. (If your answer to (b) was "no," better go back and change it!) Use ∞ as your reference point.

d. For a point charge q at the origin, show that

SE.da+1λ2VVdτ=1ε0q

where S is the surface, V the volume, of any sphere centered at q.

e. Show that this result generalizes:

SE.da+1λ2VVdτ=1ε0Qenc

for any charge distribution. (This is the next best thing to Gauss's Law, in the new "electrostatics.”)

f. Draw the triangle diagram (like Fig. 2.35) for this world, putting in all the appropriate formulas. (Think of Poisson's equation as the formula for ρ in terms of V, and Gauss's law (differential form) as an equation for ρ in terms of E.)

g. Show that some of the charge on a conductor distributes itself (uniformly!) over the volume, with the remainder on the surface. [Hint: E is still zero, inside a conductor.]

Find the electric field a distance zabove the center of a circular loop of radius r(Fig. 2.9) that carries a uniform line charge λ

Find the net force that the southern hemisphere of a uniformly charged solid sphere exerts on the northern hemisphere. Express your answer in terms of the radius R and the total charge Q.

What is the minimum-energy configuration for a system ofNequal

point charges placed on or inside a circle of radius R? Because the charge on

a conductor goes to the surface, you might think theNcharges would arrange

themselves (uniformly) around the circumference. Show (to the contrary) that for

N = 12 it is better to place 11 on the circumference and one at the center. How about for N = 11 (is the energy lower if you put all 11 around the circumference, or if you put 10 on the circumference and one at the center)? [Hint: Do it numerically-you'll need at least 4 significant digits. Express all energies as multiples of q24πε0R]

All of electrostatics follows from 1/r2the character of Coulomb's law, together with the principle of superposition. An analogous theory can therefore be constructed for Newton's law of universal gravitation. What is the gravitational energy of a sphere, of mass M and radius R,assuming the density is uniform? Use your result to estimate the gravitational energy of the sun (look up the relevant numbers). Note that the energy is negative-masses attract,whereas (like) electric charges repel.As the matter "falls in," to create the sun, its energy is converted into other forms (typically thermal), and it is subsequently released in the form of radiation. The sun radiates at a rate of 3.86×1026W; if all this came from gravitational energy, how long would the sun last? [The sun is in fact much older than that, so evidently this is notthe source of its power.]

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