TI SM73302MFE

SM73302
SM73302 88 MHz, Precision, Low Noise, 1.8V CMOS Input, Decompensated
Operational Amplifier
Literature Number: SNOSB93
SM73302
88 MHz, Precision, Low Noise, 1.8V CMOS Input,
Decompensated Operational Amplifier
General Description
Features
The SM73302 low noise, CMOS input operational amplifier
while
offers a low input voltage noise density of 5.8 nV/
consuming only 1.15 mA of quiescent current. The SM73302
is stable at a gain of 10 and has a gain bandwidth (GBW)
product of 88 MHz. The SM73302 has a supply voltage range
of 1.8V to 5.5V and can operate from a single supply. The
SM73302 features a rail-to-rail output stage, and is part of the
precision amplifier family and is ideal for a variety of instrumentation applications.
The SM73302 provides optimal performance in low voltage
and low noise systems. A CMOS input stage, with typical input
bias currents in the range of a few femtoamperes, and an input common mode voltage range, which includes ground,
makes the SM73302 ideal for low power sensor applications
where high speeds are needed.
The SM73302 is manufactured using National’s advanced
VIP50 process. The SM73302 is offered in a 5-Pin SOT-23
package.
(Typical 5V supply, unless otherwise noted)
■ Renewable Energy Grade
±150 µV (max)
■ Input offset voltage
5.8 nV/√Hz
■ Input referred voltage noise
100 fA
■ Input bias current
88 MHz
■ Gain bandwidth product
1.8V to 5.5V
■ Supply voltage range
1.15mA
■ Supply current
Rail-to-Rail
output
swing
■
25 mV from rail
— @ 10 kΩ load
45 mV from rail
— @ 2 kΩ load
■ Guaranteed 2.5V and 5.0V performance
0.04% @1 kHz, 600Ω
■ Total harmonic distortion
−40°C to 125°C
■ Temperature range
Applications
■
■
■
■
■
■
ADC interface
Photodiode amplifiers
Active filters and buffers
Low noise signal processing
Medical instrumentation
Sensor interface applications
Typical Application
30157769
Photodiode Transimpedance Amplifier
30157739
Input Referred Voltage Noise vs. Frequency
LMH™ is a trademark of National Semiconductor Corporation.
© 2011 National Semiconductor Corporation
301577
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SM73302 88 MHz, Precision, Low Noise, 1.8V CMOS Input, Decompensated Operational Amplifier
August 16, 2011
SM73302
Absolute Maximum Ratings (Note 1)
If Military/Aerospace specified devices are required,
please contact the National Semiconductor Sales Office/
Distributors for availability and specifications.
For soldering specifications:
see product folder at www.national.com and
www.national.com/ms/MS/MS-SOLDERING.pdf
ESD Tolerance (Note 2)
Human Body Model
Machine Model
Charge-Device Model
VIN Differential
Supply Voltage (V+ – V−)
Input/Output Pin Voltage
Storage Temperature Range
Junction Temperature (Note 3)
2000V
Operating Ratings
200V
Temperature Range (Note 3)
Supply Voltage (V+ – V−)
−40°C ≤ TA ≤ 125°C
1000V
±0.3V
6.0V
V+ +0.3V, V− −0.3V
−65°C to 150°C
+150°C
2.5V Electrical Characteristics
(Note 1)
−40°C to 125°C
2.0V to 5.5V
0°C ≤ TA ≤ 125°C
1.8V to 5.5V
Package Thermal Resistance (θJA (Note 3))
5-Pin SOT-23
180°C/W
(Note 4)
Unless otherwise specified, all limits are guaranteed for TA = 25°C, V+ = 2.5V, V− = 0V, VCM = V+/2 = VO. Boldface limits apply at
the temperature extremes.
