HI Charles,
thank you for reply, it's very appreciated.
Charles Hansen wrote:
Yes, Maxpou, you are correct. I know that English is not your first language and that is why I suggested Tietze and Schenk. I was hoping that it has been translated into other languages. In many ways it is better than Horowitz and Hill. Actually it is best to have them both...
I have Horowitz and Hill second edition, but I will order the other book as soon as possible. Thank you for your suggestions
Charles Hansen wrote:
As far as the input impedance of Q3, yes it is very high. I would state the reason differently however. I would say that it is because the G-S junction is a reverse-biased diode. This is a very helpful way to look at it. It then become obvious why the input impedance is so high. It also warns you what happens if the input signal exceeds +/- 0.6 Vpeak (think about it).
I have a problem if I want 2Vrms at output.
Charles Hansen wrote:
The input impedance of the collector of Q7 is also high. There are many ways to understand this. One way is to look at the slope of the characteristic curves. Look at the basically (but not quite) horizontal lines. If you look at the change in Vce divided by the change in Ic, the unit will be reciprocal ohms. This is referred to as the output conductance of the part and is the reciprocal of the output resistance. The flatter the curves, the higher the output impedance. Most BJTs have an output impedance (at the collector) on the order of a few hundred kohms.
Thank you again for your explaination.
Charles Hansen wrote:
So if the current is coming out of Q4 then it will be hard to go into either Q3 or Q7. By Ohm's law E = IR, so what will the voltage be at the junction of Q3, Q4, and Q7?
I'm not sure but, if I set my current sink (Q7) at 4mA for 2Vrms I add a resistor to ground of 1.4K to the junction of Q4, Q3 and Q7.
Maxpou