Answer
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Hint: First find out the total impedance of an electric circuit containing all the three components that are resistor, capacitor and inductor. Then calculate the root mean square current by using the root mean square voltage which is the AC equivalent of the DC or the source voltage applied.
Complete step by step answer:
To get a better understanding of phase angle let us make a phasor diagram for an LCR circuit.
The angle $\varphi $ denotes the phase angle between voltage and current.
Now the total impedance of the circuit is given by
$Z = \sqrt {{R^2} + {{({X_L} - {X_C})}^2}} $
Where $R$ is the resistance of the circuit, ${X_L}$ is the inductive reactance and ${X_C}$ is the capacitive reactance.
Now the current is defined as
${I_{rms}} = \dfrac{{{V_{rms}}}}{Z}$
$\tan \varphi = \dfrac{{{X_L} - {X_C}}}{R}$ (from the phasor diagram)
$ \therefore \varphi = {\tan ^{ - 1}}\dfrac{{{X_L} - {X_C}}}{R}$
Which is the required phase angle.
Now for the second part of the question, we have three cases that need to be discussed.
Case 1: For an LCR circuit if ${X_L} > {X_C}$ , the current will be more inductive than capacitive and the current will lag behind the source voltage.
Case 2: For an LCR circuit if ${X_L} < {X_C}$ , the current will be more capacitive than inductive and the current will lead to the source voltage.
Case 3: For the LCR circuit if ${X_L} = {X_C}$ , then the circuit will resist and current and source voltage will be in the same phase.
Note: It is helpful to treat phase as if it is defined in a vector plane for simpler understanding. In a purely inductive circuit, the phase is positive while in a purely capacitive circuit the phase will be negative. In the case of a resistive circuit, the circuit is said to be in a resonant condition which has numerous circuit applications and the phase angle is zero.
Complete step by step answer:
To get a better understanding of phase angle let us make a phasor diagram for an LCR circuit.
The angle $\varphi $ denotes the phase angle between voltage and current.
Now the total impedance of the circuit is given by
$Z = \sqrt {{R^2} + {{({X_L} - {X_C})}^2}} $
Where $R$ is the resistance of the circuit, ${X_L}$ is the inductive reactance and ${X_C}$ is the capacitive reactance.
Now the current is defined as
${I_{rms}} = \dfrac{{{V_{rms}}}}{Z}$
$\tan \varphi = \dfrac{{{X_L} - {X_C}}}{R}$ (from the phasor diagram)
$ \therefore \varphi = {\tan ^{ - 1}}\dfrac{{{X_L} - {X_C}}}{R}$
Which is the required phase angle.
Now for the second part of the question, we have three cases that need to be discussed.
Case 1: For an LCR circuit if ${X_L} > {X_C}$ , the current will be more inductive than capacitive and the current will lag behind the source voltage.
Case 2: For an LCR circuit if ${X_L} < {X_C}$ , the current will be more capacitive than inductive and the current will lead to the source voltage.
Case 3: For the LCR circuit if ${X_L} = {X_C}$ , then the circuit will resist and current and source voltage will be in the same phase.
Note: It is helpful to treat phase as if it is defined in a vector plane for simpler understanding. In a purely inductive circuit, the phase is positive while in a purely capacitive circuit the phase will be negative. In the case of a resistive circuit, the circuit is said to be in a resonant condition which has numerous circuit applications and the phase angle is zero.
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