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A\(5.00{\rm{ g}}\)charged insulating ball hangs on a\(30.0{\rm{ cm}}\)long string in a uniform horizontal electric field as shown in Figure 18.56. Given the charge on the ball is\(1.00{\rm{ }}\mu {\rm{C}}\), find the strength of the field.

Figure 18.56 A horizontal electric field causes the charged ball to hang at an angle of\(8.00^\circ \).

Short Answer

Expert verified

The strength of the electric field is \(6.89 \times {10^3}{\rm{ N}}/{\rm{C}}\).

Step by step solution

01

Electrostatic force

When a charged particle is placed in an electric, it experiences some electrostatic force.The expression for the force experienced by the charged particle is,

\({F_e} = qE\)

Here, \(q\) is the charge on the proton and \(E\) is the electric field.

02

Free body diagram of charged insulating ball

The free body diagram or the force diagram of the charged insulating ball when it is placed in an electric field is represented as,

Free body diagram of the charged insulating ball when it is placed in an electric field

Here, \(q\) is the charge on the insulating ball, \(E\) is the electric field \(qE\) is the force experienced by the charged insulating ball, \(m\) is the mass of the ball, \(g\) is the acceleration due to gravity, \(mg\) is the weight of the ball, and \(T\) is the tension force in the string.

03

Force equations

The equilibrium force equation in the horizontal direction is,

\(\begin{array}{c}\sum {{F_x}} = 0\\qE - T\sin \left( {{8^ \circ }} \right) = 0\\T\sin \left( {{8^ \circ }} \right) = qE\end{array}\)

The equilibrium force equation in the vertical direction is,

\(\begin{array}{c}\sum {{F_y}} = 0\\T\cos \left( {8^\circ } \right) - mg = 0\\T\cos \left( {8^\circ } \right) = mg\end{array}\)

Dividing equation (1.1) by (1.2),

\(\begin{array}{c}\frac{{T\sin \left( {8^\circ } \right)}}{{T\cos \left( {8^\circ } \right)}} = \frac{{qE}}{{mg}}\\\tan \left( {8^\circ } \right) = \frac{{qE}}{{mg}}\end{array}\)

Rearranging the above equation in order to get an expression for the electric field.

\(E = \frac{{mg\tan \left( {8^\circ } \right)}}{q}\)

Substitute\(5.00{\rm{ g}}\)for\(m\),\(9.81{\rm{ m}}/{{\rm{s}}^2}\)for\(g\)and\(1.00{\rm{ }}\mu {\rm{C}}\)for\(q\).

\(\begin{array}{c}E = \frac{{\left( {5.00{\rm{ g}}} \right) \times \left( {9.81{\rm{ m}}/{{\rm{s}}^2}} \right) \times \tan \left( {8^\circ } \right)}}{{\left( {1.00{\rm{ }}\mu {\rm{C}}} \right)}}\\ = \frac{{\left( {5.00{\rm{ g}}} \right) \times \left( {\frac{{{{10}^{ - 3}}{\rm{ kg}}}}{{1{\rm{ g}}}}} \right) \times \left( {9.81{\rm{ m}}/{{\rm{s}}^2}} \right) \times \tan \left( {8^\circ } \right)}}{{\left( {1.00{\rm{ }}\mu {\rm{C}}} \right) \times \left( {\frac{{{{10}^{ - 6}}{\rm{ C}}}}{{1{\rm{ }}\mu {\rm{C}}}}} \right)}}\\ = 6.89 \times {10^3}{\rm{ N}}/{\rm{C}}\end{array}\)

Hence, the strength of the electric field is \(6.89 \times {10^3}{\rm{ N}}/{\rm{C}}\).

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Most popular questions from this chapter

Calculate the magnitude of the electric field 2.00 m from a point charge of 5.00 mC (such as found on the terminal of a Van de Graaff).

A simple and common technique for accelerating electrons is shown in Figure 18.55, where there is a uniform electric field between two plates. Electrons are released, usually from a hot filament, near the negative plate, and there is a small hole in the positive plate that allows the electrons to continue moving. (a) Calculate the acceleration of the electron if the field strength is\(2.50 \times {10^4}{\rm{ N/C}}\). (b) Explain why the electron will not be pulled back to the positive plate once it moves through the hole.

Figure 18.55 Parallel conducting plates with opposite charges on them create a relatively uniform electric field used to accelerate electrons to the right. Those that go through the hole can be used to make a TV or computer screen glow or to produce X-rays.

Would the self-created electric field at the end of a pointed conductor, such as a lightning rod, remove positive or negative charge from the conductor? Would the same sign charge be removed from a neutral pointed conductor by the application of a similar externally created electric field? (The answers to both questions have implications for charge transfer utilizing points.)

An eccentric inventor attempts to levitate by first placing a large negative charge on himself and then putting a large positive charge on the ceiling of his workshop. Instead, while attempting to place a large negative charge on himself, his clothes fly off. Explain.

What is grounding? What effect does it have on a charged conductor? On a charged insulator?

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