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What is the impedance of a series RLC circuit when the frequency of time- varying emf is set to the resonant frequency of the circuit?

Short Answer

Expert verified
Answer: At the resonant frequency, the impedance of a series RLC circuit is equal to the resistance R.

Step by step solution

01

Recall the formula for resonant frequency

For a series RLC circuit, the resonant frequency is given by the formula: \[ f_r = \frac{1}{2 \pi \sqrt{LC}} \] where L is the inductance, C is the capacitance, and \(f_r\) is the resonant frequency.
02

Recall the formula for the impedance

The impedance of a series RLC circuit is given by the formula: \[ Z = \sqrt{R^2 + (\omega L - \frac{1}{\omega C})^2} \] where R is the resistance, L is the inductance, C is the capacitance, \(\omega\) is the angular frequency, and Z is the impedance.
03

Calculate the angular frequency at resonance

At resonance, the angular frequency of the time-varying emf is equal to the angular frequency of the resonant frequency. We can use the following relationship between angular frequency and frequency: \[ \omega = 2 \pi f \] Since we know the resonant frequency, we can plug it in to calculate the angular frequency at resonance: \[ \omega_r = 2 \pi f_r \]
04

Calculate the impedance at resonance

Now, we can find the impedance at the resonant frequency by plugging in the values of R, L, and C and the angular frequency at resonance into the impedance formula: \[ Z_r = \sqrt{R^2 + (\omega_r L - \frac{1}{\omega_r C})^2} \] At resonance, the reactive parts of the impedance, the inductive reactance, and the capacitive reactance are equal and thus cancel each other out. Therefore, the impedance formula simplifies to: \[ Z_r = \sqrt{R^2 + (0)^2} = R \] So, the impedance of the series RLC circuit at the resonant frequency is equal to the resistance R.

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Most popular questions from this chapter

An inductor with inductance \(L=52.5 \mathrm{mH}\) is connected to an \(\mathrm{AC}\) power source that supplies \(V_{\mathrm{emf}}=19.9 \mathrm{~V}\) at \(f=669 \mathrm{~Hz}\). Find the maximum current in the circuit.

A series RLC circuit is in resonance when driven by a sinusoidal voltage at its resonant frequency, \(\omega_{0}=(L C)^{-1 / 2} .\) But if the same circuit is driven by a square-wave voltage (which is alternately on and off for equal time intervals), it will exhibit resonance at its resonant frequency and at \(\frac{1}{3}\), \(\frac{1}{5}, \frac{1}{7}, \ldots,\) of this frequency. Explain why.

An LC circuit consists of a capacitor, \(C=2.50 \mu \mathrm{F},\) and an inductor, \(L=4.00 \mathrm{mH} .\) The capacitor is fully charged using a battery and then connected to the inductor. An oscilloscope is used to measure the frequency of the oscillations in the circuit. Next, the circuit is opened, and a resistor, \(R\), is inserted in series with the inductor and the capacitor. The capacitor is again fully charged using the same battery and then connected to the circuit. The angular frequency of the damped oscillations in the RLC circuit is found to be \(20.0 \%\) less than the angular frequency of the oscillations in the LC circuit. a) Determine the resistance of the resistor. b) How long after the capacitor is reconnected in the circuit will the amplitude of the damped current through the circuit be \(50.0 \%\) of the initial amplitude? c) How many complete damped oscillations will have occurred in that time?

Why can't a transformer be used to step up or step down the voltage in a DC circuit?

For which values of \(f\) is \(X_{L}>X_{C} ?\) a) \(f>2 \pi(L C)^{1 / 2}\) b) \(f>(2 \pi L C)^{-1}\) c) \(f>\left(2 \pi(L C)^{1 / 2}\right)^{-1}\) d) \(f>2 \pi L C\)

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