Symbol
VOS
Parameter
Conditions
Min
Typ
Max
(Note 6) (Note 5) (Note 6)
Input Offset Voltage
±20
±180
±480
µV
−1.0
±4
μV/°C
−40°C ≤ TA ≤ 85°C
0.05
1
25
−40°C ≤ TA ≤ 125°C
0.05
1
100
.006
0.5
50
TC VOS Input Offset Voltage Temperature Drift
(Note 7, Note 9)
IB
Input Bias Current
VCM = 1.0V
(Note 8, Note 9)
IOS
Input Offset Current
VCM = 1.0V
(Note 9)
CMRR
Common Mode Rejection Ratio
0V ≤ VCM ≤ 1.4V
83
80
94
PSRR
Power Supply Rejection Ratio
2.0V ≤ V+ ≤ 5.5V, VCM = 0V
85
80
100
1.8V ≤ V+ ≤ 5.5V, VCM = 0V
85
98
CMVR
Common Mode Voltage Range
CMRR ≥ 60 dB
Open Loop Voltage Gain
VOUT = 0.15V to 2.2V,
RL = 2 kΩ to V+/2
VOUT = 0.15V to 2.2V,
RL = 10 kΩ to V+/2
VOUT
Output Voltage Swing High
Output Voltage Swing Low
IOUT
Output Current
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pA
dB
1.5
1.5
88
82
98
92
88
110
25
70
77
RL = 10 kΩ to V+/2
20
60
66
RL = 2 kΩ to V+/2
30
70
73
RL = 10 kΩ to V+/2
15
60
62
Sourcing to V−
VIN = 200 mV (Note 10)
36
30
47
Sinking to V+
VIN = –200 mV (Note 10)
7.5
5
15
V
dB
RL = 2 kΩ to V+/2
2
pA
dB
−0.3
−0.3
CMRR ≥ 55 dB
AVOL
Units
mV from
either rail
mA
Parameter
IS
Supply Current
SR
Slew Rate
Conditions
Min
Typ
Max
(Note 6) (Note 5) (Note 6)
0.95
AV = +10, Rising (10% to 90%)
32
AV = +10, Falling (90% to 10%)
24
1.30
1.65
Units
mA
V/μs
GBW
Gain Bandwidth
AV = +10, RL = 10 kΩ
88
en
Input Referred Voltage Noise Density
f = 1 kHz
6.2
nV/
in
Input Referred Current Noise Density
f = 1 kHz
0.01
pA/
f = 1 kHz, AV = 1, RL = 600Ω
0.01
THD+N Total Harmonic Distortion + Noise
5V Electrical Characteristics
MHz
%
(Note 4)
Unless otherwise specified, all limits are guaranteed for TA = 25°C, V+ = 5V, V− = 0V, VCM = V+/2 = VO. Boldface limits apply at
the temperature extremes.
Symbol
VOS
Parameter
Conditions
Min
Typ
Max
(Note 6) (Note 5) (Note 6)
Input Offset Voltage
±10
±150
±450
µV
−1.0
±4
μV/°C
−40°C ≤ TA ≤ 85°C
0.1
1
25
−40°C ≤ TA ≤ 125°C
0.1
1
100
.01
0.5
50
TC VOS Input Offset Voltage Temperature Drift
(Note 7, Note 9)
IB
Input Bias Current
VCM = 2.0V
(Note 8, Note 9)
IOS
Input Offset Current
VCM = 2.0V
(Note 9)
CMRR
Common Mode Rejection Ratio
0V ≤ VCM ≤ 3.7V
85
80
100
PSRR
Power Supply Rejection Ratio
2.0V ≤ V+ ≤ 5.5V, VCM = 0V
85
80
100
1.8V ≤ V+ ≤ 5.5V, VCM = 0V
85
98
CMVR
Common Mode Voltage Range
CMRR ≥ 60 dB
Open Loop Voltage Gain
VOUT = 0.3V to 4.7V,
RL = 2 kΩ to V+/2
VOUT = 0.3V to 4.7V,
RL = 10 kΩ to V+/2
VOUT
Output Voltage Swing High
Output Voltage Swing Low
107
92
88
110
IS
Output Short Circuit Current
dB
35
70
77
RL = 10 kΩ to V+/2
25
60
66
42
70
73
25
60
66
RL = 10 kΩ to V+/2
IOUT
V
RL = 2 kΩ to V+/2
RL = 2 kΩ to
Sourcing to V−
VIN = 200 mV (Note 10)
46
38
60
Sinking to V+
VIN = –200 mV (Note 10)
10.5
6.5
21
Supply Current
1.15
3
pA
dB
4
4
88
82
V+/2
pA
dB
−0.3
−0.3
CMRR ≥ 55 dB
AVOL
Units
mV from
either rail
mA
1.40
1.75
mA
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SM73302
Symbol
SM73302
Symbol
SR
Parameter
Slew Rate
Conditions
Min
Typ
Max
(Note 6) (Note 5) (Note 6)
AV = +10, Rising (10% to 90%)
35
AV = +10, Falling (90% to 10%)
28
Units
V/μs
GBW
Gain Bandwidth
AV = +10, RL = 10 kΩ
88
en
Input Referred Voltage Noise Density
f = 1 kHz
5.8
nV/
in
Input Referred Current Noise Density
f = 1 kHz
0.01
pA/
f = 1 kHz, AV = 1, RL = 600Ω
0.01
THD+N Total Harmonic Distortion + Noise
MHz
%
Note 1: Absolute Maximum Ratings indicate limits beyond which damage to the device may occur. Operating Ratings indicate conditions for which the device is
intended to be functional, but specific performance is not guaranteed. For guaranteed specifications and the test conditions, see the Electrical Characteristics
Tables.
