00:02
Alright, so in this question, given this circuit here, and yeah, that's clear now for you to see.
00:12
We got all the, we got that transistor.
00:20
Got the three resistors there.
00:24
We'll source and we've got a bunch of other things going on.
00:27
We have the current going on there.
00:29
So what we want to do here a couple of things.
00:32
First is to find the current gain.
00:37
The forward common emitter current gain.
00:44
Next we'll find the vcc and then we would have to find so voltage, collect a current, and then we have to find that resistor right there rb.
01:01
Okay, so let's get to it.
01:04
Well, first of all, we want to calculate, we need to figure for us to find that current gain.
01:11
We know that what we're going to is that current gain has to be ic over ib all right that's how i'm thinking about this so we can reverse engineer this and we will get to where we need to be well again that current gain would be the current through the collector divided by the current at base, right? okay, so, well, one thing to see here would be that this i -c would be approximately equal to a current at their metta, and i hope you can see why that would be the case.
02:17
And this in turn is equal to, well, if you want to use oms law, which is v equals to i -r, we can see that here, the i would be be v over r, therefore the current at the emitter would be v the voltage across that emitter over the resistor at the, you know, the meter.
02:50
So let me put that in actual writing here.
02:53
So we get that this becomes, well, i .e, approximately, i .e over i .b.
03:03
What is i .e? i .e.
03:05
Really.
03:06
Is ve over vr and that's also going to be over i b.
03:16
Good.
03:20
So, well, this is the current here, i .b.
03:28
So that's not too bad.
03:30
We can, we know what that would be.
03:33
You can figure that out.
03:34
So let's do the rest of it.
03:37
By the way, this is a.
03:39
Therefore, we get that, well, ve is the current.
03:47
At the emitter.
03:50
So the voltage at that meter, well, that is, voltage across here is 2 .1.
03:59
Again, this is the emitter, right? so let's do it.
04:02
So it's going to be 2 .1 over that resistor here, the meter, which would be 0 .68.
04:17
And that is all over, all over the current base here, which is going to be 20 micro -ooms.
04:33
So 20 micro -amps.
04:37
So let's actually do this.
04:40
Make sure we have this.
04:41
This also was in kilos.
04:43
So that's to the third.
04:45
And this is in volts, so that is an acid unit.
04:47
Okay? just wanted to make sure that we have everything here in the right unit.
04:54
So you see that we have it all set up.
04:56
So the answer here, really, comes to 154 .5.
05:07
And this is the value of what? this is the forward common emitter current gain.
05:34
Let's now try for the next one.
05:39
We ought to figure out the vcc.
05:44
What is this one here? so for vcc, what we can do? well, we're going to apply kirchhoff's voltage law across the output terminal.
06:04
So for kirchhoff's voltage law, remember what that is.
06:08
It says if we go round a loop, what happens? we add up all the voltages.
06:16
It's going to give us the sum come to zero.
06:22
What does that look like? let's say we started here, the vcc, right? take that voltage.
06:31
We'll go across the collector, right? start here, we go.
06:43
We did that.
06:44
But it's going to be a voltage drop.
06:47
So that's going to be the ic, or rc.
06:51
This is rc.
06:53
Right? this is ic...