Title: Feedback Amplifier Stability
1Feedback Amplifier Stability
- Feedback analysis
- Midband gain with feedback
- New low and high 3dB frequencies
- Modified input and output resistances, e.g.
- Amplifiers frequency characteristics
- Feedback amplifiers gain
- Define Loop Gain as ßfA
- Magnitude
- Phase
A(?)
Ao
Afo
Amplifier becomes unstable (oscillates) if at
some frequency ?i we have
2Feedback Amplifier Instability
General form of Magnitude plot of ßfA
- Amplifier with one pole
- Phase shift of - 900 is the maximum
- Cannot get - 1800 phase shift.
- No instability problem
- Amplifier with two poles
- Phase shift of - 1800 the maximum
- Can get - 1800 phase shift !
- For stability analysis, we define two
important frequencies - ?1 is where magnitude of ßfA goes to unity
(0 dB) - ?180 is where phase of ßfA goes to -180o
- Instability problem if ?1 ?180
ßfA(dB)
0 dB
General form of Phase plot of ßfA
00
- 450
- 900
- 1350
- 1800
3Gain and Phase Margins
ßfA(dB)
- Gain and phase margins measure how far
amplifier is from the instability condition - Phase margin
- Gain margin
- What are adequate margins?
- Phase margin 500 (minimum)
- Gain margin 10 dB (minimum)
0 dB
Gain margin
- 30
00
- 450
- 900
F(?1)
- 1350
Phase margin
F(?180)
- 1800
4Numerical Example - Gain and Phase Margins
ßfA(dB)
Pole 1
23.5 dB
Pole 2
Gain margin
Phase Shift (degrees)
Note that the gain and phase margins
depend on the feedback factor ßf and so
the amount of feedback and feedback
resistors. Directly through the value of
ßf. Indirectly since the gain Ao and
pole frequencies are influenced by
the feedback resistors, e.g. the
loading effects analyzed previously.
Phase margin
5Amplifier Design for Adequate Gain and
Phase Margins
General form of Magnitude plot of A
- How much feedback to use? What ßf ?
- A change of ßf means redoing ßf A(?)
plots! - Is there an alternate way to find the
gain and phase margins? YES - Plot magnitude and phase of gain A(?)
instead of ßf A(?) vs frequency - Plot horizontal line at 1/ ßf on magnitude
plot (since ßf is independent of
frequency) - Why? At intersection of 1/ ßf with A(?),
? ?1 - So this intersection point gives the value
where ? ?1 ! - Then we can find the gain and phase
margins as before. - If not adequate margins, pick another ßf
value, draw another 1/ ßf line and repeat
process. - Note ßf is a measure of the amount of
feedback. Larger ßf means more feedback. - Recall for ßf 0, we have NO feedback
- As ßf increases, we have more feedback
A(dB)
1/ßf(dB)
Gain margin
A(?180)
0 dB
General form of Phase plot of A
00
- 450
- 900
- 1350
F(?1)
Phase margin
- 1800
F(?180)
6Example - Gain and Phase MarginsAlternate
Method
A(dB)
43.5 dB
1/ßf(dB)
Gain margin
A(?180)
Phase margin
These are the same results as before for
the gain and phase margins .
7Feedback Amplifier with Multiple Poles
A(?)
- Previous feedback analysis
- Midband gain
- New low and high 3dB frequencies
-
-
- Amplifiers typically have multiple high and
low frequency poles. - Does feedback change the poles other than
the dominant ones? - YES, feedback changes the other poles as
well. - This is called pole mixing.
- This can affect the gain and phase margin
determinations ! - The bandwidth is still enlarged as
described previously - But the magnitude and phase plots are
changed, so the gain and phase margins are
modified.
Ao
Afo
8Feedback Effect on Amplifier with Two Poles
New poles of the feedback amplifier occur
when
- Gain of a two pole amplifier
- Gain of the feedback amplifier
Midband gain of feedback amplifier.
Gain of feedback amplifier having two new,
different high frequency poles.
9Feedback Effect on Amplifier with Two Poles
- Feedback amplifier poles
- For no feedback (ßf 0),
- For some feedback (ßf Ao gt 0), Q increases
and 1- 4Q2 ? 0 so poles move towards each
other as ßf increases. - For ßf such that Q 0.5, then 1- 4Q2 0
so two poles coincide at - For larger ßf such that Q gt 0.5, 1- 4Q2 lt 0
so poles become complex frequencies.
Root-Locus Diagram
j?
s ? j?
?
j?
?
10Frequency Response - Feedback Amplifier with
Two Poles
- Amplifier with some feedback ( ßf Ao gt 0 ),
as ßf increases 1 - 4Q2 ? 0 so poles move
towards each other. For sufficient feedback,
Q 0.5 and 1 - 4Q2 0 so the poles meet
at the midpoint.
Increasing feedback, poles meet for Q 0.5
Af(dB)
Original amplifier
Original poles before feedback
For Q 0.707, we get the maximally
flat characteristic For Q gt 0.7, get a
peak in characteristic at
corresponding to oscillation in the
amplifier output for a pulsed input
(undesirable).
