When a voltage is applied to a series R-C circuit, the charge q across C rises asymptotically to and the current i decays from its initial value towards zero. The rise of q and the fall of i both involve the same exponential function of time.
The value is called the ``time constant'' of the circuit.
Connect the square wave generator, which alternatively places a fixed voltage and a short circuit across a series RC circuit for equal time intervals, as shown in Fig. 9.4. The rise and decay of i can then be observed by using the oscilloscope to measure the voltage across R as a function of time. [The oscilloscope measures V(t); therefore i(t)=V(t)/R.] Be sure to connect your circuit so that the square wave generator and the oscillator share a common ground.
Figure 9.4: - Square wave generator to measure RC time constant.
Adjust the period of the square wave generator to allow several time constants between consecutive ``switching'' and adjust the sweep time of the oscilloscope to observe the rise and decay of the current.
Measure by determining the time it takes the current to fall to 1/e of its initial value.
The variation of the charge on the capacitor may be observed by using the oscilloscope to measure the voltage across C:
Reconnect your circuit, again making sure that the square wave generator and the oscilloscope share a common ground.
The value of will depend on the internal resistance of the square wave generator as well as the external resistor used: . The internal resistance can be measured in the following way: