0:00
This question.
00:01
So, in the first part, a p -n junction, a p -n junction, junction -based diode is a semiconductor, is a semiconductor represented by s dot c, semiconductor device formed by joining, formed by joining two different types, two different types of semiconductors, that is namely it is p -type semiconductor and p -type semiconductor and second one is n -type semiconductor.
00:54
The p -n junction is a crucial component in various, the p -n junction, the p -n junction is a crucial, crucial component in various electronic device, in various electronic, electronic devices.
01:30
So, the main physical principle and principles underlying the operation of the p -n junction are, first one is majority and minority charge carriers, majority and minority, minority carriers.
01:50
So, in n -type of semiconductor, in n -type, majority charge carriers are electrons and minority will be positively charged, that is holes and in n -type and in p -type, in p -type, the majority charge carriers are holes, these are majority charge carriers, majority charge carriers and here also this is majority charge carriers.
02:25
Now, another thing is formation of depletion region, formation of, of depletion, depletion region.
02:40
So, it is formed when, when n -type and p -type semiconductor are brought together.
02:46
Electrons from n -type, electrons from n -type diffuse, diffuse to the, to the p -side, okay and holes and holes from the p -side diffuse to n -side.
03:10
The movement of charge carriers lead to the formation of depletion region.
03:15
Now, the third thing is barrier potential.
03:20
So, third is barrier potential, barrier potential.
03:29
So, as the charge carrier diffuse across the junction, they create an electric field that opposes further carrier movement and the third is forward bias, forward bias.
03:43
When the, when a positive voltage is applied to p -side and the negative voltage to the n -side, it is forward bias and the reverse goes to the reverse bias.
03:55
That is the, the positive side, positive potential of the battery is connected to the negative of the n, n -side of the p -n junction.
04:08
Now, moving forward, we have to derive the current for forward bias as well as for reverse bias.
04:15
So, for, firstly for forward bias, the total current will be i drift plus i diffusion...