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5/25/2018 0574.Solving Op Amp Stability 2013_Part 2
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Solving Op Amp Stability IssuesPart 2
(For Voltage Feedback Op Amps)
Tim Green & Collin Wells
Precision Analog Linear Applications1
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StabilityTricks and Rules-of-Thumb
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180
0
135
45
10 100 1k 10k 100k 1M 10M
Frequency
(Hz)90
(degrees)
-45
fp1
fp2 fz1
fcl
90o
Phase Margin
at fcl
45o
Phase Buffer
away from
180o
Phase Shift
90
o
Phase Shift
at fcl
3
Loop Gain Bandwidth Rule: 45 degrees for f < fcl
Aol(Loop Gain) Phase Plot
Loop Stability Criteria:< -180 degree phase shift at fcl
Design for: < -135 degree phase shift at all frequencies < fclWhy?:
Because Aol is not always Typical
Power-up, Power-down, Power-transientUndefined TypicalAol
Allows for phase shift due to real world Layout & Component Parasitics
Prevent excessive ringing due to phase margin dip near fcl
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4
+
-
+
-
VIN
RI
RF
VOUT
CL
CnRn
0
20
40
60
80
100
10M1M100k10k1k100101
Frequency (Hz)
A
(dB)
fcl
fp1
fp2
fz1
fp3
Aol
1/Beta
VOUT
/VIN
Loop Gain View: Poles: fp1, fp2, fz1; Zero: fp3
Rules of Thumb for Good Loop Stability:
Place fp3 within a decade of fz1
fp1 and fz1 = -135phase shift at fz1
fp3 < decade will keep phase from dipping further
Place fp3 at least a decade below fcl
Allows Aol curve to shift to the left by one decade
Frequency Decade Rules for Loop GainFor 45OPhase Buffer away from 180OPhase Shift
Aol 1/b Loop Gainfp1 pole ----- pole
fp2 pole ----- polefz1 ----- zero pole
fp3 ----- pole zero
Note locations of poles in zeroes in Aol and 1/plots
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1 10 100 1K 10K 100K 1M 10M
-45
-90
0
+45
+90
Frequency (Hz)
Phase
Shift(deg)
Frequency (Hz)
Phase
Sh
ift(deg)
1 10 100 1K 10K 100K 1M 10M
+45
0
+90
+135
+180
fcl
fp1
fz1
fp3
fp2
Individual Pole & Zero Plot
Final Plot
45O
Phase Buffer 5
Frequency Decade Rules for Loop GainPhase Plot Prediction
At fcl:Phase Shift = 135O
Phase Margin = 45O
Aol 1/b Loop Gainfp1 pole ----- pole
fp2 pole ----- pole
fz1 ----- zero pole
fp3 ----- pole zero
Note locations of poles in zeroes in Aol and 1/plots
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6
Op Amp Circuits & Second Order Systems
0
20
40
60
80
100
10M1M100k10k1k100101
Frequency (Hz)
A
(dB)
Aol
1/Beta
fp1
fp2
fcl
+
-
+
-
VIN
RFRI
4.7k 4.7k
VOUT
Most Op Amps are dominated by Two Poles:
Aol curve shows a low frequency pole, fp1
Aol curve also has a high frequency pole, fp2
Often fp2 is at fcl for unity gain
This yields 45 degrees phase margin at unity gain
Most Op Amp Circuits are
adequately analyzed,
simulated, and real world
tested using well-known
second order system
response behavior.
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7
Control Loop - Second Order System
G(s)R(s) C(s)
1:Overdamped
1:DampedCritically
0:StableMarginally
10:dUnderdampe
:AC)and(StepResponseLoopClosed
ratiodamping
(rad/s)frequencynatural
n
2
nn
2
2
n
:where
s2s
R(s)
C(s)
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8
Closed Loop Peaking inAC Frequency Sweep vs Phase Margin
From: Dorf, Richard C. Modern Control Systems. Addison-WesleyPublishing Company. Reading, Massachusetts. Third Edition, 1981.
Phase Margin AC Peaking
@wn
90 -7dB
80 -5dB
70 -4dB
60 -1dB
50 +1dB
40 +3dB
30 +6dB
20 +9dB
13 +10dB
10 +14dB
*
* Phase Margin:
1) Measure closed loop AC peaking in dB
2) Find dB peaking on graph above and read closest damping ratio, 3) Use damping ratio, , to find phase margin using Slide 75 graph
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9
Transient Real World Stability Test
Test Tips:
Choose test frequency
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10
2nd Order Transient Curves
From: Dorf, Richard C. Modern Control Systems. Addison-WesleyPublishing Company. Reading, Massachusetts. Third Edition, 1981.
