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Bare free charges do not remain stationary when close together. To illustrate this, calculate the acceleration of two isolated protons separated by\({\bf{2}}.{\bf{00}}{\rm{ }}{\bf{nm}}\)(a typical distance between gas atoms). Explicitly show how you follow the steps in the Problem-Solving Strategy for electrostatics.

Short Answer

Expert verified

The acceleration of the proton is \(3.45 \times {10^{16}}{\rm{ m/}}{{\rm{s}}^{\rm{2}}}\).

Step by step solution

01

Newton’s second law of motion

According to the Newton’s second law of motion, the rate of change of momentum is directly proportional to the force applied.

\(\begin{aligned} {\rm{F\mu }}\frac{{{\rm{\Delta p}}}}{{{\rm{\Delta t}}}}\\{\rm{ = k}}\left( {\frac{{{\rm{mv - mu}}}}{{{\rm{\Delta t}}}}} \right)\\{\rm{ = k}}\left( {{\rm{m}}\left( {\frac{{{\rm{v - u}}}}{{{\rm{\Delta t}}}}} \right)} \right)\end{aligned}\)

Here, F is the force, \(\Delta p\) is the change in momentum, \({\rm{\Delta t}}\) is the change in time, k is the proportionality constant (k =1), m is the mass, v is the final velocity, and u is the initial velocity.

The acceleration of the body is,

\(a\, = \,\frac{{v{\rm{ }} - {\rm{ }}u}}{{\Delta t}}\)

From equation (1.1) and (1.2),

\(F = ma\)

02

Acceleration of the proton

The electrostatic force between two protons is,

\(F = \frac{{Kqq}}{{{r^2}}}\)

Here, \(K\) is the electrostatic force constant \(\left( {K = 9 \times {{10}^9}{\rm{ N \times }}{{\rm{m}}^{\rm{2}}}{\rm{/}}{{\rm{C}}^{\rm{2}}}} \right)\), q is the charge on proton \(\left( {q = 1.6 \times {{10}^{ - 19}}{\rm{ }}C} \right)\), and r is the separation between the protons \(\left( {r = 2.00{\rm{ }}nm} \right)\).

From equation (1.3), and (1.4),

\(ma = \frac{{Kqq}}{{{r^2}}}\)

Here, m is the mass of proton \(\left( {m = 1.67 \times {{10}^{ - 27}}{\rm{ }}kg} \right)\), and a is the acceleration of proton.

The expression for the acceleration of proton is,

\(a = \frac{{Kqq}}{{m{r^2}}}\)

Substituting all known values,

\(\begin{aligned} a &= \frac{{\left( {9 \times {{10}^9}{\rm{ N}} \cdot {{\rm{m}}^{\rm{2}}}{\rm{/}}{{\rm{C}}^{\rm{2}}}} \right) \times \left( {1.6 \times {{10}^{ - 19}}{\rm{ C}}} \right) \times \left( {1.6 \times {{10}^{ - 19}}{\rm{ C}}} \right)}}{{\left( {1.67 \times {{10}^{ - 27}}{\rm{ kg}}} \right) \times {{\left( {2.00{\rm{ nm}}} \right)}^2}}}\\ &= \frac{{\left( {9 \times {{10}^9}{\rm{ N}} \cdot {{\rm{m}}^{\rm{2}}}{\rm{/}}{{\rm{C}}^{\rm{2}}}} \right) \times \left( {1.6 \times {{10}^{ - 19}}{\rm{ C}}} \right) \times \left( {1.6 \times {{10}^{ - 19}}{\rm{ C}}} \right)}}{{\left( {1.67 \times {{10}^{ - 27}}{\rm{ kg}}} \right) \times {{\left( {\left( {2.00{\rm{ nm}}} \right) \times \left( {\frac{{{{10}^{ - 9}}{\rm{ m}}}}{{1{\rm{ nm}}}}} \right)} \right)}^2}}}\\ &= 3.45 \times {10^{16}}{\rm{ m/}}{{\rm{s}}^{\rm{2}}}\end{aligned}\)

Hence, the acceleration of the proton is \(3.45 \times {10^{16}}{\rm{ m/}}{{\rm{s}}^{\rm{2}}}\).

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Most popular questions from this chapter

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.

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).

If two equal charges each of\({\rm{1 C}}\)each are separated in air by a distance of\({\rm{1 km}}\), what is the magnitude of the force acting between them? You will see that even at a distance as large as\({\rm{1 km}}\), the repulsive force is substantial because\({\rm{1 C}}\)is a very significant amount of charge.

Sketch the electric field lines in the vicinity of the conductor in Figure 18.49 given the field was originally uniform and parallel to the object’s long axis. Is the resulting field small near the long side of the object?

Figure 18.49

The practical limit to an electric field in air is about\(3.00 \times {10^6}{\rm{ N}}/{\rm{C}}\). Above this strength, sparking takes place because air begins to ionize and charges flow, reducing the field. (a) Calculate the distance a free proton must travel in this field to reach\(3.00\% \)of the speed of light, starting from rest. (b) Is this practical in air, or must it occur in a vacuum?

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