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(a) In Figure 16.14, what is the direction of the electric field? IsV=Vf-Vipositive or negative? (b) In figure 16.15, what is the direction of the electric field? IsV=Vf-Vipositive or negative?

Short Answer

Expert verified

(a) The value of V=Vf-Viis positive and the direction of the electric field is from ‘positive to negative’

(b) The value of electric field and V=Vf-Viis zero.

Step by step solution

01

Electric Field Direction

The direction of the electric field for a moving charged particle relies upon the change in the value of the potential difference.

If the electric potential increases from one point to another then the direction of the electric field would be opposite to that of electric potential.

02

(a) The direction of the electric field

In the figure (a), the termirepresents the initial position and frepresents the final position of the particle.

From the given Figure (a), the electric charge moves between two charged plates from the negative region to the positive region.

So, the value of the potential difference between two positions of the particle is given by,

V=Vf-ViV>0positive

Hence, the value ofV=Vf-Viis positive.

The value of the potential difference increases from initial to final position, so the direction of the electric field would be opposite to the potential difference.

Hence, the direction of the electric field is from ‘positive to negative’.

03

(b) The direction of the electric field

From the given Figure (b), the electric charge moves from the negative to the positive inside a closed region.

Inside a closed conductor, the value of the electric field as well as the value of the potential difference is zero.

So, the value of the potential difference between two positions of the particle is given by,

V=Vf-ViV=0

Hence, the value of electric field and V=Vf-Viis zero.

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Most popular questions from this chapter

The long rod shown in Figure 16.76 has length L and carries a uniform charge −Q. Calculate the potential difference VA-VC. All of the distances are small compared to L. Explain your work carefully

A rod uniformly charged with charge -q is bent into a semicircular arc of radius b, as shown in Figure 16.97. What is the potential relative to infinity at location A, at the center of the arc?

Locations A, B and C are in a region of uniform electric field, as shown in Figure 16.66. Location A is at (-0.3,0,0)m. Location B is at (0.4,0,0)m. In the region the electric field has the value (850,400,0)N/C . For a path starting at A and ending at B calculate:

(a) the displacement vector I-.

(b) the change in electric potential,

(c) the potential energy change for the system when a proton moves from A to B ,

(d) the potential energy change for the system when an electron moves from A to B.

2 Three charged metal disks are arranged as shown in Figure 16.75 (cutaway view). The disks are held apart by insulating supports not shown in the diagram. Each disk has an area of 2.5 m2 (this is the area of one flat surface of the disk). The charge Q1=5×10-8Cand the charge Q2=4×10-7C.

(a) What is the electric field (magnitude and direction) in the region between disks 1 and 2? (b) Which of the following statements are true? Choose all that apply. (1) Along a path from A to B, EΔI(2) VB-VA=0.(3) localid="1657088862802" VB-VA=-Q/2.5ε0+(0.003)V. . (c) To calculateVC-VB , where should the path start and where should it end? (d) Shouldlocalid="1657089209063" VC-VB be positive or negative? Why? (1) Positive, because localid="1657089087291" ΔIis opposite to the direction of . (2) Negative, becauseΔI is in the same direction asE . (3) Zero, becauseΔIE. (e) What is the potential differenceVC-VB ? (f) What is the potential differenceVD-VC ? (g) What is the potential differenceVF-VD ? (h) What is the potential differenceVG-VF ? (i) What is the potential differenceVG-VA? (j) The charged disks have tiny holes that allow a particle to pass through them. An electron that is traveling at a fast speed approaches the plates from the left side. It travels along a path from A to G. Since no external work is done on system of plates + electron, ΔK+ΔU=Wext=0. Consider the following states: initial, electron at location A; final, electron at location G. (1) What is the change in potential energy of the system? (2) What is the change in kinetic energy of the electron?

What is the maximum possible potential (relative to infinity) of the metal sphere of 10-cm radius? What is the maximum possible potential (relative to infinity) of the metal sphere of only 1-mm radius? These results hint at the reason why a highly charged piece of metal (with uniform potential throughout) tends to spark at places where the radius of curvature is small or at places where there are sharp points. Remember that breakdown electric strength for air is roughly\[{\bf{3 \times 1}}{{\bf{0}}^{\bf{6}}}\;\frac{{\bf{V}}}{{\bf{m}}}\].

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