Overshoot Phase Margin
(%) (deg)
10 57.5
15 50
20 42.5
25 40
30 35
35 32.5
40 30
45 27.5
50 25
* Phase Margin:
1) Measure closed loop transient overshoot (%)
2) Find overshoot on graph above and read closest damping ratio, 3) Use damping ratio, , or Overshoot (%) to find phase margin using Slide 75 graph
** 25%
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11
2nd Order Damping Ratio, Overshoot, Phase Margin
40% = Overshoot
= 0.3
fM = 30deg
= 0.3
Overshoot = 40%, Phase Margin = 30 degrees
1. Start at % Overshoot on x-axis
2. Read up to Damping Ratio on Percent Maximum Overshoot curve
3. Read Across to Damping Ratio on y-axis4. Use Damping Ratio to read across to Phase Margin curve.
Overshoot Phase Margin
(%) (deg)
10 57.5
15 50
20 42.5
25 40
30 35
35 32.5
40 30
45 27.5
50 25
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12
When ROis really ZO!!
OPA627 has RO OPA2376 has ZO
Resistive
Resistive
Capacitive Inductive
OPA2376OPA627
Note:Some op amps have ZOcharacteristics other than pureresistanceconsult data sheet / manufacturer / SPICE Model
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13
Open Loop Output ImpedanceSPICE Measurement
ic)(LogarithmVout(ohms)Zout
ic)(LogarithmVoutto(dB)utConvert Vo
VoutZo
Zounloadedfor0AValueDCIG1
GeneratorCurrentACisIG1
AnalysisACSPICERun
:TestZoSPICE
T
Frequency (Hz)
1 10 100 1k 10k 100k 1M 10M 100M
Ro(ohms)
53.5
54.0
54.5
55.0
55.5
Vcc 15V
Vee 15V
IG1
L1 1TH
C1 1TF
Vout
+
-
+
U1 OPA627E
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14
Summary for StabilityFor Stabi l i ty Loop Gain Analysis all we need is:1) Aolfrom op amp data sheet or macromodel
2) 1/basic by application, modified for stability3) Z_Loadgiven by application
4) ZoOp Amp open loop, small signal AC output impedance
from op amp data sheet or macromodel
Stability General Comments:1) Stability by modifying 1/bwill decrease closed loop bandwidth
2) Stability compensation can slow large signal response (charging of caps)check it3) Simulate AC Transfer function (Closed Loop AC Response) as final check
4) Simulate Small Signal Transient Response as final check
5) DC operation in the lab does not guarantee stability
6) Marginal stability can cause undesired overshoot and ringing
7) DC circuits can get real world transient inputs from supplies, inputs, or output
8) That ringing in your circuit is notyour Grandmothers dial telephoneT
Time (s)
100u 150u 200u 250u 300u
VOUT
33.64m
64.94m
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15
Acknowledgements
Jerald Graeme Books:
http://www.amazon.com/Jerald-G.-Graeme/e/B001HO9X60
A special thanks to Jerald Graeme, whom we honorably dub The Godfather of
1/ for his work at Burr-Brow n Corpo rat ion in research and wr i t ing aboutOp Amp Stabi l i ty using 1/Jerald Graeme Brief Biography:From: http://electronicdesign.com/analog/jerald-graeme
When ICs and op amps were separate devices, Jerald Graeme was among the first to develop a combined IC
op amp while at Burr-Brown, in a 1968 team effort with Motorola. He designed many more op amps and video
amplifiers whose precision, high speed, or low drift amplification made them a very useful component in a
variety of analog applications. Nine U.S. patents and numerous foreign counterparts resulted from these
designs. The internationally acknowledged authority on electronic amplifiers wrote five very popular books about
op amps, the latest being Photodiode Amplifiers: Op Amp Solutions and Optimizing Op Amp Performance. The
latter, subtitled "A new approach for maximizing op amp behavior in circuit designs without extensive
mathematical analysis," offers design equations and models that reflect real-world op amp behavior and makes
analysis of difficult-looking configurations easy. Graeme's earlier books are: Op Amps: Design and Application,
Designing with Operational Amplifiers, and Amplifier Applications of Op Amps. He expects signal processingwith op amps to be the domain of digital devices, but they will still require an analog interface to integrate with
real-world items like process control or avionics.
