Capacitance and Potential Difference of Series Capacitors
We are given:
- Two capacitors \( X \) and \( Y \) connected in series to a battery of \( V = 6 \, \text{V} \).
- Same plate area \( A \) and separation \( d \).
- Capacitor \( X \) has air between plates, \( Y \) has dielectric of constant \( K = 4 \).
- Equivalent capacitance: \( C_\text{eq} = 4 \, \mu\text{F} \).
Step 1: Capacitance of Individual Capacitors
For a parallel plate capacitor:
\[
C = \frac{\varepsilon_0 \, K \, A}{d}
\]
- For capacitor \( X \) (air, \( K = 1 \)):
\[
C_X = \frac{\varepsilon_0 A}{d}
\]
- For capacitor \( Y \) (dielectric \( K = 4 \)):
\[
C_Y = \frac{4 \varepsilon_0 A}{d} = 4 C_X
\]
---
Step 2: Relation Between Series Capacitances
For capacitors in series:
\[
\frac{1}{C_\text{eq}} = \frac{1}{C_X} + \frac{1}{C_Y}
\]
Substitute \( C_Y = 4 C_X \):
\[
\frac{1}{4 \, \mu\text{F}} = \frac{1}{C_X} + \frac{1}{4 C_X} = \frac{1 + 0.25}{C_X} = \frac{1.25}{C_X}
\]
\[
C_X = 1.25 \times 4 \, \mu\text{F} = 5 \, \mu\text{F}
\]
\[
C_Y = 4 C_X = 4 \times 5 \, \mu\text{F} = 20 \, \mu\text{F}
\]
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Step 3: Potential Difference Across Each Capacitor
In series, charge \( Q \) on both capacitors is the same:
\[
Q = C_\text{eq} \, V = 4 \times 10^{-6} \times 6 = 24 \times 10^{-6} \, \text{C}
\]
Voltage across each capacitor:
\[
V_X = \frac{Q}{C_X} = \frac{24 \times 10^{-6}}{5 \times 10^{-6}} = 4.8 \, \text{V}
\]
\[
V_Y = \frac{Q}{C_Y} = \frac{24 \times 10^{-6}}{20 \times 10^{-6}} = 1.2 \, \text{V}
\]
Check: \( V_X + V_Y = 4.8 + 1.2 = 6 \, \text{V} \) ✔
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Step 4: Summary
- Capacitances: \( C_X = 5 \, \mu\text{F}, \quad C_Y = 20 \, \mu\text{F} \)
- Potential differences: \( V_X = 4.8 \, \text{V}, \quad V_Y = 1.2 \, \text{V} \)
Conclusion:
The series combination of capacitors with one dielectric results in a higher capacitance for the dielectric capacitor and a smaller potential drop across it, while the air capacitor takes a larger voltage share. This maintains the total voltage equal to the battery voltage.