To keep the resonance frequency \(\omega\) unchanged, we know:
\[ \omega' = \omega = \frac{1}{\sqrt{L'C'}} \]
Given:
\[ L'C' = LC \]
Substituting \(C' = 4C\) into the equation:
\[ L' \cdot (4C) = LC \implies L' = \frac{L}{4} \]
Thus, the inductance must be decreased by:
\[ L - L' = L - \frac{L}{4} = \frac{3L}{4} \]
A | B | Y |
0 | 0 | 1 |
0 | 1 | 0 |
1 | 0 | 1 |
1 | 1 | 0 |