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An LCR circuit has L=10 mH,R=150 Omega a...

An `LCR` circuit has `L=10 mH,R=150 Omega` and `C=1 muF` connacted in series to a source of `150sqrt2 cos omegat` volt. At a frequency that is `50%` of the resonant frequency.calculate the average power (in watt) dissipated per cycle.

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To solve the problem step by step, we will follow the outlined procedure to calculate the average power dissipated in the LCR circuit. ### Step 1: Calculate the Resonant Frequency The resonant frequency (\( \omega_0 \)) of the LCR circuit is given by the formula: \[ \omega_0 = \frac{1}{\sqrt{LC}} \] Given: - \( L = 10 \, \text{mH} = 10 \times 10^{-3} \, \text{H} \) - \( C = 1 \, \mu\text{F} = 1 \times 10^{-6} \, \text{F} \) Substituting the values: \[ \omega_0 = \frac{1}{\sqrt{(10 \times 10^{-3})(1 \times 10^{-6})}} = \frac{1}{\sqrt{10^{-8}}} = 10^4 \, \text{rad/s} \] ### Step 2: Calculate the Frequency at 50% of Resonant Frequency The frequency (\( \omega \)) at 50% of the resonant frequency is: \[ \omega = \frac{\omega_0}{2} = \frac{10^4}{2} = 5 \times 10^3 \, \text{rad/s} \] ### Step 3: Calculate the Impedance of the Circuit The impedance (\( Z \)) of the LCR circuit is given by: \[ Z = \sqrt{R^2 + \left( \omega L - \frac{1}{\omega C} \right)^2} \] Given: - \( R = 150 \, \Omega \) - \( L = 10 \times 10^{-3} \, \text{H} \) - \( C = 1 \times 10^{-6} \, \text{F} \) Calculating \( \omega L \) and \( \frac{1}{\omega C} \): \[ \omega L = (5 \times 10^3)(10 \times 10^{-3}) = 50 \, \text{V} \] \[ \frac{1}{\omega C} = \frac{1}{(5 \times 10^3)(1 \times 10^{-6})} = 200 \, \text{V} \] Now, substituting these values into the impedance formula: \[ Z = \sqrt{150^2 + (50 - 200)^2} = \sqrt{150^2 + (-150)^2} = \sqrt{22500 + 22500} = \sqrt{45000} = 150\sqrt{2} \, \Omega \] ### Step 4: Calculate the Average Power Dissipated The average power (\( P \)) dissipated in the circuit can be calculated using the formula: \[ P = \frac{V_{\text{rms}}^2}{R} \cdot \cos \phi \] Where \( \cos \phi = \frac{R}{Z} \). Given: - The source voltage is \( V(t) = 150\sqrt{2} \cos(\omega t) \), thus \( V_{\text{rms}} = 150 \, \text{V} \). Now, calculate \( \cos \phi \): \[ \cos \phi = \frac{R}{Z} = \frac{150}{150\sqrt{2}} = \frac{1}{\sqrt{2}} \] Substituting into the power formula: \[ P = \frac{(150)^2}{150} \cdot \frac{1}{\sqrt{2}} = 150 \cdot \frac{1}{\sqrt{2}} = \frac{150}{\sqrt{2}} = 75\sqrt{2} \, \text{W} \] ### Final Answer The average power dissipated per cycle is: \[ P \approx 75 \, \text{W} \]

To solve the problem step by step, we will follow the outlined procedure to calculate the average power dissipated in the LCR circuit. ### Step 1: Calculate the Resonant Frequency The resonant frequency (\( \omega_0 \)) of the LCR circuit is given by the formula: \[ \omega_0 = \frac{1}{\sqrt{LC}} \] ...
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