Note 2: Human Body Model, applicable std. MIL-STD-883, Method 3015.7. Machine Model, applicable std. JESD22-A115-A (ESD MM std. of JEDEC)
Field-Induced Charge-Device Model, applicable std. JESD22-C101-C (ESD FICDM std. of JEDEC).
Note 3: The maximum power dissipation is a function of TJ(MAX), θJA. The maximum allowable power dissipation at any ambient temperature is
PD = (TJ(MAX) - TA)/θJA. All numbers apply for packages soldered directly onto a PC Board.
Note 4: Electrical Table values apply only for factory testing conditions at the temperature indicated. Factory testing conditions result in very limited self-heating
of the device such that TJ = TA. No guarantee of parametric performance is indicated in the electrical tables under conditions of internal self-heating where TJ >
TA.
Note 5: Typical values represent the most likely parametric norm as determined at the time of characterization. Actual typical values may vary over time and will
also depend on the application and configuration. The typical values are not tested and are not guaranteed on shipped production material.
Note 6: Limits are 100% production tested at 25°C. Limits over the operating temperature range are guaranteed through correlations using the statistical quality
control (SQC) method.
Note 7: Offset voltage average drift is determined by dividing the change in VOS by temperature change.
Note 8: Positive current corresponds to current flowing into the device.
Note 9: Parameter is guaranteed by design and/or characterization and is not test in production.
Note 10: The short circuit test is a momentary test, the short circuit duration is 1.5 ms.
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SM73302
Connection Diagram
5-Pin SOT-23
30157701
Top View
Ordering Information
Package
Part Number
5-Pin SOT-23
SM73302MFE
Package Marking
Transport Media
SC3B
250 Units Tape and Reel
SM73302MF
NSC Drawing
1k Units Tape and Reel
SM73302MFX
MF05A
3k Units Tape and Reel
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SM73302
Typical Performance Characteristics
Unless otherwise specified, TA = 25°C, V– = 0, V+ = 5V,
VS = V+ - V−, VCM = VS/2.
TCVOS Distribution
Offset Voltage Distribution
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30157791
TCVOS Distribution
Offset Voltage Distribution
30157793
30157792
Supply Current vs. Supply Voltage
Offset Voltage vs. VCM
30157705
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30157709
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SM73302
Offset Voltage vs. VCM
Offset Voltage vs. VCM
30157711
30157751
Offset Voltage vs. Temperature
Slew Rate vs. Supply Voltage
30157752
30157712
Input Bias Current Over Temperature
Input Bias Current vs. VCM
30157762
30157787
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SM73302
Offset Voltage vs. Supply Voltage
Sourcing Current vs. Supply Voltage
30157727
30157720
Sinking Current vs. Supply Voltage
Sourcing Current vs. Output Voltage
30157750
30157719
Sinking Current vs. Output Voltage
Positive Output Swing vs. Supply Voltage
30157717
30157754
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Positive Output Swing vs. Supply Voltage
30157715
30157716
Negative Output Swing vs. Supply Voltage
Positive Output Swing vs. Supply Voltage
30157714
30157718
Negative Output Swing vs. Supply Voltage
Input Referred Voltage Noise vs. Frequency
30157739
30157713
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SM73302
Negative Output Swing vs. Supply Voltage
SM73302
Time Domain Voltage Noise
Overshoot and Undershoot vs. CLOAD
30157781
30157730
THD+N vs. Frequency
THD+N vs. Frequency
30157704
30157726
THD+N vs. Peak-to-Peak Output Voltage (VOUT)
THD+N vs. Peak-to-Peak Output Voltage (VOUT)
30157774
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30157775
10
Closed Loop Output Impedance vs. Frequency
30157732
30157706
Crosstalk Rejection
Small Signal Transient Response, AV = +10
30157753
30157780
Large Signal Transient Response, AV = +10
Small Signal Transient Response, AV = +10
30157755
30157757
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SM73302
Open Loop Gain and Phase
SM73302
Large Signal Transient Response, AV = +10
PSRR vs. Frequency
30157763
30157770
CMRR vs. Frequency
Input Common Mode Capacitance vs. VCM
30157756
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30157776
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Advantages of Decompensated Op Amp
A unity gain stable op amp, which is fully compensated, is
designed to operate with good stability down to gains of ±1.
