The charged balloon in FIGURE Q24.7 expands as it is blown up, increasing in size from the initial to final diameters shown. Do the electric field strengths at points 1, 2, and 3 increase, decrease, or stay the same? Explain your reasoning for each.

Short Answer

Expert verified

Electric field at point 1 is the same

Electric field at point 2 decreases

Electric field at point 3 is the same

Step by step solution

01

Given information and theory used

Given Figure :

Theory used :

At all sites in electrostatic equilibrium inside a conductor, the Electric Field is zero. However, all surplus charges on the conductor accumulate on the outside surface, and as further charges are added, they spread out on the outer surface until they reach the electrostatic equilibrium points. The electric field at the surface of a charged conductor in the form

Esurface=ηε0, where η is the surface charge density.

02

Determining if the electric field strengths at points 1, 2, and 3 increase, decrease, or stay the same 

The surface charge density is not constant and is a physical parameter that relies on the conductor's geometry. Calculating the surface charge density using the electric field outside the conductor :

Because the electric field at point 1 is the same at both the beginning and the end of the balloon, the electric field at point 1 is the same.

The electric field at point 2 is weaker. Because point 2 is outside the balloon at first, an electric field exists due to charges on the surface; however, as the balloon expands, point 2 becomes inside the balloon, and the electric field vanishes. The electric field shrinks in this situation.

The electric field at point 3 is same. Point 3 lies outside the balloon both before and after the expansion, therefore the electric field is the same.

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Most popular questions from this chapter

A spark occurs at the tip of a metal needle if the electric field strength exceeds 3.0×106N/C, the field strength at which air breaks down. What is the minimum surface charge density for producing a spark?

Find the electric field inside and outside a hollow plastic ball of radius R that has chargeQ uniformly distributed on its outer surface.

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.

What is the net electric flux through the two cylinders shown inFIGURE EX24.16? Give your answer in terms of RandE

FIGURE P24.47shows an infinitely wide conductor parallel to and distance dfrom an infinitely wide plane of charge with surface charge density η. What are the electric field E1to E4in regions 1to 4?

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