00:01
So here we are given i m this is equal to 1 .18 m a by divided by v.
00:10
So small signal mid base ac equivalent.
00:15
This are capacitors shortened and if we talk about a v this is equal to minus i m multiplied by 3k multiplied by 3 .9 k vgs divided by vgs multiplied by 10 raised to the power 6 divided by 10 raised to the power 6 plus 10 raised to the power 3.
00:51
So a v this is equal to minus 1 .18 into 10 raised to the power minus 3 multiplied by 1 .695 multiplied by 10 raised to the power 3.
01:09
So from here we get a v as minus 2 .0008 which is basically equal to minus 2.
01:20
So a v this is equal to minus 2 and then we have z i this is equal to 10 raised to the power 6 plus 10 raised to the power 3.
01:32
So this is going to be equal to 1 0 0 1 k ohms.
01:40
Now talking about the high frequency.
01:45
So by using the miller theorem so we have c m this is equal to c gd 1 minus a v.
01:58
So substituting we have 4 pf 1 plus 2.
02:07
This is equal to 4 multiplied by 3 is 12.
02:12
So it will be 12 pf.
02:15
Similarly c n this is equal to c gd 1 minus 1 divided by a v and we have 4 pf 1 plus 1 divided by 2.
02:30
So we have this as 6 pf.
02:34
Now c in this is equal to cwi plus cgs plus c m.
02:47
So this is nothing but 3 plus 6 plus 12...