The series LRC circuit is an example of a damped, simple harmonic oscillator and the damping is accurately exponential. It is easy to apply a single-frequency sinusoidal voltage and to observe the response. The experimental set up is left out all through the course for the students to play with - and they do. They come back to test ideas related to superposition, and the difference in the charge and current responses, for example.
The hands-on experience with real electronic components and measuring devices cements the ideas. Students must physically select a sinusoidal voltage and measure its frequency, and carefully observe the frequency, amplitude and phase shift of the response (in our implementation, “response” is the current in the circuit with voltage across the resistor as proxy for the current). When asked beforehand, some students are not sure that the current will have the same frequency as the driving force. Most predict some sort of resonant response, but are unsure about magnitudes, how to measure and so on. Very few can predict or explain the phase shift, or easily relate the measured time shift to a radian shift.
This concrete example is a useful prompt many times in later discussions about harmonic systems: The instructor might ask, “Tell the class what happened in the LRC lab when you changed the frequency of the driving voltage?” Students may ask, “How does the response plot I made in the LRC lab translate to what we're doing in this pendulum example?” Remembering a physical activity is much easier than remembering a discussion.
We use this activity as a chance to for students to synthesize what they've learned in a coherent write up. There is a very clear distinction between the “measurements” and the “interpretation”, so the lab write-up can be broken into different sections, if necessary.