NSC LMV796MFX 17 mhz, low noise, cmos input, 1.8v operational amplifier Datasheet

LMV796/LMV797
17 MHz, Low Noise, CMOS Input, 1.8V Operational
Amplifiers
General Description
Features
The LMV796 (Single) and the LMV797 (Dual) low noise,
CMOS input operational amplifiers offer a low input voltage
while consuming only 1.15 mA
noise density of 5.8 nV/
(LMV796) of quiescent current. The LMV796 and LMV797
are unity gain stable op amps and have gain bandwidth of 17
MHz. The LMV796/ LMV797 have a supply voltage range of
1.8V to 5.5V and can operate from a single supply. The
LMV796/LMV797 each feature a rail-to-rail output stage capable of driving a 600Ω load and sourcing as much as 60 mA
of current.
The LMV796 family 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, make the LMV796 and the LMV797 ideal
for low power sensor applications.
(Typical 5V supply, unless otherwise noted)
n Input referred voltage noise
5.8 nV/
n Input bias current
100 fA
n Unity gain bandwidth
17 MHz
n Supply current per channel
— LMV796
1.15 mA
— LMV797
1.30 mA
n Rail-to-rail output swing
— @ 10 kΩ load
25 mV from rail
35 mV from rail
— @ 2 kΩ load
n Guaranteed 2.5V and 5.0V performance
n Total harmonic distortion
0.01% @1 kHz, 600Ω
n Temperature range
−40˚C to 125˚C
The LMV796/LMV797 are manufactured using National’s
advanced VIP50 process and are offered in a 5-pin SOT23
and an 8-pin MSOP package respectively.
n
n
n
n
n
Applications
Photodiode amplifiers
Active filters and buffers
Low noise signal processing
Medical instrumentation
Sensor interface applications
Typical Application
20183569
Photodiode Transimpedance Amplifier
© 2006 National Semiconductor Corporation
DS201835
20183539
Input Referred Voltage Noise vs. Frequency
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LMV796/LMV797 17 MHz, Low Noise, CMOS Input, 1.8V Operational Amplifiers
May 2006
LMV796/LMV797
Absolute Maximum Ratings (Note 1)
Soldering Information
If Military/Aerospace specified devices are required,
please contact the National Semiconductor Sales Office/
Distributors for availability and specifications.
Infrared or Convection (20 sec)
235˚C
Wave Soldering Lead Temp (10
sec)
260˚C
ESD Tolerance (Note 2)
Human Body Model
2000V
Machine Model
Operating Ratings (Note 1)
200V
Temperature Range (Note 3)
± 0.3V
VIN Differential
Supply Voltage (V+ – V−)
Input/Output Pin Voltage
Storage Temperature Range
+
Supply Voltage (V – V )
−40˚C ≤ TA ≤ 125˚C
6.0V
V+ +0.3V, V− −0.3V
2.0V to 5.5V
0˚C ≤ TA ≤ 125˚C
−65˚C to 150˚C
Junction Temperature (Note 3)
−40˚C to 125˚C
−
1.8V to 5.5V
Package Thermal Resistance (θJA (Note 3))
+150˚C
5-Pin SOT23
180˚C/W
8-Pin MSOP
236˚C/W
2.5V Electrical Characteristics
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
Parameter
VOS
Input Offset Voltage
TC VOS
Input Offset Average Drift
IB
Input Bias Current
Conditions
Min
(Note 5)
Typ
(Note 4)
Max
(Note 5)
0.1
± 1.35
± 1.65
LMV796 (Note 6)
−1.0
LMV797 (Note 6)
−1.8
VCM = 1.0V
(Notes 7, 8)
0.05
1
25
−40˚C ≤ TA ≤
125˚C
0.05
1
100
Input Offset Current
(Note 8)
CMRR
Common Mode Rejection
Ratio
0V ≤ VCM ≤ 1.4V
80
75
94
PSRR
Power Supply Rejection