Af(dB)
Qgt0.7
Original amplifier
11Frequency Response of Feedback on Amplifier
with Two Poles
- 3dB
3dB frequency increases as feedback (Q and ßf)
increases!
- For no feedback (ßf 0), Q is a minimum
and we have the original two poles. - For some feedback (ßf Ao gt 0), Q gt 0 and
1- 4Q2 ? 0 so poles move towards each
other. - For ßf such that Q 0.5, then 1 - 4Q2 0
so two poles coincide at - ?o/2Q. - For larger ßf such that Q gt 0.5, 1- 4Q2 lt 0
and the poles become complex - For ßf such that Q 0.7, we get the
maximally flat response (largest bandwidth). - For larger ßf such that Q gt 0.7, we get a
peak in the frequency response and
oscillation in the amplifiers output
transient response (undesirable).
12Example - Feedback Amplifier with Two Poles
- DC bias analysis
- Configuration Shunt-Shunt (ARo Vo/Is)
- Loading Input R1 Rf , Output R2 Rf
- Midband gain analysis
10 V
10 V
RC1.5 K
RB190 K
Rf8 K
Rs10 K
?75 rx0 C? 7 pF C? 0.5 pF
If
RB210 K
RB 9 K
13Example - Feedback Amplifier with Two Poles
- Determine the feedback factor ßf
- Calculate gain with feedback ARfo
- High frequency ac equivalent circuit
Rs
Is
RB
R1
R2
14Original High Frequency Poles
Rs
Is
RB
R1
R2
C? Pole
C? Pole
Rs
RB
R1
R2
See how we did the analysis for the C?2
high frequency pole for the Series-Shunt
feedback amplifier example.
15Gain and Phase Margins
A(dB)
38.5 dB
1/ßf(dB)
Gain margin
A(?180)
F(?1)
Phase margin
F(?180)
16High Frequency Poles for Feedback Amplifier
Note that this Q value is bigger than
0.707 so the amplifier will tend to
oscillate (undesirable).
- These new poles are complex numbers !
- Original poles were at 2.1x107 and
2.3x108 rad/s. - This means the amplifier output will
have a tendency to oscillate (undesirable!) - We have too much feedback !
- Q is too large, because ßf is too
large, because Rf is too small (ßf -
1/Rf)! - How to change Rf so that ßf and Q are
not too large? - Need to increase Rf so that ßf and Q
are smaller. - How much to increase Rf ?
17Frequency Response with and without Feedback
Original amplifier (without feedback)
Amplifier with feedback
18What is the Optimum Feedback and Rf ?
Select Q 0.707 and work backward to
find ßf and then Rf Q 0.707 gives
maximally flat response !
New poles are still complex numbers, but
Q 0.707 so okay.
19Gain and Phase Margins for Optimal Bandwidth
A(dB)
38.5 dB
1/ßf(dB)
Gain margin
A(?180)
Phase margin
20Frequency Response for Optimum Feedback
Original amplifier (without feedback)
Amplifier with feedback
Note Better midband gain than before
Improved bandwidth and No
oscillation tendency !
21Design for Minimum Phase Shift (50o)
A(dB)
- Construct plots of A(?) in dB and phase
shift versus frequency as before. - Determine frequency ?180 for -180o phase shift
- For minimum 50o phase shift,
- Measure up from -180o to -130o on phase
shift plot, draw horizontal line and
determine frequency where this is reached.
This gives ?1. - Find corresponding magnitude of A(?) in
dB at this frequency (?1) on the magnitude
plot. Draw a horizontal line. This gives
the magnitude of 1/ßf in dB. - Convert 1/ßf in dB to a decimal
- Calculate Rf from ßf
1/ßf(dB)
Gain margin
A(?180)
Phase margin
- Check gain margin to see if it is okay.
YES, 40 dB ! - But Q 0.94 gt 0.707 so some tendency to
oscillate .
22Design for Minimum Gain Margin (10 dB)
A(dB)
- Construct plots of A(?) in dB and phase
shift versus frequency - Determine frequency ?180 for -180o phase shift
- For minimum 10dB gain margin,
- Draw vertical line on magnitude plot at
?180 frequency. Where it intersects the
magnitude plot, draw a horizontal line. - Measure upward from this horizontal line by
10 dB and draw a second horizontal line.
This gives the magnitude of 1/ßf in dB
(-12dB here). - Convert 1/ßf in dB to a decimal
- Calculate Rf from ßf
1/ßf(dB)
Gain margin
Phase margin
- Check phase margin to see if it is okay.
NO, only 12o ! - Q is also very large 5.1 gtgt 0.707 so
strong oscillation tendency !
23Summary of Feedback Amplifier Stability
- Feedback amplifiers are potentially unstable
- Can break into oscillation at a particular
frequency ?i where - Need to design feedback amplifier with
adequate safety margin - Minimum gain margin of 10 dB
- Minimum phase margin of 50o.
- Adjust ßf by varying size of Rf .
- Smaller Rf is, the larger is the amount of
feedback.
A(?)
Ao
Afo
Oscillation instability is a design problem
for any amplifier with two or more high
frequency poles. This is the case for ALL
amplifiers since each bipolar or MOSFET
transistor has two capacitors and each
capacitor gives rise to a high frequency
pole!