http://www.amazon.com/Jerald-G.-Graeme/e/B001HO9X60http://www.amazon.com/Jerald-G.-Graeme/e/B001HO9X60http://electronicdesign.com/analog/jerald-graemehttp://electronicdesign.com/analog/jerald-graemehttp://electronicdesign.com/analog/jerald-graemehttp://electronicdesign.com/analog/jerald-graemehttp://www.amazon.com/Jerald-G.-Graeme/e/B001HO9X60http://www.amazon.com/Jerald-G.-Graeme/e/B001HO9X60http://www.amazon.com/Jerald-G.-Graeme/e/B001HO9X60http://www.amazon.com/Jerald-G.-Graeme/e/B001HO9X60http://www.amazon.com/Jerald-G.-Graeme/e/B001HO9X60http://www.amazon.com/Jerald-G.-Graeme/e/B001HO9X605/25/2018 0574.Solving Op Amp Stability 2013_Part 2
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Acknowledgements
Op Amp Stability Series
Tim Green, Senior Analog Applications Engineer
Texas Instruments
http://www.en-
genius.net/site/zones/acquisitionZONE/technical_notes/acqt_050712
http://www.en-genius.net/site/zones/acquisitionZONE/technical_notes/acqt_050712http://www.en-genius.net/site/zones/acquisitionZONE/technical_notes/acqt_050712http://www.en-genius.net/site/zones/acquisitionZONE/technical_notes/acqt_050712http://www.en-genius.net/site/zones/acquisitionZONE/technical_notes/acqt_050712http://www.en-genius.net/site/zones/acquisitionZONE/technical_notes/acqt_050712http://www.en-genius.net/site/zones/acquisitionZONE/technical_notes/acqt_0507125/25/2018 0574.Solving Op Amp Stability 2013_Part 2
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Appendix
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Appendix Index1) Op Amp Output Impedance2) Pole and Zero: Magnitude and Phase on Bode Plots
3) Dual Feedback Paths and 1/b
4) Non-Loop Stability Problems
5) Stability: Riso (Output Cload)
6) Stability: High Gain and CF (Output Cload)
7) Stability: CF Non-Inverting (Input Cload)
8) Stability: CF Inverting (Input Cload)9) Stability: Noise Gain Inverting & Non-Inverting (Output Cload)
10) Stability: Noise Gain and CF (Output Cload)
11) Stability: Output Pin Compensation (Output Cload)
12) Stability: Riso w/Dual Feedback (Output Cload)
Zo, 1/b, Aol Technique13) Stability: Discrete Difference Amplifier (Output Cload)
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Appendix IndexAppendix No. Title Description/StabilityTechnique When to use the StabilityTechnique
1 Op Amp Output Impedance Zo vs Zout difference and datasheet curves Zo is a key parameter for stability analysis
2
Pole and Zero:
Magnitude and Phase on Bode Plots
Closed loop magnitude and phase shifts of a signal
frequency due to poles and zeroes on a Bode Plot
Magnitude and phase shift at a frequency of
interest for closed loop poles and zeroes
3 Dual Feedback Paths and 1/How to avoid problems when using dual feedback
paths for stability compensation
Key tool in analyzing op amp circuits that use
dual feedback for stability
4 Non-Loop Stability Problems
Oscillations and causes not seen in loop gain stability
simulations
Check all designs to avoid oscillations that do
not show up in SPICE simulation
5 Riso (Output Cload) Stability: Isolation resistor with feedback at op amp
Output Cload, Note: accuracy of output is
dependent upon load current
6 High Gain and CF (Output Cload) Stability: High gain circuits and a feedback capacitor Output Cload, closed loop gain >20dB
7 CF Non-Inverting (Input Cload) Stability: Non-inverting gain and feedback capacitor
Input Cload, non-inverting gain, large value
input resistor
8 CF Inverting (Input Cload) Stability: Inverting gain and feedback capacitor
Input Cload, non-inverting gain, large value
input resistor, photodiode type circuits
9
Noise Gain Inverting and
Non-Inverting (Output Cload) Stability: Noise Gain added by input R-C network Output Cload, closed loop gain 20dB
11 Output Pin Compensation (Output Cload) Stability: Series R-C on op amp output to ground
Output Cload, no access to -input, monolithic,
integrated difference amplifiers, complex
feedback where not practical to use -input
12
Riso w/Dual Feedback (Output Cload)
- Zo, 1/, Aol Technique
Stability: Isolation resistor with two feedback paths -
analysis by Zo, 1/, and Aol technique
Output Cload, some additional Vdrop across
isolation resistor is okay, accurate Vout at load
13 Discrete Difference Amplifier (Output Cload) Stability: Balanced use of noise gain (series R-C)
Output Cload, difference amp configuration,
any closed loop gain
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1) Op Amp Output Impedance
Open Loop (ZO)&
Closed Loop (ZOUT)
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21
Op Amps and Output Resistance
+
-
RDIFF
xAol
RO-IN
+IN
-
+
VE
Op Amp Model
1A
VOUT
VO
RF
RI
IOUTVFB
ROUT= VOUT/IOUT
From: Frederiksen, Thomas M. Intuitive Operational Amplifiers.McGraw-Hill Book Company. New York. Revised Edition. 1988.
