Read through the course notes before watching the video. The course note files may also contain links to associated animations or interactive simulations.
Read through the class slides. They explain all of the concepts from the module.
Do the Concept Questions first to make sure you understand the main concepts from this module. Then, when you are ready, try the Challenge Problems.
Watch the Problem Solving Help videos for insights on how to approach and solve problems related to the concepts in this module.
A circuit consists of a generator with frequency ω, a resistor with resistance R, a capacitor with capacitance C, and an inductor with an inductance L. Why does the circuit end up oscillating at the frequency of the driving electromotive force? Give an expression for the amplitude of the driven current in the circuit. Plot this current as a function of our driving frequency ω. At what frequency does it maximize, and what is the maximum current? How does the shape of this curve depend on the resistance in the circuit? What is the phase difference between the current and the driving electromotive force? In what frequency regime does the capacitor play the primary role, and in what frequency range does the inductor play the primary role?
A driven RLC circuit has a resistance of 300 Ohms, an inductance of 0.25 Henries, and a capacitance of 8 x 10-6 Farads. It is driven by a 120 V power supply at an angular frequency ω=400 radians/sec. Find the current in the circuit, the voltage you would read when you put voltmeters across the resistor, the capacitor, and the inductor, and the lead or lag of the current with respect to the driving voltage. Make sure you specify whether the current leads or lags the voltage. Is this circuit dominated by the capacitor or the inductor, or neither one?
A driven RLC circuit has a total impedance Z of 150 Ohms. The root mean square voltage of the generator is 160 Volts, and the resistance in the circuit is 110 Ohms. What is the mean power delivered to the circuit in Watts?
A driven RLC circuit is driven at its resonant frequency by a generator with an amplitude of 90 Volts. The capacitance is 2.5 x 10-6 Farads, the inductance is 0.90 Henries, and the resistance is 400 Ohms. At resonance, we have ωL = 1/ωC = 600 Ohms. What is the root mean square voltage measured individually across the capacitor and the inductor? If we put a voltmeter across both the capacitor and the inductor together, what root mean square voltage will we read?
In a driven RLC circuit, suppose you put a voltmeter across the combination of the resistance and the inductor. What is the ratio of the voltage read across that the RL combination to the generator source voltage?
The tuning RLC circuit in an FM radio has an inductance of 1 x 10-6 Henries, but we do not know the resistance or the capacitance. We vary the capacitance to tune into one FM station which broadcasts at an angular frequency ω = 6 x 108 radians per second. What is the value of the capacitance when we are receiving this station? There is an annoying nearby station which radiates at a frequency ω = 5.99 x 108 radians per second, but our tuning is so sharp that the power across the resistor due to this second station is only 1% of the power of the station we want to hear at ω = 6 x 108 radians per second. What is the resistance of the circuit?
Suppose instead of the usual arrangement of a series RLC circuit, we have all of the elements (power source, capacitor, inductor, resistor) in parallel instead of in series. How does this differ from our usual series RLC circuit? What is the expression for the total current flowing in the circuit in terms of R, L, C, and the driving amplitude of the power source Vs? If R is fixed, when is the current a maximum? Suppose R, L, and C are all fixed, is there a value of ω where the current is a maximum?