Low and High Frequency Signal Equivalent

Click For Summary
SUMMARY

The discussion focuses on deriving the low and high-frequency small signal equivalents for a PMOS amplifier circuit, specifically addressing parts b and c of the homework assignment. The high-frequency small signal equivalent involves simplifying the MOSFET capacitance model, primarily considering Cgd (Miller effect) and Cgs. The maximum gain of the amplifier is determined by analyzing the equivalent resistance and capacitance, leading to the upper 3dB frequency formula, which is calculated using τ = RC, where Ceq is defined as Cgs + Cgd.

PREREQUISITES
  • Understanding of PMOS transistor operation and characteristics
  • Familiarity with small signal analysis in electronic circuits
  • Knowledge of frequency response and 3dB cutoff concepts
  • Basic circuit analysis techniques involving capacitors and resistors
NEXT STEPS
  • Study the Miller effect in detail and its impact on amplifier design
  • Learn about the derivation of the upper 3dB frequency formula in MOSFET amplifiers
  • Explore advanced small signal models for MOSFETs, including parasitic capacitances
  • Investigate techniques for optimizing amplifier gain and frequency response
USEFUL FOR

Electrical engineers, students studying analog circuit design, and anyone involved in amplifier performance analysis will benefit from this discussion.

DODGEVIPER13
Messages
668
Reaction score
0

Homework Statement


Assume λ≠0. Also bypass capacitor is very large compared to coupling capacitor.
a.) Draw the low frequency small signal equivalent and derive lower 3dB frequency formula.
b.) Assuming transistor high frequency capacitances, draw the high frequency small signal equivalent and derive upper 3dB frequency formula
c.) What is the maximum gain of this amplifier? Finally draw the magnitude. Oh and the circuit is in the thumbnails

I only need help with b and c

Homework Equations


The Attempt at a Solution


I have figured out part a and have drawn part b I have it drawn such that it goes from ground to Vs and then to Rs, with cc1 shorted, and then Rg in parallel with Vs then Cgs in parallel with Rg and Cgd in series with the ground terminal of the mosfet. I have the dependent source connected to ground and going up as the circuit is PMOS at GmVsg and the ro, Rd, and Rl are all in parallel and on Vo. Now what I am wondering is how do I get Ceq I have Req=ro in parallel with Rd in parallel with Rl. I mean there isn't a cap on the output side so I am confused on how to find the upper frequency I know the formula is 1/(2pi(τ)) where τ=RC I think Ceq=Cgs+Cgd. Sorry for the terrible writing quality but I don't have a way to scan in my circuit nor a way to draw it.
 

Attachments

  • Capture.PNG
    Capture.PNG
    7.4 KB · Views: 567
Last edited:
Physics news on Phys.org
To do part (b) you probably want to simplify the usual 6-or-so-capacitance model for the MOSFET. I suggest cutting down to one or two. (Some of the other capacitances are removed by virtue of the heavily bypassed source anyway).

The biggest contributor to limiting the high-frequency response is probably Cgd, aka the "Miller" effect. Any voltage variations in the drain get fed back to the gate thru this capacitance.

The second-biggest contributor is probably Cgs which, since the source is heavily bypassed, is just the capacitance from the gate to ground. So just parallel Rg with Cgs.
 
Thanks man I got it figured it out
 

Similar threads

  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 10 ·
Replies
10
Views
2K
  • · Replies 12 ·
Replies
12
Views
2K
  • · Replies 12 ·
Replies
12
Views
2K
  • · Replies 4 ·
Replies
4
Views
4K
Replies
2
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 16 ·
Replies
16
Views
2K