
This problem concerns calculating the capacitance of a capacitor with a stepped geometry. The solution proceeds through a systematic analysis.
A flat plate of area \( A \) is paired with a stepped plate. The stepped structure comprises three sections, each possessing an area of \( \frac{A}{3} \) and a height of \( d \).
The fundamental formula for the capacitance \( C \) of a parallel-plate capacitor is:
\(C = \frac{\varepsilon_0 A}{d}\)
Here, \( \varepsilon_0 \) represents the permittivity of free space, \( A \) is the area of one plate, and \( d \) denotes the separation distance between the plates.
Each step of the structure acts as an individual capacitor connected in parallel with the others. The respective areas and separation distances are as follows:
The capacitance contributed by each step is inversely proportional to its separation distance:
Individual capacitances for each step:
As these capacitors are in parallel, the total capacitance \( C_{\text{total}} \) is the arithmetic sum of their individual capacitances:
\(C_{\text{total}} = C_1 + C_2 + C_3\\)
Substituting the calculated values:
\(C_{\text{total}} = \frac{\varepsilon_0 A}{3d} + \frac{\varepsilon_0 A}{6d} + \frac{\varepsilon_0 A}{9d}\)
To sum these fractions, a common denominator is employed:
\(C_{\text{total}} = \frac{6 \varepsilon_0 A}{18d} + \frac{3 \varepsilon_0 A}{18d} + \frac{2 \varepsilon_0 A}{18d}\)
\(C_{\text{total}} = \frac{(6+3+2) \varepsilon_0 A}{18d} = \frac{11 \varepsilon_0 A}{18d}\)
The calculated capacitance for the described configuration is \(\frac{11 \varepsilon_0 A}{18 d}\).