Definition of Terms:
RO= Op Amp Open LoopOutput Resistance
ROUT= Op Amp Closed LoopOutput Resistance
ROUT= RO/ (1+Ao l)
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22
1)b= VFB / VOUT = [VOUT (RI/ {RF+ RI})]/VOUT= RI/ (RF+ RI)
2) ROUT= VOUT / IOUT
3) VO= -VEAol
4) VE= VOUT[RI / (RF+ RI)]
5) VOUT= VO+ IOUTRO
6) VOUT= -VEAol + IOUTRO Substitute 3) into 5) for VO
7) VOUT= -VOUT[RI/(RF+ RI)] Aol+ IOUTRO Substitute 4) into 6) for VE
8) VOUT+ VOUT[RI/(RF+ RI)] Aol = IOUTRO Rearrange 7) to get VOUTterms on left
9) VOUT= IOUTRO/ {1+[RIAol/(RF+RI)]} Divide in 8) to get VOUTon left
10) ROUT= VOUT/IOUT=[ IOUTRO/ {1+[RIAol / (RF+RI)]} ] / IOUT
Divide both sides of 9) by IOUTto get ROUT [from 2)] on left
11) ROUT= RO / (1+Aol) Substitute 1) into 10)
Derivat ion of ROUT(Closed Loop Outpu t Resistance)
ROUT= RO/ (1+Ao l)
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23
ROUTvs RO
ROdoes NOTchange when Closed Loop feedback
is used
ROUTis the effect of RO, Aol, and controlling VO
Closed Loop feedback () forces VOto increase ordecrease as needed to accommodate VOloading
Closed Loop () increase or decrease in VOappears atVOUTas a reduction in RO
ROUTincreases as Loop Gain (Aol) decreases
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24
When ROis really ZO!!
OPA627 has RO OPA2376 has ZO
Resistive
Resistive
Capacitive Inductive
OPA2376OPA627
Note:Some op amps have ZOcharacteristics other than pureresistanceconsult data sheet / manufacturer
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25
With Complex ZO, Accurate Models are Key!
