Question: (III) A \({\bf{3}}{\bf{.70}}\;{\bf{\mu F}}\) capacitor is charged by a 12.0-V battery. It is disconnected from the battery and then connected to an uncharged \({\bf{5}}{\bf{.00}}\;{\bf{\mu F}}\) capacitor (Fig.17–43). Determine the total stored energy (a) before the two capacitors are connected, and (b) after they are connected. (c) What is the change in energy?

Short Answer

Expert verified

(a) The total energy stored before the capacitors are connected is \(2.66 \times {10^{ - 4}}\;{\rm{J}}\).

(b) The total energy stored after the capacitors are connected is \(1.13 \times {10^{ - 4}}\;{\rm{J}}\).

(c) The change in energy is \( - 1.53 \times {10^{ - 4}}\;{\rm{J}}\).

Step by step solution

01

Understanding the energy stored in a capacitor

A capacitor is a charge and energy storage device. The stored energy is proportional to the square of the potential difference between the plates.

The expression for stored energy in the capacitor is given as:

\({\rm{PE}} = \frac{1}{2}C{V^2}\) … (i)

Here, C is the capacitance and V is the potential difference.

02

Given data

The capacitance of the first capacitor is,\({C_1} = 3.70\;\mu {\rm{F}} = 3.70 \times {10^{ - 6}}\;{\rm{F}}\)

The potential across the first capacitor is,\({V_1} = 12\;{\rm{V}}\)

The capacitance of the second capacitor is, \({C_2} = 5.00\;\mu {\rm{F}} = 5.00 \times {10^{ - 6}}\;{\rm{F}}\)

03

(a) Determination of total energy stored before the capacitors are connected

From equation (i), the energy stored in the capacitor is,

\({U_1} = \frac{1}{2}{C_1}V_1^2\)

Substitute the values in the above expression.

\(\begin{aligned}{c}{U_1} &= \frac{1}{2}\left( {3.70 \times {{10}^{ - 6}}\;{\rm{F}}} \right)\left( {12.0\;{\rm{V}}} \right)\\ &= 2.66 \times {10^{ - 4}}\;{\rm{J}}\end{aligned}\)

The energy stored in the second capacitor is zero as it is initially uncharged.

Thus, the total energy stored before the capacitors are connected is \(2.66 \times {10^{ - 4}}\;{\rm{J}}\).

04

(b) Determination of total energy stored after the capacitors are connected

The initial charge on the first capacitor is, \({Q_1} = {C_1}{V_1}\)

The initial charge on the second capacitor is, \({Q_2} = 0\)

After joining, the total charge is,

\(\begin{aligned}{c}Q &= {Q_1} + {Q_2}\\ &= {C_1}{V_1} + 0\\ &= {C_1}{V_1}\end{aligned}\)

After joining, the capacitance of the parallel combination is,

\(C = {C_1} + {C_2}\)

After joining, the final potential difference is,

\(\begin{aligned}{c}V &= \frac{Q}{C}\\ &= \frac{{{C_1}{V_1}}}{{{C_1} + {C_2}}}\\ &= \frac{{\left( {3.70\;\mu {\rm{F}}} \right)\left( {12\;{\rm{V}}} \right)}}{{\left( {3.70\;\mu {\rm{F}}} \right) + \left( {5.00\;\mu {\rm{F}}} \right)}}\\ &= 5.103\;{\rm{V}}\end{aligned}\)

The final total energy stored in the system is,

\(\begin{aligned}{c}U &= \frac{1}{2}\left( {{C_1} + {C_2}} \right){V^2}\\ &= \frac{1}{2}\left( {\left( {3.70 \times {{10}^{ - 6}}\;{\rm{F}}} \right) + \left( {5.00 \times {{10}^{ - 6}}\;{\rm{F}}} \right)} \right){\left( {5.103\;{\rm{V}}} \right)^2}\\ &= 1.13 \times {10^{ - 4}}\;{\rm{J}}\end{aligned}\)

Thus, the total energy stored after the capacitors are connected is \(1.13 \times {10^{ - 4}}\;{\rm{J}}\).

05

(c) Determination of change in energy

The change in energy is,

\(\begin{aligned}{c}\Delta U &= U - {U_1}\\ &= \left( {1.13 \times {{10}^{ - 4}}\;{\rm{J}}} \right) - \left( {2.66 \times {{10}^{ - 4}}\;{\rm{J}}} \right)\\ &= - 1.53 \times {10^{ - 4}}\;{\rm{J}}\end{aligned}\)

Thus, the change in energy is \( - 1.53 \times {10^{ - 4}}\;{\rm{J}}\).

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Most popular questions from this chapter

Question: (II) A homemade capacitor is assembled by placing two 9-in. pie pans 4 cm apart and connecting them to the opposite terminals of a 9-V battery. Estimate (a) the capacitance, (b) the charge on each plate, (c) the electric field halfway between the plates, and (d) the work done by the battery to charge them. (e) Which of the above values change if a dielectric is inserted?

In an older television tube, electrons are accelerated by thousands of volts through a vacuum. If a television set were laid on its back, would electrons be able to move upward against the force of gravity? What potential difference, acting over a distance of 2.4 cm, would be needed to balance the downward force of gravity so that an electron would remain stationary? Assume that the electric field is uniform.

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(a) When fully charged, how many excess electrons are on a cell capacitor’s negative plate?

(b) After charge has been placed on a cell capacitor’s plate, it slowly “leaks” 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 “refreshed” many times per second.) Note: A DRAM cell is shown in Fig. 21–29.

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