R–L–C Series Resonant Circuit
Background information
“Resonance describes the oscillatory response of a system when it is excited by a frequency that matches or is close to the system’s natural frequency.”
The resonance frequency is given by:
$$f_{\rm r} = \frac{1}{2\pi \sqrt{LC}}\text{, or} ~~~ \omega_{\rm r} = \frac{1}{\sqrt{LC}}$$
At resonance, the current is given by:
$$I = \frac{U}{R}$$
Experimental Tasks
- The function generator shall be set to produce a sinusoidal signal, and the amplitude of the output voltage shall be 6 V. For the circuit shown above, the magnitude of the impedance is given by: $$Z = \sqrt{R^2 + (\omega L − \frac{1}{\omega C})^2}$$
As can be seen from figure 1, the inductive and capacitive voltage components partially cancel each other. There exists a specific frequency at which these components cancel completely, causing the circuit to behave as a purely resistive circuit. This frequency is known as the resonance frequency.
- Calculate the resonance frequency for the assembled measurement circuit.
(The capacitance of the capacitor is determined using a measuring instrument)
$f_{\rm r}~=~ ..........................................................$
- Adjust the frequency of the function generator so that the ratio $\frac{f}{f_{\rm r}}$ corresponds to the values listed in table 1.
- Measure the RMS voltage $U_{\rm R}$ using the oscilloscope and record the measured values in table 1.
- Plot the current as a function of the ratio $\frac{f}{f_{\rm r}}$ on a logarithmic scale.