Okay, now hopefully you're able to work out those two little problems that I just

gave you. And to wrap up this lecture, I just want

to try to increase your intuition a little bit for what's going on.

Now, these filters, these high pass and low pass filters that we've been talking

about. Are really nothing more than voltage

dividers that happen to be frequency dependent.

So, let's take a look, go back to our, old familiar voltage divider, where we

take a voltage. And we apply it to a string of, it use to

be just resisters, but now we are going to put 2 impedances and now use Z to

represent impedance. But we'll put 2 impedances in series and

then measure the voltage at the mid point.

And so, just like a voltage divider when this use to be a battery and 2 resisters

The voltage here is some fraction of the total voltage there.

Now I can replace Z1 with either a resister, inductor, or capacitor, and the

same thing for Z2. And so if we look at the different cases

of this we can compute the output, magnitude of the output voltage over the

input voltage. It's always just going to be the

magnitude of this impedance divided by the magnitude of the sum of the 2

impedance. So this is just the voltage divider

equation but rewritten with impedances. And since I have these complex numbers to

deal with, we're going to just look at the magnitudes of the output to input

response. Now here's a table that summarizes all of

the cases. Now I solved two of these cases and

hopefully you solved the other two cases. But let's take a minute and look

carefully at this table. And understand all the different cases.

So, in first the column we have Z1 it's whatever I want to put in for Z1.

And the second column is Z2 and then it tells you what kind of filter you've made

and what the cut off frequency is. Now if Z1 is a resistor and Z2 is a

capacitor, then I have the simple RC filter that we solved first and we saw

that that was at low pass filter. And it has a cutoff frequency of 1 over

RC, now that was omega tTo turn that into regular hertz units.

We have to divide by 2 pi, with a relationship between angular frequency

and regular frequency in hertz is angular frequency divided by 2 pi gives me

regular frequency. Now, let's go back and look at this a

little bit more. This is a low pass filter because Z2,

when omega is small. This impedance becomes very large and so

this is like a voltage divider with a small impedance and then a very large

impedance. And you know from the old resistive

voltage divider that you get most of the voltage drop across the larger impedance

and the voltage divider. So now at low frequency Z2, the

capacitor, becomes a very large impedance.

In fact, when omega goes to 0 this goes to infinity.

And all of the voltage appears all of the, the voltage applied to the input

appears at the output. As I go up in frequency, this factor

becomes smaller. And so I have a larger impedance here and

a smaller impedance there. And so this voltage divider then is going

to give you a smaller output voltage. So low frequencies are favored in this,

the output of this RC filter built this way and high frequencies are attenuated

by this filter. Now if I replace Z2 with an inductor,