-
+
+
4
3
5
1
2
U1 OPA2376
V1 2.5V
V2 2.5V
IG1 0
L1 1TH
C1 1TFVout
ic)(LogarithmVout(ohms)Zout
ic)(LogarithmVoutto(dB)utConvert Vo
VoutZo
Zounloadedfor0AValueDCIG1GeneratorCurrentACisIG1
AnalysisACSPICERun
:ZoMacroAmpOpofTestSPICE
T
Frequency (Hz)
10 100 1k 10k 100k 1M 10M
Impe
dance(ohms)
100.00m
1.00
10.00
100.00
1.00k
400uA Load
OPA2376
f
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26
Some Data Sheets Specify ZOUT NOTZO
1
1
2
2
3
3
Aol
1R
Aol1
RR
OUT
OOUT
b
:AolofInverseisROUT
Recognize ROUTinstead of RO:
ROUTinversely proportional to Aol
ROUTtypically
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27
Some Data Sheets Specify ZOUTNOTZO
b
b
200R11
R100
Aol1
RR
OO
OOUT
(0dB)1Aol10MHz,f1,Afor100R
:(0dB)1AolwhereRfromRCompute
VOUT
OUTO
Point frequency Aol
ROUT (AV=1)
Datasheet
ROUT (AV=1)
Computed---------- (Hz) (dB) (ohms) (ohms)
1 10M 0 100 RO = 200
2 100k 40 2 2
3 10k 60 0.2 0.2
1
2
3
TLC082
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28
2) Pole and Zero:Magnitude & Phase on Bode Plots
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Formulae for Pole and Zero Calculations
29
2
210
fp
f1
1LOG20dB)Magnitude(
poleoffrequencyfp
signaloffrequencyf:where
fforMagnitudePole
2
2
10fz
f1LOG20dB)Magnitude(
poleoffrequencyfz
signaloffrequencyf:where
fforMagnitudeZero
)fp
f(tan)degPhase( 1
poleoffrequencyfp
signaloffrequencyf
:where
fforShiftPhasePole
)fz
f(tan)degPhase( 1
poleoffrequencyfz
signaloffrequencyf
:where
fforShiftPhaseZero
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Closed Loop Gain: Magnitude and Phase
30
)1fz
f(tan)
1fz
f(tan)
2fp
f(tan)
1fp
f(tan(deg)Phase
2fz
f1LOG20
1fz
f1LOG20
2fp
f1
1LOG20
1fp
f1
1LOG20KLOG20dB)Magnitude(
1111
2
2
102
2
10
2
210
2
21010
V/VinGainDCK
2zerooffrequencyfz2
1zerooffrequencyfz1
2poleoffrequencyfp21poleoffrequencyfp1
signaloffrequencyf
:where
:ffrequencyforPhaseandMagnitudeLoopClosed
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Closed Loop Gain: Magnitude and Phase
31)
3e004766055.1
f(tan)
00974485.10
f(tan(deg)Phase
)3e004766055.1(
f1
1LOG20
)00974485.10(
f1
1LOG20)100(LOG20dB)Magnitude(
)
2fp
f(tan)
1fp
f(tan(deg)Phase
2fp
f1
1LOG20
1fp
f1
1LOG20KLOG20dB)Magnitude(
11
2
210
2
21010
11
2
210
2
21010
V/VinGainDCK
pole2offrequencyfp21poleoffrequencyfp1
signaloffrequencyf
:where
:ffrequencyforPhaseandMagnitudeLoopClosed-
++
U1 OPA364
V1 2.5V
V2 2.5V
RF 99kOhm
RI 1kOhm
VOUT
+
VIN
CF 1.6nF
R1 1kOhm
C1 15.9uF
kHz004766055.1nF6.1k992
1
CFRF2
12fp
Hz00974485.10F9.15k12
1
1C1R2
11fp
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Closed Loop Gain: Magnitude and Phase
32
T
Gain(dB)
-140
-120
-100
-80
-60
-40
-20
0
20
40
Frequency (Hz)
1 10 100 1k 10k 100k 1M 10M
Phase[deg]
-180.00
-135.00
-90.00
-45.00
0.00
[A]
[B] Gain :
VOUT B:(3.924588k; -24.084018)
Phase : VOUT B:(3.924588k; -163.475026)
Gain :
VOUT A:(92.20173; 20.624635)
Phase :
VOUT A:(92.20173; -89.067371)
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Spice Compared with Calculated Analysis
33
SPICE AC Analysis:
For best accuracy use highest resolution
i.e. maximum Number of Points
Note:
1) SPICE analysis accounts for loop gain effects and closed loop phase shifts
due to op amp Aol.
2) Calculated results do not account for loop gain effects and closed loop phase shifts
due to op amp Aol.
f Magnitude Magnitude Phase Phase(Hz) (dB) (dB) (deg) (deg)
---------- Calculated SPICE Calculated SPICE
9.22017300E+01 20.6263744 20.624635 -89.04706182 -89.067371
3.92458800E+03 -23.97775119 -24.084018 -165.49354967 -163.475026
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Closed Loop Gain: Magnitude and Phase
34
R1 1kOhm
C1 15.9uF
+
VG1
-
+
-
+
DC Gain 100RF 99kOhm
CF 1.6nF-
+
-
+
Buff er 1 VOUT
SPICE Ideal Op Amp & Poles: Equivalent Circuit
Note:
1) SPICE - Ideal Circuit analysis matches Calculated results.
