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A particle with charge\( + {q_1}\)and a particle with charge\( - {q_2}\)are located as shown in figure 16.91. What is the potential (relative to infinity) at location A.

Short Answer

Expert verified

The electric potential at location A due to both charge is \(\frac{1}{{4\pi {\varepsilon _0}}}\left( {\frac{{{q_1}}}{{{r_{1A}}}} - \frac{{{q_2}}}{{{r_{2A}}}}} \right)\).

Step by step solution

01

Identification of given data

The positive charge on the particle is\({q_1}\).

The distance of location A from positive charge is\({r_{1A}}\).

The positive charge on the particle is\( - {q_2}\)

The distance of location A from negative charge is \({r_{2A}}\).

02

Conceptual Explanation

The electric potential is the effect of charged particle at some distance from the charged particle.It is a scalar quantity so the net potential due to different charges at a location is calculated by the algebraic sum of potential of each charge.

03

Determination of electric potential at location A

The electric potential at location A due to positive charge is given as:

\({V_1} = \frac{{{q_1}}}{{4\pi {\varepsilon _0}{r_{1A}}}}\)

The electric potential at location A due to negative charge is given as:

\({V_2} = \frac{{ - {q_2}}}{{4\pi {\varepsilon _0}{r_{2A}}}}\)

The electric potential at location A due to both charges is given as:

\(\begin{array}{c}V = {V_1} + {V_2}\\V = \frac{{{q_1}}}{{4\pi {\varepsilon _0}{r_{1A}}}} + \left( {\frac{{ - {q_2}}}{{4\pi {\varepsilon _0}{r_{2A}}}}} \right)\\V = \frac{1}{{4\pi {\varepsilon _0}}}\left( {\frac{{{q_1}}}{{{r_{1A}}}} - \frac{{{q_2}}}{{{r_{2A}}}}} \right)\end{array}\)

Therefore, the electric potential at location A due to both charge is \(\frac{1}{{4\pi {\varepsilon _0}}}\left( {\frac{{{q_1}}}{{{r_{1A}}}} - \frac{{{q_2}}}{{{r_{2A}}}}} \right)\).

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Most popular questions from this chapter

Locations A and B are in a region of uniform electric field, as shown in Figure 16.67. Along a path from B to A, the change in potential is-2200V. The distance from A to B is 0.28m. What is the magnitude of the electric field in this region?

LocationsA=<a,0,0>andB=<b,0,0>are on the +x axis, as shown in Figure 16.61. Four possible expressions for the electric field along the x axis are given below. For each expression for the electric field, select the correct expression (1–8) for the potential differenceVA-VB. In each case K is a numerical constant with appropriate units.

(a)E→=<Kx2,0,0>(b)E→=<Kx3,0,0>(c)E→=<Kx,0,0>(b)E→=<Kx,0,0>(1)VA-VB=0(2)VA-VB=K(a-b)(3)VA-VB=K(1a-1b)(4)VA-VB=K(1a3a-1b3b)(5)VA-VB=12K(b2-a2)(6)VA-VB=KIn(ba)(7)VA-VB=K(a3-b3)(8)VA-VB=12K(1a2-1b2)

An electron starts from rest in a vacuum, in a region of strong field. The electron moves through a potential difference of 44V. (a) What is the kinetic energy of the electron in electron volts (eV)? (b) Which of the following statements would be true if the particle were a proton? Choose both if they are both correct. (1) The kinetic energy of the proton would be negative. (2) The proton would move in the opposite direction from the electron.

What is the potential (relative to infinity) at location B, a distance h from a ring of radius a with charge –Q as shown in figure 16.94?

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=4×10-7 C.

(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, E→⊥ΔI→(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" ΔI→is opposite to the direction of . (2) Negative, becauseΔI→ is in the same direction asE→ . (3) Zero, becauseΔI→⊥E→. (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, Δ°­+Δ±«=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?

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