Home
Class 12
PHYSICS
A wire of reistance R is connected in ...

A wire of reistance R is connected in series with an inductor of reactance `omega` L. Then quality factor of `RL` circuit is

A

`(R)/(omegaL)`

B

`(omegaL)/(R)`

C

`(R)/(sqrt(R^(2)+omega^(2)L^(2)))`

D

`(omegaL)/(sqrt(R^(2)+omega^(2)L^(2)))`

Text Solution

AI Generated Solution

The correct Answer is:
To find the quality factor (Q) of an RL circuit consisting of a resistor (R) and an inductor (L) in series, we can follow these steps: ### Step-by-Step Solution: 1. **Understand the Components**: We have a resistor with resistance \( R \) and an inductor with inductive reactance \( X_L \). The inductive reactance is given by the formula: \[ X_L = \omega L \] where \( \omega \) is the angular frequency and \( L \) is the inductance. 2. **Define the Quality Factor**: The quality factor \( Q \) for an RL circuit is defined as the ratio of the voltage across the inductor \( V_L \) to the voltage across the resistor \( V_R \): \[ Q = \frac{V_L}{V_R} \] 3. **Relate Voltages to Current**: The voltage across the inductor \( V_L \) can be expressed as: \[ V_L = I \cdot X_L \] and the voltage across the resistor \( V_R \) can be expressed as: \[ V_R = I \cdot R \] where \( I \) is the current flowing through the circuit. 4. **Substitute the Expressions**: Now, substituting these expressions into the quality factor formula gives: \[ Q = \frac{I \cdot X_L}{I \cdot R} \] 5. **Cancel Out Current**: Since the current \( I \) is the same through both components in a series circuit, we can cancel \( I \) from the numerator and denominator: \[ Q = \frac{X_L}{R} \] 6. **Substitute for Inductive Reactance**: Now, substitute \( X_L = \omega L \) into the equation: \[ Q = \frac{\omega L}{R} \] 7. **Final Expression**: Therefore, the quality factor \( Q \) for the RL circuit is: \[ Q = \frac{\omega L}{R} \] ### Conclusion: The quality factor of the RL circuit is given by: \[ Q = \frac{\omega L}{R} \]
Promotional Banner

Similar Questions

Explore conceptually related problems

In an AC circuit, a resistance of Rohm is connected in series with an inductance L . If phase angle between volage and current be 45^(@) , the value of inductive reactance will be

An inductor of inductance L and ressistor of resistance R are joined in series and connected by a source of frequency omega . Power dissipated in the circuit is

In an AC circuit, a resistance of Rohm is connected is series with an inductance L . If phase angle between volage and current be 45^(@) , the value of inductive reactance will be

A coil of inductive reactance 31 Omega has a resistance of 8 Omega . It is placed in series with a condenser of capacitive reactance 25 Omega . The combination is connected to an ac source of 110 V . The power factor of the circuit is

A coil of inductive reactance 31 Omega has a resistance of 8 ohm . It is placed in series with a condenser of capacitive reactance 25 Omega . The combination is connected to an ac source of 110 V . The power factor of the circuit is

A coil of inductive reactance 31 Omega has a resistance of 8 ohm . It is placed in series with a condenser of capacitive reactance 25 Omega . The combination is connected to an ac source of 110 V . The power factor of the circuit is

The impedance of a circuit consister of 3Omega resistance and 4Omega reactance. The power factor of the circuit is

An inductance of 1 mH a condenser of 10 mu F and a resistance of 50 Omega are connected in series. The reactances of inductor and condensers are same. The reactance of either of them will be

A 100 Omega resistasnce is connected in series with a 4 H inductor. The voltage across the resistor is V_R=(2.0V)sin(10^3 rad//s)t : (a) Find the expession of circuit current (b) Find the inductive reactance (c) derive an expression for the voltage across the inductor,

A 100 Omega resistasnce is connected in series with a 4 H inductor. The voltage across the resistor is V_R=(2.0V)sin(10^3 rad//s)t : (a) Find the expession of circuit current (b) Find the inductive reactance (c) derive an expression for the voltage across the inductor,