Question

Difficulty: Very hardCapacitors and Capacitance

A parallel-plate capacitor with air between its plates has a capacitance of 12 μF12\text{ }\mu\text{F}. A dielectric slab of relative permittivity εr=4\varepsilon_r = 4 and thickness t=d3t = \frac{d}{3}, where dd is the total plate separation, is inserted between the plates parallel to them. What is the effective capacitance of the modified capacitor?

  1. 16 μF16\text{ }\mu\text{F}Answer
  2. B
    48 μF48\text{ }\mu\text{F}
  3. C
    162 μF162\text{ }\mu\text{F}
  4. D
    6 μF6\text{ }\mu\text{F}

Answer

The effective capacitance of the modified capacitor is 16 μF16\text{ }\mu\text{F}.
Inserting a dielectric slab of thickness t=d/3t = d/3 creates a system equivalent to two series capacitors: an air-filled region of thickness 2d/32d/3 (C1=1.5C0=18 μFC_1 = 1.5 C_0 = 18\text{ }\mu\text{F}) and a dielectric-filled region of thickness d/3d/3 (C2=12C0=144 μFC_2 = 12 C_0 = 144\text{ }\mu\text{F}). Combining them via the series reciprocal formula gives Ceq=18×14418+144=16 μFC_{\text{eq}} = \frac{18 \times 144}{18 + 144} = 16\text{ }\mu\text{F}.

Step-by-Step Solution

1
Model the partially filled capacitor as two capacitors connected in series.
Air layer of thickness d1=dt=23dd_1 = d - t = \frac{2}{3}d forms capacitor C1C_1. Dielectric layer of thickness d2=t=13dd_2 = t = \frac{1}{3}d forms capacitor C2C_2.
Dividing the plate gap vertically into two distinct media creates two capacitive regions sharing the same electric flux path.
2
Calculate the individual capacitances C1C_1 and C2C_2 in terms of initial air capacitance C0=12 μFC_0 = 12\text{ }\mu\text{F}.
C1=ε0A23d=32C0=32(12)=18 μFC_1 = \frac{\varepsilon_0 A}{\frac{2}{3}d} = \frac{3}{2}C_0 = \frac{3}{2}(12) = 18\text{ }\mu\text{F} and C2=εrε0A13d=3εrC0=3(4)(12)=144 μFC_2 = \frac{\varepsilon_r \varepsilon_0 A}{\frac{1}{3}d} = 3 \varepsilon_r C_0 = 3(4)(12) = 144\text{ }\mu\text{F}.
Capacitance is inversely proportional to plate distance and directly proportional to relative permittivity.
3
Calculate the equivalent capacitance CeqC_{\text{eq}} for two series capacitors.
1Ceq=1C1+1C2=118+1144=8+1144=9144=116 μF1    Ceq=16 μF\frac{1}{C_{\text{eq}}} = \frac{1}{C_1} + \frac{1}{C_2} = \frac{1}{18} + \frac{1}{144} = \frac{8 + 1}{144} = \frac{9}{144} = \frac{1}{16}\text{ }\mu\text{F}^{-1} \implies C_{\text{eq}} = 16\text{ }\mu\text{F}.
Capacitors connected in series combine reciprocally.

Key Concept

Partially filled parallel-plate capacitors act as series combinations of distinct capacitive layers.
Estimated Time:3m 0s
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