00:01
Here we're going to take a look at several types of what are called passive filters that use just a capacitor and resistor in them.
00:12
And a reminder that for oscillating voltage sources, the capacitor has a so -called reactants that depends on frequency and it goes as the inverse of the frequency times capacitance, both in the denominator.
00:33
So this reactants, which is in oms, gets smaller, the higher the frequency is.
00:43
And that may be used to do filtering on signals.
00:47
So the little circuit to the left, what will happen as the frequency gets higher and higher, is the capacitor will act more and more just like a wire.
00:59
And more and more of the input signal voltage will be, will, fall over the resistor and less of it over the capacitor.
01:11
So if you're looking at the voltage output across the resistor, that will get more and more as the frequency increases.
01:20
And so your graph of v -out versus frequency will basically be low to start off with and then it'll kind of curve over until you basically get the same thing.
01:36
As your input voltage falling across the resistor.
01:41
And there's kind of a little breakpoint.
01:42
We won't get into the technical details, but where the curve starts to bend over and flatten out, that has a specific value, the frequency of 1 over r1, c1.
01:58
Now, we could do something very similar, but switch the placement of the resistor and capacitor.
02:05
And what will happen in that case is as the frequency increases, there will, of course, be less and less voltage across the capacitor.
02:17
So that would be what's called a low -pass filter.
02:22
So lots of voltage output to begin with, and then we'll start to go down at a particular frequency.
02:35
And again, that is technically equal to one over the inverse.
02:40
Of r2c2.
02:43
So those are time constants related to time constants for each of the rc items in each circuit.
02:56
Now, what you can do with both of these is to put them into what's called a band pass filter...