FIGUREP24.38shows a solid metal sphere at the center of a hollow metal sphere. What is the total charge on (a) the exterior of the inner sphere, (b) the inside surface of the hollow sphere, and (c) the exterior surface of the hollow sphere?

Short Answer

Expert verified

a.Charge on the exterior of the inner sphere is-10.7nC.

b.Charge on the inside surface of the hollow sphere is role="math" localid="1648744482331" +10.7nC.

c.Charge on the exterior surface of the hollow sphere is48.2nC.

Step by step solution

01

Calculation for charge on the outside of the inner sphere (part a)

(a).

The amount of electrical field that travels through a closed surface is stated because the electric flux.

The electric field through a surface is expounded to the charge inside the surface, in line with Gauss's law.

Electric flux is,

Φe=EA=Qinϵo

Qin=ϵoEA

localid="1648745447364" Qin=4πϵoEr2.....1

The gaussian surface's radius is localid="1648747531003" 8cm.

Because the electrical field is contained within the hollow sphere, it's negative.

E=-15000N/C.

Substitute values in equation localid="1648747540022" 1,

We get,

Qin=4πϵoEr2

=4π8.85×10-12C2/N·m2(-15000N/C)(0.08m)2

=-10.7×10-9C=-10.7nC

02

Calculation for charge on the within surface of the hollow sphere (part b)

(b).

The electric charge on the inner sphere's external surface generates a electric charge of the identical magnitude on the hollow sphere's interior surface.

The charge on the hollow sphere's inner surface is the image of the charge inside the small sphere, except it points within the other direction.

So,

Qin=-(-10.7nC)=+10.7nC

03

Calculation for Charge on the outside surface of the hollow sphere (part c)

(c).

The radius of the gaussian surface is r=17cm

The electric field emanating from the hollow spherical is positive.

E=15000N/C

Substitute values in equation localid="1648747517181" 1,

We get,

Qin=4πϵoEr2

=4π8.85×10-12C2/N·m2(15000N/C)(0.17m)2

=48.2×10-9C=48.2nC

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Most popular questions from this chapter

Figure 24.32bshowed a conducting box inside a parallel-plate capacitor. The electric field inside the box is E=0. Suppose the surface charge on the exterior of the box could be frozen. Draw a picture of the electric field inside the box after the box, with its frozen charge, is removed from the capacitor.

Hint: Superposition.

A spherical shell has inner radius Rinand outer radius Rout. The shell contains total charge Q, uniformly distributed. The interior of the shell is empty of charge and matter.

a. Find the electric field strength outside the shell,rRout .

b. Find the electric field strength in the interior of the shell, rRin.

c. Find the electric field strength within the shell, RinrRout.

d. Show that your solutions match at both the inner and outer boundaries

An early model of the atom, proposed by Rutherford after his discovery of the atomic nucleus, had a positive point charge +Ze (the nucleus) at the center of a sphere of radius R with uniformly distributed negative charge -Ze. Z is the atomic number, the number of protons in the nucleus and the number of electrons in the negative sphere. a. Show that the electric field strength inside this atom is

Ein=Ze4πϵ01r2-rR3

b. What is E at the surface of the atom? Is this the expected value? Explain.

c. A uranium atom has Z = 92 and R = 0.10 nm. What is the electric field strength at r = 1 2 R?

All examples of Gauss's law have used highly symmetric surfaces where the flux integral is either zero or EA. Yet we've claimed that the net Φe=Qin/ϵ0is independent of the surface. This is worth checking. FIGURE CP24.57 shows a cube of edge length Lcentered on a long thin wire with linear charge density λ. The flux through one face of the cube is not simply EA because, in this case, the electric field varies in both strength and direction. But you can calculate the flux by actually doing the flux integral.

a. Consider the face parallel to the yz-plane. Define area dAas a strip of width dyand height Lwith the vector pointing in the x-direction. One such strip is located at position localid="1648838849592" y. Use the known electric field of a wire to calculate the electric flux localid="1648838912266" dΦthrough this little area. Your expression should be written in terms of y, which is a variable, and various constants. It should not explicitly contain any angles.

b. Now integrate dΦto find the total flux through this face.

c. Finally, show that the net flux through the cube is Φe=Qin/ϵ0.

The two spheres in FIGURE Q24.8 on the next page surround equal charges. Three students are discussing the situation.

Student 1: The fluxes through spheres A and B are equal because they enclose equal charges.

Student 2: But the electric field on sphere B is weaker than the electric field on sphere A. The flux depends on the electric field strength, so the flux through A is larger than the flux through B.

Student 3: I thought we learned that flux was about surface area. Sphere B is larger than sphere A, so I think the flux through B is larger than the flux through A.

Which of these students, if any, do you agree with? Explain.

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