Step 1: Use the resonance condition for an LCR circuit
For maximum current in a series LCR circuit, resonance must occur. At resonance, the angular frequency \( \omega_0 \) is given by: \[ \omega_0 = \frac{1}{\sqrt{LC}} \]
Step 2: Convert all quantities to SI units
Step 3: Substitute values into the resonance formula
\[ \omega_0 = \frac{1}{\sqrt{LC}} = \frac{1}{\sqrt{0.1 \times 2.5 \times 10^{-8}}} \] \[ = \frac{1}{\sqrt{2.5 \times 10^{-9}}} \]
Step 4: Simplify the square root
\[ \sqrt{2.5 \times 10^{-9}} = \sqrt{2.5} \times \sqrt{10^{-9}} = 1.58 \times 10^{-4.5} \]
Step 5: Calculate the final value of \( \omega_0 \)
\[ \omega_0 = \frac{1}{1.58 \times 10^{-4.5}} = \frac{1}{1.58 \times 3.16 \times 10^{-5}} \approx \frac{1}{5 \times 10^{-5}} = 2 \times 10^4\,\text{rad/s} \]
Final Answer: The angular frequency at resonance is \( \boxed{2 \times 10^4\,\text{rad/s}} \).
In a resonance tube closed at one end. Resonance is obtained at lengths \( l_1 = 120 \, \text{cm} \) and \( l_2 = 200 \, \text{cm} \). If \( v_s = 340 \, \text{m/s} \), find the frequency of sound.
Relative stability of the contributing structures is :
Let A be a 3 × 3 matrix such that \(\text{det}(A) = 5\). If \(\text{det}(3 \, \text{adj}(2A)) = 2^{\alpha \cdot 3^{\beta} \cdot 5^{\gamma}}\), then \( (\alpha + \beta + \gamma) \) is equal to:
Let \( \alpha, \beta \) be the roots of the equation \( x^2 - ax - b = 0 \) with \( \text{Im}(\alpha) < \text{Im}(\beta) \). Let \( P_n = \alpha^n - \beta^n \). If \[ P_3 = -5\sqrt{7}, \quad P_4 = -3\sqrt{7}, \quad P_5 = 11\sqrt{7}, \quad P_6 = 45\sqrt{7}, \] then \( |\alpha^4 + \beta^4| \) is equal to: