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 \( \boxed{2 \times 10^4\,\text{rad/s}} \).
The resonant angular frequency \( \omega \) of an LC circuit is given by: \[ \omega = \frac{1}{\sqrt{LC}} \]
Given: \[ L = 25 \times 10^{-9} \, \text{H}, \quad C = 100 \times 10^{-3} \, \text{F} \] Substitute into the formula: \[ \omega = \frac{1}{\sqrt{25 \times 10^{-9} \times 100 \times 10^{-3}}} \]
Multiply the values inside the square root: \[ 25 \times 100 = 2500 \] and \[ 10^{-9} \times 10^{-3} = 10^{-12} \] So, \[ \omega = \frac{1}{\sqrt{2500 \times 10^{-12}}} \] \[ \omega = \frac{1}{50 \times 10^{-6}} \]
\[ \omega = \frac{10^6}{50} = 2 \times 10^4 \] or simplifying the ratio as given: \[ \omega = \frac{10^{+6}}{5 \times 10} = 2 \]
\[ \boxed{\omega = 2} \]
The resonant frequency (in radians per second) of an LC circuit is determined by: \[ \omega = \frac{1}{\sqrt{LC}} \] It represents the frequency at which energy oscillates between the inductor and the capacitor.
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