Question: Near the surface of the Earth there is an electric field of about \({\bf{150}}\;{{\bf{V}} \mathord{\left/{\vphantom {{\bf{V}} {\bf{m}}}} \right.} {\bf{m}}}\)which points downward. Two identical balls with mass \({\bf{m = 0}}{\bf{.670}}\;{\bf{kg}}\) are dropped from a height of 2.00 m, but one of the balls is positively charged with \({{\bf{q}}_{\bf{1}}}{\bf{ = 650}}\;{\bf{\mu C}}\), and the second is negatively charged with \({{\bf{q}}_{\bf{2}}}{\bf{ = }} - {\bf{650}}\;{\bf{\mu C}}\). Use conservation of energy to determine the difference in the speed of the two balls when they hit the ground. (Neglect air resistance.)

Short Answer

Expert verified

The difference in the speed of the balls when they are hitting the ground is \[0.093\;{{\rm{m}} \mathord{\left/{\vphantom {{\rm{m}} {\rm{s}}}} \right.} {\rm{s}}}\].

Step by step solution

01

Step 1:Understanding of the electric potential difference  

The value of the electric potential difference can be calculated by multiplying the value of the magnitude of the electric field with the distance between the two points.

02

Given information 

The electric field is,\[E = 150\;{{\rm{V}} \mathord{\left/{\vphantom {{\rm{V}} {\rm{m}}}} \right.} {\rm{m}}}\].

The mass of the balls is,\[m = 0.670\;{\rm{kg}}\].

The height is,\[h = 2.00\;{\rm{m}}\].

The charge on one ball is,\[{q_1} = 650\;{\rm{\mu C}}\].

The charge on another ball is,\[{q_2} = - 650\;{\rm{\mu C}}\].

03

Evaluation of the potential difference 

The potential difference can be calculated as:

\[\begin{array}{c}{V_1} - {V_2} = Eh\\ = \left({150\;{{\rm{V}} \mathord{\left/{\vphantom {{\rm{V}} {\rm{m}}}} \right.} {\rm{m}}}} \right)\left( {2\;{\rm{m}}} \right)\\ = 300\;{\rm{V}}\end{array}\]

04

Evaluation of the speed of both the balls 

Apply the conservation of energy principle at the time of dropping of the ball and the ball at the surface of the Earth.

\[\begin{array}{c}mgh + q{V_1} = \frac{1}{2}m{v^2} + q{V_2}\\\frac{1}{2}m{v^2} = mgh + q\left( {{V_1} - {V_2}} \right)\\v = \sqrt {\frac{{2mgh + 2q\left( {{V_1} - {V_2}} \right)}}{m}} \\v = \sqrt {2gh + \frac{{2q\left( {{V_1} - {V_2}} \right)}}{m}} \end{array}\]

The velocity of the positively charged ball can be calculated as:

\[\begin{array}{c}{v_{{q_1}}} = \sqrt {2gh + \frac{{2{q_1}\left( {{V_1} - {V_2}} \right)}}{m}} \\ = \sqrt {2\left( {9.8\;{{\rm{m}} \mathord{\left/{\vphantom {{\rm{m}} {{{\rm{s}}^{\rm{2}}}}}} \right.} {{{\rm{s}}^{\rm{2}}}}}} \right)\left( {2\;{\rm{m}}} \right) + \frac{{2\left\{ {\left( {{\rm{650}}\;{\rm{\mu C}}} \right)\left( {\frac{{{\rm{1}}{{\rm{0}}^{{\rm{ - 6}}}}\;{\rm{C}}}}{{{\rm{1}}\;{\rm{\mu C}}}}} \right)} \right\}\left( {300\;{\rm{V}}} \right)}}{{\left( {0.670\;{\rm{kg}}} \right)}}} \\ = 6.307\;{{\rm{m}} \mathord{\left/{\vphantom {{\rm{m}} {\rm{s}}}} \right.} {\rm{s}}}\end{array}\]

