In Figure 12-39, calculate the voltage across the capacitor every 0.1 ms for one complete period of the input.Then sketch the capacitor waveform. Assume the Thevenin resistance of the generator is negligible.
In Figure 12-39, calculate the voltage across the capacitor every 0.1 ms for one complete period of the input.Then sketch the capacitor waveform. Assume the Thevenin resistance of the generator is negligible.
The period of the square wave is 1 ms. which is approximately 12 \tau . This means that 6 \tau will elapse after each change of the pulse, allowing the capacitor to fully charge and fully discharge.
For the increasing exponential,
v=V_{F}(1- e^{-t/RC})= V_{F}(1-e^{-t/\tau })At 0.1 ms : v = 2.5 V( 1 – e^{-0.1ms/0.084ms}) = 1 .74 V
At 0.2 ms : v = 2.5 V( 1 – e^{-0.2ms/0.084ms}) = 2.27 V
At 0.3 ms : v = 2.5 V( 1 – e^{-0.3ms/0.084ms}) = 2.43 V
At 0.4 ms : v = 2.5 V( 1 – e^{-0.4ms/0.084ms}) = 2.48 V
At 0.5 ms : v = 2.5 V( 1 – e^{-0.5ms/0.084ms}) = 2.49 V
For the decreasing exponential.
v=V_{i}(e^{-t/RC})= V_{i}(e^{-t/\tau })In the equation, time is shown from the point when the change occurs (subtracting 0.5 ms from the actual time). For example, at 0.6 ms, t = 0.6 ms — 0.5 ms = 0.1 ms.
At 0.6 ms: v = 2.5 V(e^{-0.1ms/0.084ms}) = 0.76 V
At 0.7 ms: v = 2.5 V(e^{-0.2ms/0.084ms}) = 0.23 V
At 0.8 ms: v = 2.5 V(e^{-0.3ms/0.084ms}) = 0.07 V
At 0.9 ms: v = 2.5 V(e^{-0.4ms/0.084ms}) = 0.02 V
At 1.0 ms: v = 2.5 V(e^{-0.5ms/0.084ms}) = 0.01 V
Figure 12-40 is a plot of these results.