2) No loop gain effect or closed loop phase shifts due to op amp Aol.
f Magnitude Magnitude Phase Phase
(Hz) (dB) (dB) (deg) (deg)
---------- Calculated SPICE - Ideal Calculated SPICE - Ideal
9.22017300E+01 20.6263744 20.626374 -89.04706182 -89.047062
3.92458800E+03 -23.97775119 -23.977751 -165.49354967 -165.49355
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Closed Loop Gain: Magnitude and Phase
35
SPICE Ideal Op Amp & Poles: Equivalent CircuitT
Gain(dB)
-160
-140
-120
-100
-80
-60
-40
-20
0
20
40
Frequency (Hz)
1 10 100 1k 10k 100k 1M 10M
Phase[deg]
-180
-135
-90
-45
0
[B]
[A] SPICE Poles-Magnitude and Phas eIdeal Op Amp Circuit
Gain :
VOUT B:(3.924588k; -23.977751)
Phase :
VOUT B:(3.924588k; -165.49355)
Gain :
VOUT A:(92.20173; 20.626374)
Phase :
VOUT A:(92.20173; -89.047062)
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36
3) Dual Feedback Paths and 1/
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37
Dual Feedback Networks:Analyze & Plot each FB#? 1/
Smallest FB#? dominates 1/
1/= 1 / (1 + 2)
1/relative to VO
Note: VO = Op Amp Aol Output before
Ro for this Dual Feedback Example
Analogy:Two people are talking in your ear. Which
one do you hear? The one talking the loudest!
Dual Feedback:Op amp has two feedback paths
talking to it. It listens to the one that feeds back the
largest voltage (= VFB / VOUT). This implies the
smallest 1/!
Dual Feedback and 1/Concept
0
20
40
60
80
100
10M1M100k10k1k100101
Frequency (Hz)
A(
dB)
Aol
1/Beta[1/(b1 + b2)]
FB#1
b
fcl
FB#2
b
+
-
+
-
VOUT
CLRiso
CF
RF
RI
VIN
RO
FB#1
FB#2
VO
VOA
Dual Feedback and 1/
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38
Answer:
TheLargest
(Smallest 1/)willdominate!
Dual Feedback and 1/
How will the two feedbacks combine?
-
Large
Small
Small 1/
Large 1/
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39
0
20
40
60
80
100
10M1M100k10k1k100101
Frequency (Hz)
A
(dB)
Aol
1/Beta
FB#1
fcl
FB#2
1/Beta
Dual Feedback and the BIG NOT
Dual Feedback and the BIG NOT:
1/Slope changes from +20db/decadeto -20dB/decade Implies a complex conjugate pole in the 1/Plot with small damping ratio, .
Implies a complex conjugate zero in the Aol(Loop Gain Plot) with small damping ratio, . +/-90phase shift at frequency of complex zero/complex pole.
Phase slope from +/-90/decade slope to +/-180in narrow band near frequency
of complex zero/complex pole depending upon damping ratio, .
Complex zero/complex pole can cause severegain peaking in closed loop response.
WARNING:This can be
hazardous to your circuit!
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40
Complex Conjugate Pole Phase Example
From: Dorf, Richard C. Modern Control Systems. Addison-Wesley Publishing Company. Reading, Massachusetts.
Third Edition, 1981.
