Figure 14.69 shows a neutral, solid piece of metal placed near two points charges. Copy this diagram.

(a) On your diagram, show the polarization of the piece of metal.

(b) Then, at location A inside the solid piece of metal, carefully draw and label three vectors: (1) E1, the electric field due to -q1; (2) E2, the electric field due to +q2; (3) E3, the electric field due to all of the charges on the metal.

(c) Explain briefly why you drew the vectors the way you did.

Short Answer

Expert verified
  1. In the diagram of the charges present, polarize the metal piece. The positive charge attracts the metal's free electrons, leaving an electron deficiency or, to put it another way, a positive charge attracting the negative charge.
  2. The vector fields E1were drawn, due to the charge -q1, the vector field E2due to the charge +q2and the resulting vector field E3.
  3. The positive charges produce a force and hence an electric field E2in the opposite direction of the charge-point X line. At point A, the negative charge causes an attractive force towards it, and its electric field E1follows the force. The sum of these two vectors produces the final fieldE3.

Step by step solution

01

Identification of given data

The given data can be listed below,

  1. The electric field E1due to charge-q1 .
  2. The electric field E2due to charge +q2.
02

Concept/Significance of polarization

The term polarization, also known as electric polarization, is the alignment of the dipole moments of permanent or induced dipoles in the direction of an applied electric field.

03

(a) Determination of the polarization of the piece of metal in a diagram. 

The polarization of charges is shown below in the diagram.

Thus, in the diagram of the charges present, polarize the metal piece. The positive charge attracts the metal's free electrons, leaving an electron deficiency or, to put it another way, a positive charge attracting the negative charge.

04

(b) Determination of the electric field due to all of the charges on the metal 

The diagram for electric fields is given below,

Thus, the vector fields E1were drawn, due to the -q1charge, the vector field E2due to the charge and the resulting vector field E3.

05

(c) Explanation of briefly why you drew the vectors the way you did

Positive charge generates a force and, as a result, an electric field E2in the opposite direction of the charge-point X line. The negative charge at point A attracts it with its electric field E1, which is parallel to the force. The resulting field E1is obtained by summing these two vectors.

Thus, the positive charges produce a force and hence an electric field E2in the opposite direction of the charge-point X line. At point A, the negative charge causes an attractive force towards it, and its electric field E1follows the force. The sum of these two vectors produces the final fieldE3.

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Most popular questions from this chapter

A very thin spherical plastic shell of radius15 cm carries a uniformly distributed negative charge of 8 nC(8×109 C)on its outer surface (so it makes an electric field as though all the charge were concentrated at the center of the sphere). An uncharged solid metal block is placed nearby. The block is10cm thick, and it is10cm away from the surface of the sphere. See Figure 14.97. (a) Sketch the approximate charge distribution of the neutral solid metal block.

(b) Draw the electric field vector at the center of the metal block that is due solely to the charge distribution you sketched (that is, excluding the contributions of the sphere).

(c) Calculate the magnitude of the electric field vector you drew. Explain briefly. If you must make any approximations, state what they are.

Try rubbing a plastic pen through your hair, and you’ll find that you can pick up a tiny scrap of paper when the pen is about one centimeter above the paper. From this simple experiment you can estimate how much an atom in the paper is polarized by the pen! You will need to make several assumptions and approximations. Hints may be found at the end of the chapter. (a) Suppose that the center of the outer electron cloud (q=-4e) of a carbon atom shifts a distance s when the atom is polarized by the pen. Calculate s algebraically in terms of the charge Q on the pen. (b) Assume that the pen carries about as much charge Q as we typically find on a piece of charged invisible tape. Evaluate s numerically. How does this compare with the size of an atom or a nucleus? (c) Calculate the polarizability αof a carbon atom. Compare your answer to the measured value of 1.96×10-40C.m/(N/C)(T. M. Miller and B. Bederson, “Atomic and molecular polarizabilities: a review of recent advances,” Advances in Atomic and Molecular Physics, 13, 1–55, 1977).(d) Carefully list all assumptions and approximations.

A neutral copper block is polarized as shown in Figure 14.90, due to an electric field made by external charges (not shown). Which arrow (a–j) in Figure 14.90 best indicates the direction of the net electric field at location B, which is inside the copper block ?

You have two identical neutral metal spheres labeled A and B, mounted on insulating posts, and you have a plastic pen that charges negatively when you rub it on your hair (Figure 14.77).


(a) (+ and −) Explain in detail, including diagrams, what operations you would carry out to give sphere A some positive charge and sphere B an equal amount of negative charge. (b) (+ and +) Explain in detail, including diagrams, what operations you would carry out on the neutral spheres to give sphere A some positive charge and sphere B an equal amount of positive charge (the spheres are initially uncharged).

Which of the following are true? Select all that apply. (1) In equilibrium, there is no net flow of mobile charged particles inside a conductor. (2) The electric field from an external charge cannot penetrate to the center of a block of iron. (3) The net electric field inside a block of aluminum is zero under all circumstances. (4) If the net electric field at a particular location inside a piece of metal is not zero, the metal is not in equilibrium. (5) The net electric field at any location inside a block of copper is zero if the copper block is in equilibrium.

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