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The Middle Wire Splits the Series Pair

Irodov 3.123DifficultyDifficulty 2 of 5UniquenessUniqueness 2 of 5

Problem Irodov 3.123

Two batteries, each of emf E=60\mathcal{E} = 60 V, are connected in series in a left vertical branch, both with the positive terminal upward. A right vertical branch holds two capacitors in series, C1=2.0C_1 = 2.0 μ\muF above and C2=3.0C_2 = 3.0 μ\muF below. The top wire (section 11) joins the tops of the two branches and the bottom wire (section 22) joins their bottoms. A middle wire runs from the junction between the batteries, through an open switch SwSw and then along section 33, to the junction between the capacitors. The switch is now closed. Find the charges that flow through sections 11, 22 and 33, each counted positive when it flows from the battery side toward the capacitor side.

The circuit with the switch open. Both batteries have the long (+) plate up; the arrows give the positive senses for the charges through sections 1, 2 and 3.

The circuit with the switch open. Both batteries have the long (++) plate up; the arrows give the positive senses for the charges through sections 11, 22 and 33.

Given
  • E=60\mathcal{E} = 60 V (each battery)
  • C1=2.0 μC_1 = 2.0~\muF
  • C2=3.0 μC_2 = 3.0~\muF
  • SwSw open, then closed
  • capacitors uncharged before the circuit was assembled (assumed)
Find
q1q_1, q2q_2, q3q_3, in the senses of the arrows

Solution

Step 1The charges with the switch open

With the switch open the middle wire carries nothing, so C1C_1 and C2C_2 are in series across the two batteries, 2E2\mathcal{E} in all. The junction between them, with the two plates on it, is isolated and neutral (the capacitors are assumed uncharged to begin with), so both capacitors carry the same charge:

q0=C1C2C1+C2⋅2E(1) q_0 = \frac{C_1C_2}{C_1 + C_2}\cdot 2\mathcal{E} \tag{1}

The upper plate of C1C_1, on the positive top wire, carries +q0+q_0; the lower plate of C2C_2 carries −q0-q_0; the two plates on the middle junction carry −q0-q_0 and +q0+q_0.

Step 2The charges with the switch closed

Closing the switch ties the junction between the capacitors to the junction between the batteries. Each capacitor then sits across one battery:

qC1′=C1E,qC2′=C2E(2) q_{C_1}' = C_1\mathcal{E}, \qquad q_{C_2}' = C_2\mathcal{E} \tag{2}

The upper plate of C1C_1 carries +C1E+C_1\mathcal{E}, the lower plate of C2C_2 carries −C2E-C_2\mathcal{E}, and the middle junction holds −C1E+C2E-C_1\mathcal{E} + C_2\mathcal{E} on its two plates.

Step 3Charge through each section

Subtracting the plate charges ±q0\pm q_0 of (1) from those of (2):

q1=C1E−2EC1C2C1+C2=EC1(C1+C2−2C2)C1+C2q2=−C2E−(−2EC1C2C1+C2)=EC2(2C1−C1−C2)C1+C2q3=(C2−C1)E−(q0−q0)\begin{aligned} q_1 &= C_1\mathcal{E} - \frac{2\mathcal{E}C_1C_2}{C_1 + C_2} = \frac{\mathcal{E}C_1(C_1 + C_2 - 2C_2)}{C_1 + C_2}\\[2pt] q_2 &= -C_2\mathcal{E} - \left(-\frac{2\mathcal{E}C_1C_2}{C_1 + C_2}\right) = \frac{\mathcal{E}C_2(2C_1 - C_1 - C_2)}{C_1 + C_2}\\[2pt] q_3 &= (C_2 - C_1)\mathcal{E} - (q_0 - q_0) \end{aligned}

With C1+C2=5.0 μC_1 + C_2 = 5.0~\muF and C1−C2=−1.0 μC_1 - C_2 = -1.0~\muF, numerically:

q1=60×2.0×(−1.0)5.0 μCq2=60×3.0×(−1.0)5.0 μCq3=60×(3.0−2.0) μC\begin{aligned} q_1 &= \frac{60 \times 2.0 \times (-1.0)}{5.0}~\mu\text{C}\\[2pt] q_2 &= \frac{60 \times 3.0 \times (-1.0)}{5.0}~\mu\text{C}\\[2pt] q_3 &= 60 \times (3.0 - 2.0)~\mu\text{C} \end{aligned}
q1=EC1(C1−C2)C1+C2=−24 μCq2=EC2(C1−C2)C1+C2=−36 μCq3=E(C2−C1)=+60 μC\begin{gathered} q_1 = \frac{\mathcal{E}C_1(C_1 - C_2)}{C_1 + C_2} = -24~\mu\text{C}\\[2pt] q_2 = \frac{\mathcal{E}C_2(C_1 - C_2)}{C_1 + C_2} = -36~\mu\text{C}\\[2pt] q_3 = \mathcal{E}(C_2 - C_1) = +60~\mu\text{C} \end{gathered}
(3)

So 24 μ24~\muC flows back along section 11 and 36 μ36~\muC back along section 22, while 60 μ60~\muC flows along the arrow of section 33.

Check

The three sections together carry everything that reaches the capacitor plates, and the total charge on all four plates is zero before and after, so the three charges must add up to zero. Indeed

q1+q2+q3=E(C1−C2)(C1+C2)C1+C2+E(C2−C1)=0q_1 + q_2 + q_3 = \frac{\mathcal{E}(C_1 - C_2)(C_1 + C_2)}{C_1 + C_2} + \mathcal{E}(C_2 - C_1) = 0

and in numbers −24−36+60=0-24 - 36 + 60 = 0. For equal capacitors the series pair already splits the 2E2\mathcal{E} evenly, so closing the switch changes nothing, and all three charges vanish.

Remark

The middle wire lets each capacitor take the voltage of its own battery instead of sharing 2E2\mathcal{E} in proportion to 1/C1/C. With the switch open the smaller capacitor C1C_1 held 72 V, more than its battery’s 60 V, so it gives charge back through section 11; the larger C2C_2 held only 48 V and charges further, fed through section 33 at its upper plate while positive charge drains back along section 22 from its lower one.