The resonance frequency \(\omega\) remains constant, implying:
\[ \omega' = \omega = \frac{1}{\sqrt{L'C'}} \]
It is provided that:
\[ L'C' = LC \]
Substituting \(C' = 4C\) yields:
\[ L' \cdot (4C) = LC \implies L' = \frac{L}{4} \]
Therefore, the inductance change required is:
\[ L - L' = L - \frac{L}{4} = \frac{3L}{4} \]
| A | B | Y |
| 0 | 0 | 1 |
| 0 | 1 | 0 |
| 1 | 0 | 1 |
| 1 | 1 | 0 |