Ratio
2.0V ≤ V+ ≤ 5.5V, VCM = 0V
80
75
100
1.8V ≤ V+ ≤ 5.5V, VCM = 0V
80
98
CMVR
Input Common-Mode Voltage
Range
CMRR ≥ 60 dB
CMRR ≥ 55 dB
AVOL
Large Signal Voltage Gain
VOUT = 0.15V to 2.2V,
RLOAD = 2 kΩ to V+/2
10
VOUT
Output Swing High
Output Swing Low
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fA
dB
1.5
1.5
LMV796
85
80
98
LMV797
82
78
92
88
84
110
V
dB
RLOAD = 2 kΩ to V+/2
25
75
82
RLOAD = 10 kΩ to V+/2
20
65
71
RLOAD = 2 kΩ to V+/2
30
75
78
RLOAD = 10 kΩ to V+/2
15
65
67
2
pA
dB
−0.3
-0.3
VOUT = 0.15V to 2.2V,
RLOAD = 10 kΩ to V+/2
mV
µV/˚C
−40˚C ≤ TA ≤ 85˚C
IOS
Units
mV from
rail
IOUT
IS
Output Short Circuit Current
Supply Current per Amplifier
SR
Slew Rate
(Continued)
Sourcing to V−
VIN = 200 mV (Note 9)
35
28
47
Sinking to V+
VIN = –200 mV (Note 9)
7
5
15
mA
LMV796
0.95
1.30
1.65
LMV797
per channel
1.1
1.50
1.85
AV = +1, Rising (10% to 90%)
8.5
AV = +1, Falling (90% to 10%)
10.5
mA
V/µs
GBWP
Gain Bandwidth Product
14
MHz
en
Input-Referred Voltage Noise
f = 1 kHz
6.2
nV/
in
Input-Referred Current Noise
f = 1 kHz
0.01
pA/
THD+N
Total Harmonic Distortion +
Noise
f = 1 kHz, AV = 1, RLOAD = 600Ω
0.01
%
5V Electrical Characteristics
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
Parameter
VOS
Input Offset Voltage
TC VOS
Input Offset Average Drift
IB
Input Bias Current
Conditions
Min
(Note 5)
Typ
(Note 4)
Max
(Note 5)
0.1
± 1.35
± 1.65
LMV796 (Note 6)
−1.0
LMV797 (Note 6)
−1.8
VCM = 2.0V
(Notes 7, 8)
0.1
1
25
−40˚C ≤ TA ≤
125˚C
0.1
1
100
Input Offset Current
(Note 8)
CMRR
Common Mode Rejection
Ratio
0V ≤ VCM ≤ 3.7V
80
75
100
PSRR
Power Supply Rejection
Ratio
2.0V ≤ V+ ≤ 5.5V, VCM = 0V
80
75
100
1.8V ≤ V+ ≤ 5.5V, VCM = 0V
80
98
CMVR
Input Common-Mode Voltage
Range
CMRR ≥ 60 dB
CMRR ≥ 55 dB
AVOL
Large Signal Voltage Gain
VOUT = 0.3V to 4.7V,
RLOAD = 2 kΩ to V+/2
10
3
pA
fA
dB
dB
−0.3
-0.3
VOUT = 0.3V to 4.7V,
RLOAD = 10 kΩ to V+/2
mV
µV/˚C
−40˚C ≤ TA ≤ 85˚C
IOS
Units
4
4
LMV796
85
80
97
LMV797
82
78
89
88
84
110
V
dB
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LMV796/LMV797
2.5V Electrical Characteristics
LMV796/LMV797
5V Electrical Characteristics
VOUT
Output Swing High
Output Swing Low
(Continued)
RLOAD = 2 kΩ to V+/2
35
75
82
RLOAD = 10 kΩ to V+/2
25
65
71
LMV796
42
75
78
LMV797
50
80
83
20
65
67
RLOAD = 2 kΩ to V+/2
RLOAD = 10 kΩ to V+/2
IOUT
IS
Output Short Circuit Current
Supply Current per Amplifier
SR
Slew Rate
Sourcing to V−
VIN = 200 mV (Note 9)
45
37
60
Sinking to V+
VIN = –200 mV (Note 9)
10
6
21
mA
LMV796
1.15
1.40
1.75
LMV797
per channel
1.30
1.70
2.05
AV = +1, Rising (10% to 90%)
6.0
9.5
AV = +1, Falling (90% to 10%)
7.5
11.5
17
mV from
rail
mA
V/µs
GBWP
Gain Bandwidth Product
en
Input-Referred Voltage Noise
f = 1 kHz
5.8
nV/
MHz
in
Input-Referred Current Noise
f = 1 kHz
0.01
pA/
THD+N
Total Harmonic Distortion +
Noise
f = 1 kHz, AV = 1, RLOAD = 600Ω
0.01
%
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 is 1.5 kΩ in series with 100 pF. Machine Model is 0Ω in series with 200 pF
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: Typical values represent the parametric norm at the time of characterization.
