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Question: The connections shown in figure are established with the switch S open. How much charge will flow th...

The connections shown in figure are established with the switch S open. How much charge will flow through the switch if it is closed?

Answer

0 μC\mu C

Explanation

Solution

When the switch S is open, the circuit consists of a 24V battery connected in parallel to two branches. The top branch has a 1 μ\muF capacitor (C1C_1). The bottom branch has a 2 μ\muF capacitor (C2C_2).

The diagram indicates that the left plates of both capacitors are connected to the positive terminal of the battery (24V), and the right plates of both capacitors are connected to the negative terminal of the battery (0V). Therefore, when the switch is open, both capacitors are directly across the 24V battery.

The voltage across the 1 μ\muF capacitor is V1=24VV_1 = 24V. The charge on the 1 μ\muF capacitor is Q1=C1V1=(1μF)×(24V)=24μCQ_1 = C_1 V_1 = (1 \mu F) \times (24V) = 24 \mu C.

The voltage across the 2 μ\muF capacitor is V2=24VV_2 = 24V. The charge on the 2 μ\muF capacitor is Q2=C2V2=(2μF)×(24V)=48μCQ_2 = C_2 V_2 = (2 \mu F) \times (24V) = 48 \mu C.

When the switch S is closed, it connects the right plate of the 1 μ\muF capacitor to the right plate of the 2 μ\muF capacitor. The circuit configuration remains the same: both capacitors are still connected in parallel across the 24V battery.

The voltage across the 1 μ\muF capacitor is V1=24VV'_1 = 24V. The charge on the 1 μ\muF capacitor is Q1=C1V1=(1μF)×(24V)=24μCQ'_1 = C_1 V'_1 = (1 \mu F) \times (24V) = 24 \mu C.

The voltage across the 2 μ\muF capacitor is V2=24VV'_2 = 24V. The charge on the 2 μ\muF capacitor is Q2=C2V2=(2μF)×(24V)=48μCQ'_2 = C_2 V'_2 = (2 \mu F) \times (24V) = 48 \mu C.

The charge that flows through the switch is the difference in charge that redistributes on the plates connected by the switch. Let's consider the charge on the right plates of the capacitors. Initially (switch open), the right plates are connected to the negative terminal (0V). Charge on the right plate of C1C_1 is q1r=Q1=24μCq_{1r} = -Q_1 = -24 \mu C. Charge on the right plate of C2C_2 is q2r=Q2=48μCq_{2r} = -Q_2 = -48 \mu C.

After closing the switch, the circuit configuration does not change the voltage across the capacitors. The right plates are still effectively at 0V potential relative to the negative terminal of the battery. Charge on the right plate of C1C_1 is q1r=Q1=24μCq'_{1r} = -Q'_1 = -24 \mu C. Charge on the right plate of C2C_2 is q2r=Q2=48μCq'_{2r} = -Q'_2 = -48 \mu C.

The total charge that flows through the switch is the sum of the change in charge on the right plates: Charge flow = (q1rq1r)+(q2rq2r)(q'_{1r} - q_{1r}) + (q'_{2r} - q_{2r}) = (24μC(24μC))+(48μC(48μC))(-24 \mu C - (-24 \mu C)) + (-48 \mu C - (-48 \mu C)) = 0μC+0μC=0μC0 \mu C + 0 \mu C = 0 \mu C.

Therefore, no charge flows through the switch when it is closed.