D l F db k d 1/ E l
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41
Dual Feedback and 1/Example
VCC 12
RF 100k
VO
VEE 12
REF02Trim
Out
Vin
Gnd
U2 REF02
VREF
Riso 26.7
CL 10u
Vout
CF 82n
-
++
U1 OPA177E
FB#1
FB#2
5V
5V
5V
Dual Feedback:
FB#1 through RF forces accurate Vout across CL
FB#2 through CF dominates at high frequency for stability
Riso provides isolation between FB#1 and FB#2
Z E t l M d l f D l F db k A l i
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VFB CF 82n
Vout
CL 10u
Riso 26.7
VREFREF02
Trim
Out
Vin
Gnd
U2 REF02
VOA
Ro 60
-
+
-
+
VCV1
VEE 12
VO
RF 100k
VCC 12
-
++
U1 OPA177Ex1
Zo External Model 4.9991V4.9991V
4.999V
4.9991V
4.999V
42
Zo External Model for Dual Feedback Analysis
Zo External Model:
VCV1 ideally isolates U1 so U1 only provides data sheet AolSet Ro to match measured Ro
Analyze with unloaded Ro (largest Ro) which creates worst instability
Use 1/on Aol stability analysis
1/, taken from VOA will include the effects of Zo, Riso and CL
D l F db k FB#1 A d FB#2
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43
Dual Feedback, FB#1 And FB#2
VFB CF 82n
Vout
CL 10u
Riso 26.7
VREFREF02
Trim
Out
Vin
Gnd
U2 REF02
VOA
Ro 60
-
+
-
+
VCV1
VEE 12
VO
RF 100k
VCC 12
-
++
U1 OPA177Ex1
Zo External Model 4.9991V4.9991V
4.999V
4.9991V
4.999V
FB#1 and FB#2 1/ Analysis:
There is only one net voltage fed back as to the -input of the op amp_net = _FB#1 + _FB#2
This implies that the largest will dominate smallest 1/ will dominate
Analyze FB#1 with CF = open since it will only dominate at high frequencies
Analyze FB#2 with CL = short since it is at least 10x CF
FB#1
FB#2
D l F db k d 1/ E l
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Dual Feedback and 1/ExampleT
Aol
FB#1 1/b
Frequency (Hz)
10m 100m 1 10 100 1k 10k 100k 1M 10M
Gain(dB)
-40
-20
0
20
40
60
80
100
120
140
160
FB#1 1/b
Aol
fza
fzx
fpc
1/b
1/bFB#11/bFB#2
Vout/Vin
fcl
D al Feedback and 1/ Create the BIG NOT
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Dual Feedback and 1/Create the BIG NOT
VCC 12
RF 100k
VO
VEE 12
-
+
-
+VCV1 Ro 60
VOA
REF02Trim
Out
Vin
Gnd
U2 REF02
VREF
Riso 26.7
CL 10u
Vout
VFBLT 1T
CT 1T
+
VG1
Vtrim
CF 220p
-
++
U1 OPA177E x1
Aol = VOA
FB#1: 1/Beta1= VOA / VFB
Loop Gain = VFB
Zo Ex ternal Model1.2298V
4.999V
4.9991V
4.999V
4.9991V
4.9991V
Dual Feedback and 1/ Create the BIG NOT
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46
Dual Feedback and 1/Create the BIG NOT
T
Aol
FB#1 1/b
Frequency (Hz)
10m 100m 1 10 100 1k 10k 100k 1M 10M
Gain(dB)
-40
-20
0
20
40
60
80
100
120
140
160
FB#1 1/b
Aol
fzafpc
1/b
1/bFB#11/bFB#2 fcl
Dual Feedback and 1/ Create the BIG NOT
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T
Aol
BIG NOT 1/
Frequency (Hz)
10m 100m 1 10 100 1k 10k 100k 1M 10M
G
ain(dB)
-40
-20
0
20
40
60
80
100
120
140
160
Aol
BIG NOT 1/
fcl
47
Dual Feedback and 1/Create the BIG NOT
STABLE???
???
BIG NOT 1/:At fcl rate-of-closure rule-of-thumb says circuit is stable but is it?
BIGNOT
Dual Feedback and 1/ Create the BIG NOT
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Dual Feedback and 1/ Create the BIG NOT
STABLE???
???
BIG NOT Loop Gain:
Loop Gainphase shift >135 degrees (
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Dual Feedback and 1/Create the BIG NOT
VCC 12
RF 100k
VO
VEE 12
-
+
-
+
VCV1 Ro 60
VOA
REF02Trim
Out
Vin
Gnd
U2 REF02
VREF
Riso 26.7
CL 10u
Vout
VFB
Vtrim
CF 220p
+
Vin-
++
U1 OPA177E
x1
DC=0V
Transient=10mVpp
f =100Hz, 10ns rise/f all
Zo External Model1.2298V
4.999V
4.9991V
4.999V
4.9991V
4.9991V
Dual Feedback and 1/ Create the BIG NOT
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Dual Feedback and 1/Create the BIG NOTT
Time (s)
0.00 2.50m 5.00m 7.50m 10.00m
VO
4.34
5.38
VOA
3.04
6.10
Vin
-100.00m
100.00m
Vout
4.76
5.17STABLE
BIG NOT Transient Stability Test:
Excessive ringing and marginal stability are apparent. Real world implementation and
use may cause even more severe oscillations. We do not want this in production!
