Câu hỏi 17

 Đáp án B

Ta có:

\(I = \frac{{{E_0}}}{Z} = \frac{{\omega {\Phi _0}}}{{\sqrt {{R^2} + {{({Z_L} - {Z_C})}^2}} }} = \frac{{{\Phi _0}}}{{\sqrt {\frac{1}{{{C^2}{\omega ^4}}} - \frac{{\frac{{2L}}{C} - {R^2}}}{{{\omega ^2}}} + {L^2}} }} = \frac{{{\Phi _0}}}{{\sqrt y }}\)

I_Maxkhi y_min

\( \to \frac{1}{{{\omega _0}^2}} = \frac{{\frac{{2L}}{C} - {R^2}}}{{\frac{2}{{{C^2}}}}} = LC - \frac{{{R^2}{C^2}}}{2}\)

\(\begin{array}{l}{I_1} = {I_2} \to {y_1} = {y_2}\\ \to \frac{1}{{\omega _1^2}} + \frac{1}{{\omega _2^2}} = \frac{2}{{\omega _0^2}} \to \omega _0^2 = \frac{{2{\omega _1}{\omega _2}}}{{\omega _1^2 + \omega _2^2}}\end{array}\)

Vì \(\omega \)tỉ lệ thuận với n, ta suy ra:

\( \to n_0^2 = \frac{{2{n_1}{n_2}}}{{n_1^2 + n_2^2}}\)