Experiment 9: Time and Capacitors
72 Chapter 2
theory
The time constant (continued)
The cake eater will always have a few crumbs to eat, be-
cause he never takes 100% of the remainder. Likewise, the
capacitor will never acquire a full charge. In a perfect world
of perfect components, this process would continue for an
infinite time.
In the real world, we say rather arbitrarily:
After 5 × TC the capacitor will be so nearly fully
charged, we won’t care about the difference.
In the table is a calculation (rounded to two decimal places)
showing the charge accumulating on a capacitor in a 12-
volt circuit where the time constant is 1 second.
Here’s how to understand the table. V1 is the current charge
on the capacitor. Subtract this from the supply voltage (12
volts) to find the difference. Call the result V2. Now take 63%
of V2, and add this to the current charge (V1) and call the
result V4. This is the new charge that the capacitor will have
after 1 second, so we copy it down to the next line in the
table, and it becomes the new value for V1.
Now we repeat the same process all over again. Figure 2-82
shows this in graphical form. Note that after 5 seconds,
the capacitor has acquired 11.92 volts, which is 99% of
the power supply voltage. This should be close enough to
satisfy anyone’s real-world requirements.
Time
in secs
V1:
Charge on capacitor
V2:
12 – V1
V3:
63% of V2
V4:
V1 + V3
0 0.00 12.00 7.56 7.56
1 7.56 4.44 2.80 10.36
2 10.36 1.64 1.03 11.39
3 11.39 0.61 0.38 11.77
4 11.77 0.23 0.15 11.92
5 11.92
If you try to verify these numbers by measuring the voltage
across the capacitor as it charges, remember that because
your meter steals a little current, there will be a small
discrepancy that will increase as time passes. For practical
purposes, the system works well enough.
TC TC TC TC
(^01)
2
3
+63%
+63%
+63%
Figure 2-82. A capacitor starts with 0 volts. After 1 time con-
stant it adds 63% of the available voltage. After another time
constant, it adds another 63% of the remaining voltage differ-
ence, and so on.