Concept:
Capacitive compensation is implemented in transmission lines to improve voltage profiles, reduce losses, and increase power transfer capacity.
* Shunt Capacitors: Connected in parallel across the line to supply reactive power ($Q_{\text{shunt}}$) locally, raising the voltage profile by minimizing lagging power factor currents.
* Series Capacitors: Connected in series with the line conductors to physically negate a portion of the line's series inductive reactance ($X_L$). This directly reduces the overall series voltage drop ($\Delta V = I \cdot X_c$).
Step 1: Formulate the mathematical expressions for reactive power capacity.
Let $\Delta V$ be the desired voltage boost required by the power network system.
For a series capacitor, the reactive power injected depends on the line current ($I$) flowing through it:
\[
Q_{\text{series}} = 3 \cdot I^2 \cdot X_{\text{series}}
\]
Since the voltage drop across the series capacitor is $\Delta V = I \cdot X_{\text{series}}$, we can substitute this expression to get:
\[
Q_{\text{series}} = 3 \cdot I \cdot \left(I \cdot X_{\text{series}}\right) = 3 \cdot I \cdot \Delta V
\]
For a shunt capacitor, the reactive power injected depends directly on the system operating line voltage ($V$):
\[
Q_{\text{shunt}} = 3 \cdot \frac{V^2}{X_{\text{shunt}}}
\]
The voltage boost provided by a shunt capacitor can be approximated using short-circuit dynamics as:
\[
\Delta V \approx \frac{Q_{\text{shunt}} \cdot X_L}{3 \cdot V} \implies Q_{\text{shunt}} = 3 \cdot V \cdot \Delta V \cdot \frac{1}{X_L}
\]
Step 2: Compare the capacities for identical voltage boost profiles.
Let's look at the basic equations for the reactive power capacities required to achieve the same voltage change $\Delta V$:
\[
\frac{Q_{\text{shunt}}}{Q_{\text{series}}} = \frac{3 \cdot V \cdot \Delta V \cdot \frac{1}{X_L}}{3 \cdot I \cdot \Delta V} = \frac{V}{I \cdot X_L} = \frac{1}{\left(\frac{I \cdot X_L}{V}\right)}
\]
The term $\frac{I \cdot X_L}{V}$ represents the percentage inductive voltage drop across the transmission line, which is typically a small fraction (e.g., $0.1$ to $0.2$) under normal operating conditions.
\[
\frac{I \cdot X_L}{V} \ll 1 \implies \frac{Q_{\text{shunt}}}{Q_{\text{series}}} \gg 1 \implies Q_{\text{shunt}} > Q_{\text{series}}
\]
This mathematically demonstrates that to achieve the exact same voltage boost, a shunt capacitor must have a much larger reactive power capacity than a series capacitor.
Thus, the capacity of the shunt capacitor is greater than that of the series capacitor, which aligns with Option (B).