155264 An L-C-R series circuit with a resistance of $100 \Omega$ is connected to $200 \mathrm{~V}$ (AC source) and angular frequency $300 \mathrm{rad} / \mathrm{s}$. When only the capacitor is removed, then the current lags behind the voltage by $60^{\circ}$. When only the inductor is removed by the current leads the voltage by $60^{\circ}$. The average power dissipated in original $\mathbf{L}-\mathrm{C}-\mathrm{R}$ circuit is
155265 A series LCR circuit is connected across a sauce of alternating emf of changing frequency and resonates at frequency $f_{0}$. Keeping capacitance constant, if the inductance $(L)$ is increased by $\sqrt{3}$ times and resistance is increased $(R)$ by 1.4 times, the resonant frequency now is
155264 An L-C-R series circuit with a resistance of $100 \Omega$ is connected to $200 \mathrm{~V}$ (AC source) and angular frequency $300 \mathrm{rad} / \mathrm{s}$. When only the capacitor is removed, then the current lags behind the voltage by $60^{\circ}$. When only the inductor is removed by the current leads the voltage by $60^{\circ}$. The average power dissipated in original $\mathbf{L}-\mathrm{C}-\mathrm{R}$ circuit is
155265 A series LCR circuit is connected across a sauce of alternating emf of changing frequency and resonates at frequency $f_{0}$. Keeping capacitance constant, if the inductance $(L)$ is increased by $\sqrt{3}$ times and resistance is increased $(R)$ by 1.4 times, the resonant frequency now is
155264 An L-C-R series circuit with a resistance of $100 \Omega$ is connected to $200 \mathrm{~V}$ (AC source) and angular frequency $300 \mathrm{rad} / \mathrm{s}$. When only the capacitor is removed, then the current lags behind the voltage by $60^{\circ}$. When only the inductor is removed by the current leads the voltage by $60^{\circ}$. The average power dissipated in original $\mathbf{L}-\mathrm{C}-\mathrm{R}$ circuit is
155265 A series LCR circuit is connected across a sauce of alternating emf of changing frequency and resonates at frequency $f_{0}$. Keeping capacitance constant, if the inductance $(L)$ is increased by $\sqrt{3}$ times and resistance is increased $(R)$ by 1.4 times, the resonant frequency now is
155264 An L-C-R series circuit with a resistance of $100 \Omega$ is connected to $200 \mathrm{~V}$ (AC source) and angular frequency $300 \mathrm{rad} / \mathrm{s}$. When only the capacitor is removed, then the current lags behind the voltage by $60^{\circ}$. When only the inductor is removed by the current leads the voltage by $60^{\circ}$. The average power dissipated in original $\mathbf{L}-\mathrm{C}-\mathrm{R}$ circuit is
155265 A series LCR circuit is connected across a sauce of alternating emf of changing frequency and resonates at frequency $f_{0}$. Keeping capacitance constant, if the inductance $(L)$ is increased by $\sqrt{3}$ times and resistance is increased $(R)$ by 1.4 times, the resonant frequency now is
155264 An L-C-R series circuit with a resistance of $100 \Omega$ is connected to $200 \mathrm{~V}$ (AC source) and angular frequency $300 \mathrm{rad} / \mathrm{s}$. When only the capacitor is removed, then the current lags behind the voltage by $60^{\circ}$. When only the inductor is removed by the current leads the voltage by $60^{\circ}$. The average power dissipated in original $\mathbf{L}-\mathrm{C}-\mathrm{R}$ circuit is
155265 A series LCR circuit is connected across a sauce of alternating emf of changing frequency and resonates at frequency $f_{0}$. Keeping capacitance constant, if the inductance $(L)$ is increased by $\sqrt{3}$ times and resistance is increased $(R)$ by 1.4 times, the resonant frequency now is