The large amount of compensation does provide an op amp
that is relatively easy to use; however, a decompensated op
amp is designed to maximize the bandwidth and slew rate
without any additional power consumption. This can be very
advantageous.
The SM73302 requires a gain of ±10 to be stable. However,
with an external compensation network (a simple RC network) these parts can be stable with gains of ±1 and still
maintain the higher slew rate. Looking at the Bode plots for
the SM73302 and its closest equivalent unity gain stable op
amp, the LMP7715, one can clearly see the increased bandwidth of the SM73302. Both plots are taken with a parallel
combination of 20 pF and 10 kΩ for the output load.
ADVANTAGES OF THE SM73302
Wide Bandwidth at Low Supply Current
The SM73302 is a high performance op amp that provides a
GBW of 88 MHz with a gain of 10 while drawing a low supply
current of 1.15 mA. This makes it ideal for providing wideband
amplification in data acquisition applications.
With the proper external compensation, the SM73302 can be
operated at gains of ±1 and still maintain much faster slew
rates than comparable unity gain stable amplifiers. The increase in bandwidth and slew rate is obtained without any
additional power consumption over the LMP7715.
Low Input Referred Noise and Low Input Bias Current
The SM73302 has a very low input referred voltage noise
at 1 kHz). A CMOS input stage ensures
density (5.8 nV/
a small input bias current (100 fA) and low input referred current noise (0.01 pA/
). This is very helpful in maintaining
signal integrity, and makes the SM73302 ideal for audio and
sensor based applications.
Low Supply Voltage
The SM73302 has performance guaranteed at 2.5V and 5V
supply. This part is guaranteed to be operational at all supply
voltages between 2.0V and 5.5V, for ambient temperatures
ranging from −40°C to 125°C, thus utilizing the entire battery
lifetime. The SM73302 is also guaranteed to be operational
at 1.8V supply voltage, for temperatures between 0°C and
125°C optimizing their usage in low-voltage applications.
RRO and Ground Sensing
Rail-to-Rail output (RRO) swing provides the maximum possible dynamic range. This is particularly important when operating at low supply voltages. An innovative positive
feedback scheme is used to boost the current drive capability
of the output stage. This allows the SM73302 to source more
than 40 mA of current at 1.8V supply. This also limits the performance of this part as a comparator, and hence the usage
of the SM73302 in an open-loop configuration is not recommended. The input common-mode range includes the negative supply rail which allows direct sensing at ground in single
supply operation.
30157722
FIGURE 1. SM73302 AVOL vs. Frequency
Small Size
The small footprint of the SM73302 package saves space on
printed circuit boards, and enables the design of smaller electronic products, such as cellular phones, pagers, or other
portable systems. Long traces between the signal source and
the op amp make the signal path more susceptible to noise
pick up.
The physically smaller SM73302 allows the op amp to be
placed closer to the signal source, thus reducing noise pickup
and maintaining signal integrity.
30157723
FIGURE 2. LMP7715 AVOL vs. Frequency
Figure 1 shows the much larger 88 MHz bandwidth of the
SM73302 as compared to the 17 MHz bandwidth of the
LMP7715 shown in Figure 2. The decompensated SM73302
has five times the bandwidth of the LMP7715.
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SM73302
USING THE DECOMPENSATED SM73302
Application Information
SM73302
unity gain op amp. Figure 4 shows the lead-lag configuration.
Only RC and C are added for the necessary compensation.
What is a Decompensated Op Amp?
