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Question: A \({\bf{3}}{\bf{.4}}\;{\bf{\mu C}}\) and a \({\bf{ - 2}}{\bf{.6}}\;{\bf{\mu C}}\) charge are placed 2.5 cm apart. At what points along the line joining them is (a) the electric field zero, and (b) the electric potential zero?

Short Answer

Expert verified

(a)The electric field is zero at 17.4 cm from the negative charge and on the opposite side from the positive charge.

(b) The one point where the net electric potential is zero is at 1.1 cm from the negative charge and towards the positive charge. The second point where the net electric potential is zero is at 8.1 cm from the negative charge and away from the positive charge.

Step by step solution

01

Understanding of electric field  

The magnitude of the electric field can be calculated by evaluating the charge's value and the charge's distance from a particular point.

In this question, the direction of the electric field at a point is away from the positive charge and towards the negative charge.

02

Given information 

The first charge is,\( {q_1} = 3.4\;{\rm{\mu C}}\).

The second charge is,\( {q_2} = - 2.6\;{\rm{\mu C}}\).

The separation between the charges is,\( d = 2.5\;{\rm{cm}}\).

03

(a) Evaluation of the point where the net electric field is zero. 

The schematic diagram for the problem can be drawn as:

Here,\({E_1}\)and \({E_2}\)are the electric fields due to charge\({q_1}\)and \({q_2}\) respectively and \(P\) is the point at a distance \(x\) from the negative charge along the line joining the two charges where the net electric field is zero.

For the net electric field to be zero, we can write:

\( \begin{aligned}{c}{E_{{\rm{net}}}} = 0\\{E_1} - {E_2} = 0\\{E_1} = {E_2}\\\frac{{k{q_1}}}{{{{\left( {d + x} \right)}^2}}} = \frac{{k{q_2}}}{{{x^2}}}\end{aligned}\)

Solve further the above equation.

\( \begin{aligned}{c}\frac{{d + x}}{x} = \sqrt {\frac{{{q_1}}}{{{q_2}}}} \\x = \frac{d}{{\sqrt {\left| {\frac{{{q_1}}}{{{q_2}}}} \right| - 1} }}\\ = \frac{{\left( {2.5\;{\rm{cm}}} \right)}}{{\sqrt {\left| {\frac{{\left( {3.4\;{\rm{\mu C}}} \right)}}{{\left( { - 2.6\;{\rm{\mu C}}} \right)}}} \right| - 1} }}\\ = 17.4\;{\rm{cm}}\end{aligned}\)

Thus, the electric field is zero at 17.4 cm from the negative charge and on the opposite side from the positive charge.

04

(b) Evaluation of the points where the net electric potential is zero.

The schematic diagram can be drawn as:

The\(P\) and \(R\) are the two points where the electric potential can be zero. The points where the electric potential is zero lies near the smaller magnitude charge.

For the net electric potential to be zero at point R, one can write:

\( \begin{aligned}{c}{V_1} = \frac{{k{q_1}}}{{d - {x_1}}} + \frac{{k{q_2}}}{{{x_1}}}\\0 = \frac{{k{q_1}}}{{d - {x_1}}} + \frac{{k{q_2}}}{{{x_1}}}\\\frac{{k{q_1}}}{{d - {x_1}}} = - \frac{{k{q_2}}}{{{x_1}}}\\{q_1}{x_1} = - {q_2}\left( {d - {x_1}} \right)\end{aligned}\)

Solve further the above equation.

\( \begin{aligned}{c}{x_1} = \frac{{ - {q_2}d}}{{\left( {{q_1} - {q_2}} \right)}}\\ = \frac{{ - \left( { - 2.6\;{\rm{\mu C}}} \right)\left( {2.5\;{\rm{cm}}} \right)}}{{\left( {\left( {3.4\;{\rm{\mu C}}} \right) - \left( { - 2.6\;{\rm{\mu C}}} \right)} \right)}}\\ = 1.08\;{\rm{cm}}\\ \approx 1.1\;{\rm{cm}}\end{aligned}\)

Thus, the one point where the net electric potential is zero is at 1.1 cm from the negative charge and towards the positive charge.

For the net electric potential to be zero at point P, one can write:

\( \begin{aligned}{c}{V_2} = \frac{{k{q_1}}}{{d + {x_2}}} + \frac{{k{q_2}}}{{{x_2}}}\\0 = \frac{{k{q_1}}}{{d + {x_2}}} + \frac{{k{q_2}}}{{{x_2}}}\\\frac{{k{q_1}}}{{d + {x_2}}} = - \frac{{k{q_2}}}{{{x_2}}}\\{q_1}{x_2} = - {q_2}\left( {d + {x_2}} \right)\end{aligned}\)

Solve further the above equation.

\( \begin{aligned}{c}{x_2} = - \frac{{{q_2}d}}{{\left( {{q_1} + {q_2}} \right)}}\\ = \frac{{ - \left( { - 2.6\;{\rm{\mu C}}} \right)\left( {2.5\;{\rm{cm}}} \right)}}{{\left( {\left( {3.4\;{\rm{\mu C}}} \right) + \left( { - 2.6\;{\rm{\mu C}}} \right)} \right)}}\\ = 8.12\;{\rm{cm}} \approx {\rm{8}}{\rm{.1}}\;{\rm{cm}}\end{aligned}\)

Thus, the second point where the net electric potential is zero is at 8.1 cm from the negative charge and away from the positive charge.

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Most popular questions from this chapter

If the electric field \({\bf{\vec E}}\) is uniform in a region, what can you infer about the electric potential V? If V is uniform in a region of space, what can you infer about \({\bf{\vec E}}\).

(II) Point a is 62 cm north of a \( - {\bf{3}}{\bf{.8}}\;{\bf{\mu C}}\) point charge, and point b is 88 cm west of the charge (Fig. 17โ€“40). Determine (a) \({{\bf{V}}_{\bf{b}}} - {{\bf{V}}_{\bf{a}}}\) and (b) \({{\bf{\vec E}}_{\bf{b}}} - {{\bf{\vec E}}_{\bf{a}}}\) (magnitude and direction).

FIGURE 17โ€“40 Problem 27.

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

In the dynamic random access memory (DRAM) of a computer, each memory cell contains a capacitor for charge storage. Each of these cells represents a single binary bit value of โ€œ1โ€ when its 35-fF capacitor \(\left( {{\bf{1}}\;{\bf{fF = 1}}{{\bf{0}}^{{\bf{ - 15}}}}\;{\bf{F}}} \right)\) is charged at 1.5 V, or โ€œ0โ€ when uncharged at 0 V.

(a) When fully charged, how many excess electrons are on a cell capacitorโ€™s negative plate?

(b) After charge has been placed on a cell capacitorโ€™s plate, it slowly โ€œleaksโ€ off at a rate of about \({\bf{0}}{\bf{.30}}\;{\bf{fC/s}}\). How long does it take for the potential difference across this capacitor to decrease by 2.0% from its fully charged value? (Because of this leakage effect, the charge on a DRAM capacitor is โ€œrefreshedโ€ many times per second.) Note: A DRAM cell is shown in Fig. 21โ€“29.

Four identical point charges are arranged at the corners of a square [Hint: Draw a figure]. The electric field E and potential V at the centre of the square are

(a) \(E = 0\), \(V = 0\).

(b) \(E = 0\), \(V \ne 0\).

(c) \(E \ne 0\), \(V \ne 0\).

(d) \(E \ne 0\), \(V = 0\).

(e) \(E = V\) regardless of the value.

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