155226 In a series $L C R$ circuit the frequency of a $10 \mathrm{~V}$ AC voltage source is adjusted in such a fashion that the reactance of the inductor measure $15 \Omega$ and that of capacitor $11 \Omega$. If $R=3 \Omega$, the potential difference across the series combination of $L$ and $C$ will be :

155227 An LCR circuit of $R=100 \Omega$ is connected to an AC source $100 \mathrm{~V}, 50 \mathrm{~Hz}$. The magnitude of phase difference between current and voltage is $3^{\circ}$. The power dissipated in the LCR circuit is :

155228 In $L-R$ circuit, resistance is $8 \Omega$ and inductive reactance is $6 \Omega$, then impedance is :

155229 The LC parallel resonant circuit

155230 If the inductance and capacitance are both doubled in L-C-R circuit, the resonant frequency of the circuit will

155226 In a series $L C R$ circuit the frequency of a $10 \mathrm{~V}$ AC voltage source is adjusted in such a fashion that the reactance of the inductor measure $15 \Omega$ and that of capacitor $11 \Omega$. If $R=3 \Omega$, the potential difference across the series combination of $L$ and $C$ will be :

155227 An LCR circuit of $R=100 \Omega$ is connected to an AC source $100 \mathrm{~V}, 50 \mathrm{~Hz}$. The magnitude of phase difference between current and voltage is $3^{\circ}$. The power dissipated in the LCR circuit is :

155228 In $L-R$ circuit, resistance is $8 \Omega$ and inductive reactance is $6 \Omega$, then impedance is :

155229 The LC parallel resonant circuit

155230 If the inductance and capacitance are both doubled in L-C-R circuit, the resonant frequency of the circuit will

155226 In a series $L C R$ circuit the frequency of a $10 \mathrm{~V}$ AC voltage source is adjusted in such a fashion that the reactance of the inductor measure $15 \Omega$ and that of capacitor $11 \Omega$. If $R=3 \Omega$, the potential difference across the series combination of $L$ and $C$ will be :

155227 An LCR circuit of $R=100 \Omega$ is connected to an AC source $100 \mathrm{~V}, 50 \mathrm{~Hz}$. The magnitude of phase difference between current and voltage is $3^{\circ}$. The power dissipated in the LCR circuit is :

155228 In $L-R$ circuit, resistance is $8 \Omega$ and inductive reactance is $6 \Omega$, then impedance is :

155229 The LC parallel resonant circuit

155230 If the inductance and capacitance are both doubled in L-C-R circuit, the resonant frequency of the circuit will

155226 In a series $L C R$ circuit the frequency of a $10 \mathrm{~V}$ AC voltage source is adjusted in such a fashion that the reactance of the inductor measure $15 \Omega$ and that of capacitor $11 \Omega$. If $R=3 \Omega$, the potential difference across the series combination of $L$ and $C$ will be :

155227 An LCR circuit of $R=100 \Omega$ is connected to an AC source $100 \mathrm{~V}, 50 \mathrm{~Hz}$. The magnitude of phase difference between current and voltage is $3^{\circ}$. The power dissipated in the LCR circuit is :

155228 In $L-R$ circuit, resistance is $8 \Omega$ and inductive reactance is $6 \Omega$, then impedance is :

155229 The LC parallel resonant circuit

155230 If the inductance and capacitance are both doubled in L-C-R circuit, the resonant frequency of the circuit will

155226 In a series $L C R$ circuit the frequency of a $10 \mathrm{~V}$ AC voltage source is adjusted in such a fashion that the reactance of the inductor measure $15 \Omega$ and that of capacitor $11 \Omega$. If $R=3 \Omega$, the potential difference across the series combination of $L$ and $C$ will be :

155227 An LCR circuit of $R=100 \Omega$ is connected to an AC source $100 \mathrm{~V}, 50 \mathrm{~Hz}$. The magnitude of phase difference between current and voltage is $3^{\circ}$. The power dissipated in the LCR circuit is :

155228 In $L-R$ circuit, resistance is $8 \Omega$ and inductive reactance is $6 \Omega$, then impedance is :

155229 The LC parallel resonant circuit

155230 If the inductance and capacitance are both doubled in L-C-R circuit, the resonant frequency of the circuit will