The differences between the unity gain stable op amp and the
decompensated op amp are shown in Figure 3. This Bode plot
assumes an ideal two pole system. The dominant pole of the
decompensated op amp is at a higher frequency, f1, as compared to the unity gain stable op amp which is at fd as shown
in Figure 3. This is done in order to increase the speed capability of the op amp while maintaining the same power dissipation of the unity gain stable op amp. The SM73302 has a
dominant pole at 1.6 kHz. The unity gain stable LMP7715/
LMP7716 have their dominant pole at 300 Hz.
30157725
FIGURE 4. SM73302 with Lead-Lag Compensation for
Inverting Configuration
To cover how to calculate the compensation network values
it is necessary to introduce the term called the feedback factor
or F. The feedback factor F is the feedback voltage VA-VB
across the op amp input terminals relative to the op amp output voltage VOUT.
30157724
From feedback theory the classic form of the feedback equation for op amps is:
FIGURE 3. Open Loop Gain for Unity Gain Stable Op Amp
and Decompensated Op Amp
Having a higher frequency for the dominate pole will result in:
1. The DC open loop gain (AVOL) extending to a higher
frequency.
2. A wider closed loop bandwidth.
3. Better slew rate due to reduced compensation
capacitance within the op amp.
The second open loop pole (f2) for the SM73302 occurs at 45
MHz. The unity gain (fu’) occurs after the second pole at 51
MHz. An ideal two pole system would give a phase margin of
45° at the location of the second pole. The SM73302 has parasitic poles close to the second pole, giving a phase margin
closer to 0°. Therefore it is necessary to operate the SM73302
at a closed loop gain of 10 or higher, or to add external compensation in order to assure stability.
For the LMP7715, the gain bandwidth product occurs at 17
MHz. The curve is constant from fd to fu which occurs before
the second pole.
For the SM73302 the GBW = 88 MHz and is constant between
f1 and f2. The second pole at f2 occurs before AVOL =1. Therefore fu’ occurs at 51 MHz, well before the GBW frequency of
88 MHz. For decompensated op amps the unity gain frequency and the GBW are no longer equal. Gmin is the minimum
gain for stability and for the SM73302 this is a gain of 18 to
20 dB.
A is the open loop gain of the amplifier and AF is the loop gain.
Both are highly important in analyzing op amps. Normally AF
>>1 and so the above equation reduces to:
Deriving the equations for the lead-lag compensation is beyond the scope of this datasheet. The derivation is based on
the feedback equations that have just been covered. The inverse of feedback factor for the circuit in Figure 4 is:
(1)
where 1/F's pole is located at
(2)
1/F's zero is located at
Input Lead-Lag Compensation
The recommended technique which allows the user to compensate the SM73302 for stable operation at any gain is leadlag compensation. The compensation components added to
the circuit allow the user to shape the feedback function to
make sure there is sufficient phase margin when the loop gain
is as low as 0 dB and still maintain the advantages over the
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(3)
14
SM73302
(4)
The circuit gain for Figure 4 at low frequencies is −RF/RIN, but
F, the feedback factor is not equal to the circuit gain. The
feedback factor is derived from feedback theory and is the
same for both inverting and non-inverting configurations. Yes,
the feedback factor at low frequencies is equal to the gain for
the non-inverting configuration.
(5)
From this formula, we can see that
• 1/F's zero is located at a lower frequency compared with
1/F's pole.
• 1/F's value at low frequency is 1 + RF/RIN.
• This method creates one additional pole and one
additional zero.
• This pole-zero pair will serve two purposes:
— To raise the 1/F value at higher frequencies prior to its
intercept with A, the open loop gain curve, in order to
meet the Gmin = 10 requirement. For the SM73302
some overcompensation will be necessary for good
stability.
— To achieve the previous purpose above with no
additional loop phase delay.
Please note the constraint 1/F ≥ Gmin needs to be satisfied
only in the vicinity where the open loop gain A and 1/F intersect; 1/F can be shaped elsewhere as needed. The 1/F pole
must occur before the intersection with the open loop gain A.
In order to have adequate phase margin, it is desirable to follow these two rules:
Rule 1 1/F and the open loop gain A should intersect at the
frequency where there is a minimum of 45° of phase
margin. When over-compensation is required the intersection point of A and 1/F is set at a frequency
where the phase margin is above 45°, therefore increasing the stability of the circuit.
