The electric field is horizontal and has the values indicated on the surface of cylinder as shown in Figure 21.65. What can you deduce from this pattern of electric field? Include a numerical result.

Short Answer

Expert verified

We can deduce from the above electric field distribution that cylinder contains the charge -5.31×10-9C between surfaces of cylinder.

Step by step solution

01

Identification of given data

The length of cylinder isl=15cm

The radius of cylinder is r=5cm.

The magnitude of incoming electric field on the left side of cylinder is E1=1600N/C.

The magnitude of incoming electric field on the left side of cylinder is E2=1000N/C.

02

Conceptual Explanation

The Gauss law is applied for the cylinder to find the net charge inside the cylinder for incoming and outgoing electric field of cylinder. For this net flux for cylinder is equated to the charge inside surface divided by permittivity of free space.

03

Determination of charge enclosed inside the cylinder

The surface area of the cylinder is given as:

A=2πrl

Substitute all the values in the above equation.

A=2π5cm1m100cm15cm1m100cmA=0.0471m2

Apply the Gauss’s law to find the amount of charge inside cylinder:

E2-E1A=qε0

Here, ε0 is the permittivity of box and its value is8.854×10-12C2/N·m2 .

Substitute all the values in the above equation.

1000N/C-1600N/C=q8.854×10-12C2/N·m2q=-5.31×10-9C

Therefore, the amount of charge inside the cylinder is -5.31×10-9C.

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Most popular questions from this chapter

The electric field has been measured to be horizontal and to the right everywhere on the closed box as shown in Figure 21.66. All over the left side of box E1=100V/m and all over the right (slanting) side of box E2=300V/m.On the top the average field is E3=150V/m , on the front and back the average field is E4=175V/mand on the bottom the average field is E5=220V/m.How much charge is inside the box? Explain briefly.

You may have seen a coaxial cable connected to a television set. As shown in Figure 21.69, a coaxial cable consists of a central copper wire of radiusr1 surrounded by a hollow copper tube (typically made of braided copper wire) of inner radiusr2 and outer radius r3. Normally the space between the central wire and the outer tube is filled with an insulator, but in this problem assume for simplicity that this space is filled with air. Assume that no current runs in the cable.

Suppose that a coaxial cable is straight and has a very long length L, and that the central wire carries a charge +Q uniformly distributed along the wire (so that the charge per unit length is +Q/L everywhere along the wire). Also suppose that the outer tube carries a charge -Q uniformly distributed along its length L. The cylindrical symmetry of the situation indicates that the electric field must point radically outward or radically inward. The electric field cannot have any component parallel to the cable. In this problem, draw mathematical Gaussian cylinders of length d (with d much less than the cable length L) and appropriate radius r, centered on the central wire.

(a). Use a mathematical Gaussian cylinder located inside the central wire(r<r1) and another Gaussian cylinder with a radius in the interior of the outer tube(r2<r<r3) to determine the exact amount and location of the charge on the inner and outer conductors. (Hint: What do you know about the electric field in the interior of the two conductors? What do you know about the flux on the ends of your Gaussian cylinders?)

In chapter 15 we calculated the electric field at a location on the axis of a uniformly charged ring. Without doing all those calculations explain why we can’t use Gauss law to determine the electric field at that location.

In Figure 21.15 the magnitude of the electric field is 1000V/m, and the field is at an angle of 30oto the outward-going normal. What is the flux on the small rectangle whose dimensions are 1mmby2mm ?

Figure 21.70 shows a close-up of the central region of a capacitor made of two large metal plates of area , very close together and charged equally and oppositely. There are +Q and -Q on the inner surfaces of the plates and small amounts of charge +q and -q on the outer surfaces.

(a). Knowing Q, determine E: Consider a Gaussian surface in the shape of a shoe box, with one end of area Abox in the interior of the left plate and the other end in the air gap (surface 1 in the diagram). Using only the fact that the electric field is expected to be horizontal everywhere in this region, use Gauss’s law to determine the magnitude of the field in the air gap. Check that your result agrees with our earlier calculations in the Chapter 15. (Be sure to consider the flux on all faces of your Gaussian box.)

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