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The classic Millikan oil drop experiment was the first to obtain an accurate measurement of the charge on an electron. In it, oil drops were suspended against the gravitational force by a vertical electric field. (See Figure 18.58.) Given the oil drop to be\(1.00{\rm{ }}\mu {\rm{m}}\)in radius and have a density of\(920{\rm{ kg}}/{{\rm{m}}^3}\): (a) Find the weight of the drop. (b) If the drop has a single excess electron, find the electric field strength needed to balance its weight.

Figure 18.58 In the Millikan oil drop experiment, small drops can be suspended in an electric field by the force exerted on a single excess electron. Classically, this experiment was used to determine the electron charge\({q_e}\)by measuring the electric field and mass of the drop.

Short Answer

Expert verified

(a) The weight of the drop is\(3.78 \times {10^{ - 16}}{\rm{ N}}\).

(b) The strength of the electric field is \(2.36 \times {10^5}{\rm{ N}}/{\rm{C}}\).

Step by step solution

01

Mass

Mass is a fundamental quantity of the object which remains constant throughout the universe. The mass is related to the density of the material as,

\(m = \rho V\)

Here, \(\rho \) is the density of the material and \(V\) is the volume of the object.

02

(a) Weight of the drop

The volume of the sphere is,

\(V = \frac{4}{3}\pi {r^3}\)

Here,\(r\)is the radius of the sphere.

From equation (1.1) and (1.2), the mass of the object is,

\(m = \frac{4}{3}\pi \rho {r^3}\)

The weight of the object is,

\({F_g} = mg\)

Using equation (1.3),

\({F_{_g}} = \frac{4}{3}\pi \rho {r^3}g\)

Substitute\(920{\rm{ kg}}/{{\rm{m}}^3}\)for\(\rho \),\(1.00{\rm{ }}\mu {\rm{m}}\)for\(r\), and\(9.81{\rm{ m}}/{{\rm{s}}^2}\)for g.

\(\begin{array}{c}{F_g} = \frac{4}{3}\pi \times \left( {920{\rm{ kg}}/{{\rm{m}}^3}} \right) \times {\left( {1.00{\rm{ }}\mu {\rm{m}}} \right)^3} \times \left( {9.81{\rm{ m}}/{{\rm{s}}^2}} \right)\\ = \frac{4}{3}\pi \times \left( {920{\rm{ kg}}/{{\rm{m}}^3}} \right) \times {\left[ {\left( {1.00{\rm{ }}\mu {\rm{m}}} \right) \times \left( {\frac{{{{10}^{ - 6}}{\rm{ m}}}}{{1{\rm{ }}\mu {\rm{m}}}}} \right)} \right]^3} \times \left( {9.81{\rm{ m}}/{{\rm{s}}^2}} \right)\\ = 3.78 \times {10^{ - 16}}{\rm{ N}}\end{array}\)

Hence, the weight of the drop is \(3.78 \times {10^{ - 16}}{\rm{ N}}\).

03

(b) The strength of the electric field

The weight of the oil drop is supported by the electrostatic force due to the electric field. Therefore,

\({F_g} = qE\)

Here,\(q\)is the magnitude of the charge on electron, and\(E\)is the electric field.

The expression for the electric field is,

\(E = \frac{{{F_g}}}{q}\)

Substitute\(3.78 \times {10^{ - 14}}{\rm{ N}}\) for\({F_g}\)and\(1.6 \times {10^{ - 19}}{\rm{ C}}\)for\(q\),

\(\begin{array}{c}E = \frac{{\left( {3.78 \times {{10}^{ - 14}}{\rm{ N}}} \right)}}{{\left( {1.6 \times {{10}^{ - 19}}{\rm{ C}}} \right)}}\\ = 2.36 \times {10^5}{\rm{ N}}/{\rm{C}}\end{array}\)

Hence, the strength of the electric field is \(2.36 \times {10^5}{\rm{ N}}/{\rm{C}}\).

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Most popular questions from this chapter

Sketch the electric field lines in the vicinity of two opposite charges, where the negative charge is three times greater in magnitude than the positive. (See Figure for a similar situation).

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.

Why do most objects tend to contain nearly equal numbers of positive and negative charges?

(a) Find the total Coulomb force on a charge of \(2.00{\rm{ nC}}\) located at \(x = 4.00{\rm{ cm}}\) in Figure 18.52 (b), given that \(q = 1.00{\rm{ \mu C}}\). (b) Find the \({\rm{x}}\)-position at which the electric field is zero in Figure 18.52 (b).

Figure 18.52 (a) Point charges located at \[{\bf{3}}.{\bf{00}},{\rm{ }}{\bf{8}}.{\bf{00}},{\rm{ }}{\bf{and}}{\rm{ }}{\bf{11}}.{\bf{0}}{\rm{ }}{\bf{cm}}\] along the x-axis. (b) Point charges located at \[{\bf{1}}.{\bf{00}},{\rm{ }}{\bf{5}}.{\bf{00}},{\rm{ }}{\bf{8}}.{\bf{00}},{\rm{ }}{\bf{and}}{\rm{ }}{\bf{14}}.{\bf{0}}{\rm{ }}{\bf{cm}}\] along the x-axis

(a) By what factor must you change the distance between two-point charges to change the force between them by a factor of \(10\)? (b) Explain how the distance can either increase or decrease by this factor and still cause a factor of \(10\) change in the force.

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