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4) Non-Loop Stability Problems
Non-Loop Stability
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Non Loop Stability
Loop Frequencies
RB+
PCB Traces
Supply Bypass
Ground Loops
Output Stage Oscillations
Non-Loop Stabi l i ty
Oscillations NOT predicted by Loop Gain (Aol) Analysisor
SPICE Simulations
Non Loop Stability: Loop Frequency Definitions
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Non-Loop Stability:Loop Frequency Definitions
0
20
40
60
80
100
10M1M100k10k1k100101
Frequency (Hz)
A(dB) b
VOUT/VIN
Aol
fcl
SSBW
(Small Signal BandWidth)
fGBW
fcl:
Where Loop Gain (Aol) = 1
fGBW:
Where Op Amp Aol Curve crosses 0dB
(Unity Gain Bandwidth)
Non-Loop Stability: ? Diagnostic Questions ?
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Non-Loop Stability: ? Diagnostic Questions ?
Frequency of oscillation (fosc)?
When does the oscillation occur?
Oscillates Unloaded?
Oscillates with VIN=0?
Non-Loop Stability: fosc < fGBW
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Non Loop Stability:RB+ Resistor
+
-
+
-
VIN
RF
RI
100k
100k
RB+
VOUT
+
-
+
-
VIN
RF
RI
100k
100k
RB+
49.9k
VOUT
CB+
0.01For
0.1F
fosc fGBW
oscillates unloaded? -- may or may not
oscillates with VIN=0? -- may or may not
+
-
+
-
VIN
RF
RI
100k
100k
RB+
49.9k
VOUT
+
-
VNOISE
Ib
Ib
RB+ is Ib current match resistor to
reduce Vos errors due to Ib.
RB+ can create high impedance
node acting as antenna pickup for
unwanted positive feedback.
Many Op Amps have low Ib so error is
small. Evaluate DC errors w/o RB+.
If you use RB+ bypass
it in parallel with 0.1F
capacitor.
PROBLEM
SOLUTION
SOLUTION
Non-Loop Stability: fosc < fGBW
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Non Loop Stability:PCB Traces
fosc fGBW
oscillates unloaded? -- may or may not
oscillates with VIN=0? -- may or may not
DO NOTroute high current, low impedance output traces near high
impedance input traces. Unwanted positive feedback path.
DOroute high current output traces adjacent to each other (on top of each
other in a multi-layer PCB) to form a twisted pair for EMI cancellation.
+
-
+
-
VIN
VOUT
RI RF
Rs
GND
Non-Loop Stability: fosc < fGBW
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Non Loop Stability:Supply Lines
Gain
StagePower
Stage
RL
IL
-vs
Rs
+
-
+vs
Ls
CL
Load current, IL, flows through power
supply resistance, Rs, due to PCB traceor wiring. Modulated supply voltages
appear at Op Amp Power pins.
Modulated signal couples into amplifier
which relies on supply pins as AC
Ground.
Power supply lead inductance, Ls,
interacts with a capacitive load,
CL, to form an oscillatory LC, highQ, tank circuit.
fosc fGBW
oscillates unloaded? -- no
oscillates with VIN=0? -- may or may not
PROBLEM PROBLEM
Non-Loop Stability:P S l Li D l
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Proper Supply Line Decouple
+
-
RHF
RHF
CHF
CHF
CLF
CLF
+VS
-VS
< 4 in
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Non Loop Stability:Ground Loops
+
-+
- -VS
+VS
RL
RGyRGx
RGv
RGw
RFRI
Ground
IL
VIN
VOUT
oscillates unloaded? -- no
oscillates with VIN=0? -- yes
+
-+
- -VS
+VS
RL
RFRI
RG
Star
Ground
Point
VIN
VOUT
Ground loops are created from load current
flowing through parasitic resistances. If part
of VOUT is fed back to Op Amp +input,
positive feedback and oscillations can occur.
Parasitic resistances can be made to look
like a common mode input by using a
Single-Point or Star ground connection.
SOLUTION
PROBLEM
Non-Loop Stability: fosc > fGBW
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p yOutput Stages
-VS
L
O
A
D
oscillates unloaded? -- no
oscillates with VIN=0? -- no
Some Op Amps use composite output
stages, usually on the negative output, that
contain local feedback paths. Under reactive
loads these output stages can oscillate.
The Output R-C Snubber Network lowersthe high frequency gain of the output stage
preventing unwanted oscillations under
reactive loads.
+
-
+
-
VIN
RF
RI
100k
100k
VOUT
RSN
CSN
10to 100
.F to 1FPROBLEM SOLUTION