I don't exactly understand what you're up to? If you know the OP open loop gain characteristic, you can calculate the closed loop gain pretty accurately.
...or the gain of the buffer is unity but this under condition of the open loop gain AOL >= 60db. .........
OK - that´s correct (may be, one can define the limit at AOL>=40...50 dB, but that`s not the point).
However, please note that the limit you have mentioned (60 dB) applies to the unity-gain buffer application only!
Because in this case the loop gain T(s)=(buffer gain*AOL)=60 dB.
For other application with gain values>0 dB the limit of 60 dB applies to the loop gain - and NOT to the AOL of the opamp alone.
See my last post.
In this context, I point to the fact that the first attachement you have shown contains also the loop gain response vs. frequency.
It is simply the AOL curve - however, referred to another frequency axis, which is now the 20 dB line.
I am really sorry if still I am not getting it, so I would ask you according to the left image (part 7.2). as you see that up to wa the AOL is very high so we can apply the closed loop principles. after wa and specially near to w-3db of the closed loop response the AOL is now very low so how we still keep the same expression of the ACL of the closed loop gain in this area as like the same ACL in the low frequency region. I think my second image is describing my problem more clear
Thank you a lot
Well, I think you are able to understand my comment only if you know
* the formula from Black (and it`s meaning): Acl=Aol*a/(1+Aol*b) with b=feedback factor
* the role of the loop gain T=Aol*b
What is the remaining question?
...........
when you go now to substitute these values in the ACL = AOL / (1+b*AOL), you will find that we get a unity gain result only till 50 KHz, .
No, I don`t think so. Why 50 kHz? Why not 10 kHz or 100 kHz?
For a finite AOL we always are somewhat below 0 dB. The only question is how much error (deviation from 0 dB) you can tolerate.
By the way - also the assessment of -3dB at w=GBW applies under the assumption that AOL is a single pol model.
For real amplifiers with a second pole in the vicinity of the 0dB-crossing frequency there will be a slight peaking in the magnitude response in this frequency region.
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