The velocity of the negatively charged ball can be calculated as:

\[\begin{array}{c}{v_{{q_2}}} = \sqrt {2gh + \frac{{2{q_2}\left( {{V_1} - {V_2}} \right)}}{m}} \\ = \sqrt {2\left( {9.8\;{{\rm{m}} \mathord{\left/{\vphantom {{\rm{m}} {{{\rm{s}}^{\rm{2}}}}}} \right.} {{{\rm{s}}^{\rm{2}}}}}} \right)\left( {2\;{\rm{m}}} \right) + \frac{{2\left\{ {\left( {{\rm{ - 650}}\;{\rm{\mu C}}} \right)\left( {\frac{{{\rm{1}}{{\rm{0}}^{{\rm{ - 6}}}}\;{\rm{C}}}}{{{\rm{1}}\;{\rm{\mu C}}}}} \right)} \right\}\left( {300\;{\rm{V}}} \right)}}{{\left( {0.670\;{\rm{kg}}} \right)}}} \\ = 6.214\;{{\rm{m}} \mathord{\left/{\vphantom {{\rm{m}} {\rm{s}}}} \right.} {\rm{s}}}\end{array}\]

05

Evaluation of the difference in the speed of the balls when they are hitting the ground 

The difference in the speed of the balls when they are hitting the ground can be calculated as:

\[\begin{array}{c}v = {v_{{q_1}}} - {v_{{q_2}}}\\ = \left( {6.307\;{{\rm{m}} \mathord{\left/{\vphantom {{\rm{m}} {\rm{s}}}} \right.} {\rm{s}}}} \right) - \left( {6.214\;{{\rm{m}} \mathord{\left/{\vphantom {{\rm{m}} {\rm{s}}}} \right.} {\rm{s}}}} \right)\\ = 0.093\;{{\rm{m}} \mathord{\left/{\vphantom {{\rm{m}} {\rm{s}}}} \right.} {\rm{s}}}\end{array}\]

Thus, the difference in the speed of the balls when they are hitting the ground is \[0.093\;{{\rm{m}} \mathord{\left/{\vphantom {{\rm{m}} {\rm{s}}}} \right.} {\rm{s}}}\].

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Most popular questions from this chapter

Which of the following statements is valid?

(a) If the potential at a particular point is zero, the field at that point must be zero.

(b) If the field at a particular point is zero, the potential at that point must be zero.

(c) If the field throughout a particular region is constant, the potential throughout that region must be zero.

(d) If the potential throughout a particular region is constant, the field throughout that region must be zero.

Two identical positive charges are placed near each other. At the point halfway between the two charges,

(a) the electric field is zero and the potential is positive.

(b) the electric field is zero and the potential is zero.

(c) the electric field is not zero and the potential is positive.

(d) the electric field is not zero and the potential is zero.

(e) None of these statements is true.

(II) The dipole moment, considered as a vector, points from the negative to the positive charge. The water molecule, Fig. 17–42, has a dipole moment \({\bf{\vec p}}\) which can be considered as the vector sum of the two dipole moments, \({{\bf{\vec p}}_{\bf{1}}}\) and \({{\bf{\vec p}}_{\bf{2}}}\) as shown. The distance between each H and the O is about \({\bf{0}}{\bf{.96 \times 1}}{{\bf{0}}^{{\bf{ - 10}}}}\;{\bf{m}}\). The lines joining the centre of the O atom with each H atom make an angle of 104°, as shown, and the net dipole moment has been measured to be \({\bf{p = 6}}{\bf{.1 \times 1}}{{\bf{0}}^{{\bf{ - 30}}}}\;{\bf{C}} \cdot {\bf{m}}\). Determine the charge q on each H atom.

FIGURE 17–42 Problem 34

Which of the following do not affect capacitance?

(a) Area of the plates.

(b) Separation of the plates.

(c) Material between the plates.

(d) Charge on the plates.

(e) Energy stored in the capacitor.

Question: Three charges are at the corners of an equilateral triangle (side l) as shown in Fig. 17–45. Determine the potential at the midpoint of each of the sides. Let \[{\bf{V = 0}}\] at \[{\bf{r = }}\infty \].

FIGURE 17–45 Problem 75.

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