Rule 2 1/F’s pole should be set at least one decade below
the intersection with the open loop gain A in order to
take advantage of the full 90° of phase lead brought
by 1/F’s pole which is F’s zero. This ensures that the
effect of the zero is fully neutralized when the 1/F and
A plots intersect each other.
30157748
FIGURE 5. SM73302 Simplified Bode Plot
To obtain stable operation with gains under 10 V/V the open
loop gain margin must be reduced at high frequencies to
where there is a 45° phase margin when the gain margin of
the circuit with the external compensation is 0 dB. The pole
and zero in F, the feedback factor, control the gain margin at
the higher frequencies. The distance between F and AVOL is
the gain margin; therefore, the unity gain point (0 dB) is where
F crosses the AVOL curve.
For the example being used RIN = RF for a gain of −1. Therefore F = 6 dB at low frequencies. At the higher frequencies
the minimum value for F is 18 dB for 45° phase margin. From
Equation 5 we have the following relationship:
Now set RF = RIN = R. With these values and solving for RC
we have RC = R/5.9. Note that the value of C does not affect
the ratio between the resistors. Once the value of the resistors
is set, then the position of the pole in F must be set. A 2 kΩ
resistor is used for RF and RIN in this design. Therefore the
value for RC is set at 330Ω, the closest standard value for 2
kΩ/5.9.
Rewriting Equation 2 to solve for the minimum capacitor value
gives the following equation:
Calculating Lead-Lag Compensation for SM73302
Figure 5 is the same plot as Figure 1, but the AVOL and phase
curves have been redrawn as smooth lines to more readily
show the concepts covered, and to clearly show the key parameters used in the calculations for lead-lag compensation.
C = 1/(2πfpRC)
The feedback factor curve, F, intersects the AVOL curve at
about 12 MHz. Therefore the pole of F should not be any
larger than 1.2 MHz. Using this value and RC = 330Ω the
minimum value for C is 390 pF. Figure 6 shows that there is
too much overshoot, but the part is stable. Increasing C to 2.2
nF did not improve the ringing, as shown in Figure 7.
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SM73302
30157703
30157708
FIGURE 8. RC = 240Ω and C = 390 pF, Gain = −1
FIGURE 6. First Try at Compensation, Gain = −1
30157707
30157710
FIGURE 7. C Increased to 2.2 nF, Gain = −1
FIGURE 9. RC = 240Ω and C = 2.2 nF, Gain = −1
Some over-compensation appears to be needed for the desired overshoot characteristics. Instead of intersecting the
AVOL curve at 18 dB, 2 dB of over-compensation will be used,
and the AVOL curve will be intersected at 20 dB. Using Equation 5 for 20 dB, or 10 V/V, the closest standard value of RC
is 240Ω. The following two waveforms show the new resistor
value with C = 390 pF and 2.2 nF. Figure 9 shows the final
compensation and a very good response for the 1 MHz
square wave.
To summarize, the following steps were taken to compensate
the SM73302 for a gain of −1:
1. Values for Rc and C were calculated from the Bode plot
to give an expected phase margin of 45°. The values
were based on RIN = RF = 2 kΩ. These calculations gave
Rc = 330Ω and C = 390 pF.
2. To reduce the ringing C was increased to 2.2 nF which
moved the pole of F, the feedback factor, farther away
from the AVOL curve.
3. There was still too much ringing so 2 dB of overcompensation was added to F. This was done by
decreasing RC to 240Ω.
The LMP7715 is the fully compensated part (without the Renewable Energy Grade), which is comparable to the
SM73302 . Using the LMP7715 in the same setup, but removing the compensation network, provided the response
shown in Figure 10 .
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30157721
FIGURE 10. LMP7715 Response
For large signal response the rise and fall times are dominated by the slew rate of the op amps. Even though both parts
are quite similar the SM73302 will give rise and fall times
about 2.5 times faster than the LMP7715. This is possible
because the SM73302 is a decompensated op amp and even
though it is being used at a gain of −1, the speed is preserved
by using a good technique for external compensation.
30157782
FIGURE 11. RC = 240Ω and C = 2.2 nF, Gain = +2
30157783
FIGURE 12. LMP7715 Response Gain = +2
The response shown in Figure 11 is close to the response
shown in Figure 9. The part is actually slightly faster in the
non-inverting configuration. Decreasing the value of RC to
around 200Ω can decrease the negative overshoot but will
have slightly longer rise and fall times. The other option is to
add a small resistor in series with the input signal. Figure 12
shows the performance of the LMP7715 with no compensation. Again the decompensated parts are almost 2.5 times
faster than the fully compensated op amp.
The most difficult op amp configuration to stabilize is the gain
of +1. With proper compensation the SM73302 can be used
in this configuration and still maintain higher speeds than the
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SM73302
Non-Inverting Compensation
For the non-inverting amp the same theory applies for establishing the needed compensation. When setting the inverting
configuration for a gain of −1, F has a value of 2. For the noninverting configuration both F and the actual gain are the
same, making the non-inverting configuration more difficult to
compensate. Using the same circuit as shown in Figure 4, but
setting up the circuit for non-inverting operation (gain of +2)
results in similar performance as the inverting configuration
with the inputs set to half the amplitude to compensate for the
additional gain. Figure 11 below shows the results.
SM73302
fully compensated parts. Figure 13 shows the gain = 1, or the
buffer configuration, for these parts.
30157784
FIGURE 13. SM73302 with Lead-Lag Compensation for
Non-Inverting Configuration
30157789
Figure 13 is the result of using Equation 5 and additional experimentation in the lab. RP is not part of Equation 5, but it is
necessary to introduce another pole at the input stage for
good performance at gain = +1. Equation 5 is shown below
with RIN = ∞.
FIGURE 15. LMP7715 Response Gain = +1
With no increase in power consumption the decompensated
op amp offers faster speed than the compensated equivalent
part . These examples used RF = 2 kΩ. This value is high
enough to be easily driven by the SM73302, yet small enough
to minimize the effects from the parasitic capacitance of both
the PCB and the op amp.
Note: When using the SM73302, proper high frequency PCB
layout must be followed. The GBW of these parts is 88 MHz,
making the PCB layout significantly more critical than when
using the compensated counterparts which have a GBW of
17 MHz.
Using 2 kΩ for RF and solving for RC gives RC = 2000/6.9 =
290Ω. The closest standard value for RC is 300Ω. After some
fine tuning in the lab RC = 330Ω and RP = 1.5 kΩ were chosen
as the optimum values. RP together with the input capacitance
at the non-inverting pin inserts another pole into the compensation for the SM73302. Adding this pole and slightly reducing
the compensation for 1/F (using a slightly higher resistor value
for RC) gives the optimum response for a gain of +1. Figure
14 is the response of the circuit shown in Figure 13. Figure
15 shows the response of the LMP7715 in the buffer configuration with no compensation and RP = RF = 0.
TRANSIMPEDANCE AMPLIFIER
An excellent application for the SM73302 is as a transimpedance amplifier. With a GBW product of 88 MHz this
part is ideal for high speed data transmission by light. The
circuit shown on the front page of the datasheet is the circuit
used to test the SM73302 as a transimpedance amplifier. The
only change is that VB is tied to the VCC of the part, thus the
direction of the diode is reversed from the circuit shown on
the front page.
Very high speed components were used in testing to check
the limits of the SM73302 in a transimpedance configuration.
The photodiode part number is PIN-HR040 from OSI Optoelectronics. The diode capacitance for this part is only about
7 pF for the 2.5V bias used (VCC to virtual ground). The rise
time for this diode is 1 nsec. A laser diode was used for the
light source. Laser diodes have on and off times under 5 nsec.
The speed of the selected optical components allowed an accurate evaluation of the SM73302 as a transimpedance amplifier. Nationals evaluation board for decompensated op
amps, PN 551013271-001 A, was used and only minor modifications were necessary and no traces had to be cut.
30157788
FIGURE 14. RC = 330Ω and C = 10 nF, Gain = +1
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18
To attain maximum bandwidth and still have good stability the
pole is to be located on the open loop gain curve which is A.
If additional compensation is required one can always increase the value of CF, but this will also reduce the bandwidth
of the circuit. Therefore A = 1/F, or AF = 1. For A the equation
is:
30157761
FIGURE 16. Transimpedance Amplifier
Figure 16 is the complete schematic for a transimpedance
amplifier. Only the supply bypass capacitors are not shown.
