(II) How much work must be done to bring three electrons from a great distance apart to \({\bf{1}}{\bf{.0 \times 1}}{{\bf{0}}^{{\bf{ - 10}}}}\;{\bf{m}}\) from one another (at the corners of an equilateral triangle)?

Short Answer

Expert verified

The total work done in bringing the three charges from a great distance apart to \(1.0 \times {10^{ - 10}}\;{\rm{m}}\)from one another is \(6.9 \times {10^{ - 18}}\;{\rm{J}}\).

Step by step solution

01

Step 1:Understanding of work done

The value of the work done can be calculated by multiplying the value of the magnitude of the charge with the difference in the potential. Its value is altered linearly to the value of the magnitude of the charge.

02

Given information

The distance is,\(L = 1.0 \times {10^{ - 10}}\;{\rm{m}}\).

The charge on the electron is, \(e = - 1.6 \times {10^{ - 19}}\;{\rm{C}}\)

03

Evaluation of the total work done in bringing the three charges from a greatest distance from one another

The schematic diagram for the problem can be drawn as:

Initially, there is no other charge is present. Thus, the work done to bring the first electron from its initial position will be:

\({W_1} = 0\)

The expression for the potential difference between the electrons 1 and 2 can be written as:

\(\begin{aligned}\Delta {V_{12}} &= \frac{{k\left( { - e} \right)}}{L}\\\Delta {V_{12}} &= \frac{{ - ke}}{L}\end{aligned}\)

The expression for the work done in bringing the second electron of charge \( - e\)with a distance \(L\) to the first electron is as follows:

\(\begin{aligned}{W_2} &= \left( { - e} \right)\Delta {V_{12}}\\{W_2} &= \left( { - e} \right)\left( {\frac{{ - ke}}{L}} \right)\\{W_2} &= \frac{{k{e^2}}}{L}\end{aligned}\)

The expression for the potential difference between the electrons 1 and 3 can be written as:

\(\begin{aligned}\Delta {V_{13}} &= \frac{{k\left( { - e} \right)}}{L}\\\Delta {V_{13}} &= \frac{{ - ke}}{L}\end{aligned}\)

The expression for the potential difference between the electrons 2 and 3 can be written as:

\(\begin{aligned}\Delta {V_{23}} &= \frac{{k\left( { - e} \right)}}{L}\\\Delta {V_{23}} &= \frac{{ - ke}}{L}\end{aligned}\)

The expression for the work done in bringing the third electron to the position with the equal distance of the charge 1 and 2 is as follows:

\(\begin{aligned}{W_3} &= \left( { - e} \right)\left( {\frac{{ - ke}}{L}} \right) + \left( { - e} \right)\left( {\frac{{ - ke}}{L}} \right)\\{W_3} &= \frac{{2k{e^2}}}{L}\end{aligned}\)

The expression for the work done in bringing the third electron to the position with the equal distance of the charge 1 and 2 is as follows:

\(\begin{aligned}{W_3} &= \left( { - e} \right)\left( {\frac{{ - ke}}{L}} \right) + \left( { - e} \right)\left( {\frac{{ - ke}}{L}} \right)\\{W_3} &= \frac{{2k{e^2}}}{L}\end{aligned}\)

The total work done in bringing the three charges from a greatest distance from one another can be calculated as:

\(\begin{aligned}W &= {W_1} + {W_2} + {W_3}\\W &= 0 + \frac{{k{e^2}}}{L} + \frac{{2k{e^2}}}{L}\\W &= \frac{{3k{e^2}}}{L}\end{aligned}\)

Substitute the values in the above equation.

\(\begin{aligned}W &= \frac{{\left( 3 \right)\left( {9 \times {{10}^9}\;{{{\rm{N}} \cdot {{\rm{m}}^{\rm{2}}}} \mathord{\left/{\vphantom {{{\rm{N}} \cdot {{\rm{m}}^{\rm{2}}}} {{{\rm{C}}^{\rm{2}}}}}} \right.} {{{\rm{C}}^{\rm{2}}}}}} \right){{\left( {1.6 \times {{10}^{ - 19}}\;{\rm{C}}} \right)}^2}}}{{\left( {1.0 \times {{10}^{ - 10}}\;{\rm{m}}} \right)}}\\W &= 6.9 \times {10^{ - 18}}\;{\rm{J}}\end{aligned}\)

Thus, the total work done in bringing the three charges from a great distance apart to \(1.0 \times {10^{ - 10}}\;{\rm{m}}\) from one another is \(6.9 \times {10^{ - 18}}\;{\rm{J}}\).

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

(I) The two plates of a capacitor hold \({\bf{ + 2500}}\;{\bf{\mu C}}\) and \( - {\bf{2500}}\;{\bf{\mu C}}\) of charge, respectively, when the potential difference is 960 V. What is the capacitance.

A parallel-plate capacitor with plate area\({\bf{A = 2}}{\bf{.0}}\;{{\bf{m}}{\bf{2}}}\)and plate separation\({\bf{d = 3}}{\bf{.0}}\;{\bf{mm}}\)is connected to a 35-V battery (Fig. 17–51a).

(a) Determine the charge on the capacitor, the electric field, the capacitance, and the energy stored in the capacitor.

(b) With the capacitor still connected to the battery, a slab of plastic with dielectric strength K =3.2 is placed between the plates of the capacitor, so that the gap is completely filled with the dielectric (Fig. 17–51b). What are the new values of charge, electric field, capacitance, and the energy stored in the capacitor?\(\left( {{\bf{1}}\;{\bf{byte = 8}}\;{\bf{bits}}{\bf{.}}} \right)\)

FIGURE 17-51 Problem 96

If a negative charge is initially at rest in an electric field, will it move toward a region of higher potential or lower potential? What about a positive charge? How does the potential energy of the charge change in each instance? Explain.

Question: (I) Write the binary number 01010101 as a decimal number.

(II) Two identical \({\bf{ + 9}}{\bf{.5}}\;{\bf{\mu C}}\) point charges are initially 5.3 cm from each other. If they are released at the same instant from rest, how fast will each be moving when they are very far away from each other? Assume they have identical masses of 1.0 mg.

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free