In an LCR series circuit, an inductor 30 mH and a resistor 1 Ωar...
In an LCR series circuit, an inductor 30 mH and a resistor 1 Ω are connected in series with a capacitor. The circuit is powered by an AC voltage source.
The behavior of the circuit depends on the frequency of the AC voltage source. At low frequencies, the inductor dominates and the circuit behaves as an inductive circuit. At high frequencies, the capacitor dominates and the circuit behaves as a capacitive circuit.
At the resonant frequency, the inductive and capacitive reactances cancel each other out, resulting in a purely resistive circuit. This is the frequency at which the circuit has the maximum impedance.
The resonant frequency can be calculated using the formula:
fr = 1 / (2π√(LC))
Where fr is the resonant frequency, L is the inductance in henries, and C is the capacitance in farads.
In this circuit, the inductance is given as 30 mH, which is equal to 0.03 H. Let's assume the capacitance is C farads.
Using the formula, we can calculate the resonant frequency:
fr = 1 / (2π√(0.03C))
At the resonant frequency, the inductive and capacitive reactances are equal in magnitude but opposite in sign. Therefore, the impedance of the circuit is purely resistive and can be calculated using Ohm's Law:
Z = √(R^2 + (XL - XC)^2)
Where Z is the impedance, R is the resistance in ohms, XL is the inductive reactance in ohms, and XC is the capacitive reactance in ohms.
Since the resistance is given as 1 Ω, XL can be calculated using the formula:
XL = 2πfL
Where f is the frequency in hertz.
Similarly, XC can be calculated using the formula:
XC = 1 / (2πfC)
At the resonant frequency, XL and XC are equal in magnitude but opposite in sign, resulting in a purely resistive impedance.
In an LCR series circuit, an inductor 30 mH and a resistor 1 Ωar...
X
C - X
L = R
X = 3