CD represents the photodiode capacitance which is given on
its datasheet. CCM is the input common mode capacitance of
the op amp and, for the SM73302 it is shown in the last graph
of the Typical Performance Characteristics section of this
datasheet. In Figure 16 the inverting input pin of the SM73302
is kept at virtual ground. Even though the diode is connected
to the 2.5V line, a power supply line is AC ground, thus CD is
connected to ground.
Figure 17 shows the schematic needed to derive F, the feedback factor, for a transimpedance amplifier. In this figure
CD + CCM = CIN. Therefore it is critical that the designer knows
the diode capacitance and the op amp input capacitance. The
photodiode is close to an ideal current source once its capacitance is included in the model. What kind of circuit is this?
Without CF there is only an input capacitor and a feedback
resistor. This circuit is a differentiator! Remember, differentiator circuits are inherently unstable and must be compensated. In this case CF compensates the circuit.
The expression fGBW is the gain bandwidth product of the part.
For a unity gain stable part this is the frequency where A = 1.
For the SM73302 fGBW = 88 MHz. Multiplying A and F results
in the following equation:
For the above equation s = jω. To find the actual amplitude of
the equation the square root of the square of the real and
imaginary parts are calculated. At the intersection of F and A,
we have:
30157764
FIGURE 17. Transimpedance Feedback Model
Using feedback theory, F = VA/VOUT, this becomes a voltage
divider giving the following equation:
The noise gain is 1/F. Because this is a differentiator circuit,
a zero must be inserted. The location of the zero is given by:
19
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SM73302
CF has been added for stability. The addition of this part adds
a pole to the circuit. The pole is located at:
SM73302
After a bit of algebraic manipulation the above equation reduces to:
In the above equation the only unknown is CF. In trying to
solve this equation the fourth power of CF must be dealt with.
An excel spread sheet with this equation can be used and all
the known values entered. Then through iteration, the value
of CF when both sides are equal will be found. That is the
correct value for CF and of course the closest standard value
is used for CF.
Before moving to the lab, the transfer function of the transimpedance amplifier must be found and the units must be in
Ohms.
30157795
FIGURE 19. Rise Time
In Figure 18 the ringing and the hump during the on time is
from the laser. The higher drive levels for the laser gave ringing in the light source as well as light changing from the
thermal characteristics. The hump is due to the thermal characteristics.
Solving for CF using a 100 kΩ feedback resistor, the calculated value is 0.54 pF. One of the problems with more gain is
the very small value for CF. A 0.5 pF capacitor was used, its
measured value being 0.64 pF. For the 0.64 pF location the
pole is at 2.5 MHz. Figure 20 shows the response for a 1V
output.
The SM73302 was evaluated for RF = 10 kΩ and 100 kΩ,
representing a somewhat lower gain configuration and with
the 100 kΩ feedback resistor a fairly high gain configuration.
The RF = 10 kΩ is covered first. Looking at the Input Common
Mode Capacitance vs. VCM chart for CCM for the operating
point selected CCM = 15 pF. Note that for split supplies VCM =
2.5V, CIN = 22 pF and fGBW = 88 MHz. Solving for CF the calculated value is 1.75 pF, so 1.8 pF is selected for use.
Checking the frequency of the pole finds that it is at 8.8 MHz,
which is right at the minimum gain recommended for this part.
Some over compensation was necessary for stability and the
final selected value for CF is 2.7 pF. This moves the pole to
5.9 MHz. Figure 18 and Figure 19 show the rise and fall times
obtained in the lab with a 1V output swing. The laser diode
was difficult to drive due to thermal effects making the starting
and ending point of the pulse quite different, therefore the two
separate scope pictures.
30157796
FIGURE 20. High Gain Response
A transimpedance amplifier is an excellent application for the
SM73302. Even with the high gain using a 100 kΩ feedback
resistor, the bandwidth is still well over 1 MHz. Other than a
little over compensation for the 10 kΩ feedback resistor configuration using the SM73302 was quite easy. Of course a
very good board layout was also used for this test.
30157794
FIGURE 18. Fall Time
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20
SM73302
Physical Dimensions inches (millimeters) unless otherwise noted
5-Pin SOT23
NS Package Number MF05A
21
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SM73302 88 MHz, Precision, Low Noise, 1.8V CMOS Input, Decompensated Operational Amplifier
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