Note 5: 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 6: Offset voltage average drift is determined by dividing the change in VOS by temperature change.
Note 7: Positive current corresponds to current flowing into the device.
Note 8: Input bias current and input offset current are guaranteed by design
Note 9: The short circuit test is a momentary test, the short circuit duration is 1.5 ms.
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LMV796/LMV797
Connection Diagrams
5-Pin SOT23
8-Pin MSOP
20183501
Top View
20183502
Top View
Ordering Information
Package
5-Pin SOT23
8-Pin MSOP
Part Number
LMV796MF
LMV796MFX
LMV797MM
LMV797MMX
Package Marking
Transport Media
1k Units Tape and Reel
AT3A
3k Units Tape and Reel
1k Units Tape and Reel
AU3A
3.5k Units Tape and Reel
5
NSC Drawing
MF05A
MUA08A
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LMV796/LMV797
Typical Performance Characteristics
Unless otherwise specified, TA = 25˚C, V– = 0, V+ = Supply
+
Voltage = 5V, VCM = V /2.
Supply Current vs. Supply Voltage (LMV796)
Supply Current vs. Supply Voltage (LMV797)
20183505
20183581
VOS vs. VCM
VOS vs. VCM
20183551
20183509
VOS vs. VCM
VOS vs. Supply Voltage
20183511
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20183512
6
Voltage = 5V, VCM = V+/2. (Continued)
Slew Rate vs. Supply Voltage
Input Bias Current vs. VCM
20183529
20183562
Input Bias Current vs. VCM
Sourcing Current vs. Supply Voltage
20183587
20183520
Sinking Current vs. Supply Voltage
Sourcing Current vs. Output Voltage
20183550
20183519
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LMV796/LMV797
Typical Performance Characteristics Unless otherwise specified, TA = 25˚C, V– = 0, V+ = Supply
LMV796/LMV797
Typical Performance Characteristics Unless otherwise specified, TA = 25˚C, V– = 0, V+ = Supply
Voltage = 5V, VCM = V+/2. (Continued)
Sinking Current vs. Output Voltage
Positive Output Swing vs. Supply Voltage
20183517
20183554
Negative Output Swing vs. Supply Voltage
Positive Output Swing vs. Supply Voltage
20183515
20183516
Negative Output Swing vs. Supply Voltage
Positive Output Swing vs. Supply Voltage
20183514
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20183518
8
Voltage = 5V, VCM = V+/2. (Continued)
Negative Output Swing vs. Supply Voltage
Input Referred Voltage Noise vs. Frequency
20183513
20183539
Overshoot and Undershoot vs. CLOAD
THD+N vs. Peak-to-Peak Output Voltage (VOUT)
20183526
20183530
THD+N vs. Peak-to-Peak Output Voltage (VOUT)
THD+N vs. Frequency
20183574
20183504
9
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LMV796/LMV797
Typical Performance Characteristics Unless otherwise specified, TA = 25˚C, V– = 0, V+ = Supply
LMV796/LMV797
Typical Performance Characteristics Unless otherwise specified, TA = 25˚C, V– = 0, V+ = Supply
Voltage = 5V, VCM = V+/2. (Continued)
THD+N vs. Frequency
Open Loop Gain and Phase with Capacitive Load
20183575
20183541
Open Loop Gain and Phase with Resistive Load
Closed Loop Output Impedance vs. Frequency
20183532
20183573
Crosstalk Rejection
Small Signal Transient Response, AV = +1
20183538
20183580
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Voltage = 5V, VCM = V+/2. (Continued)
Large Signal Transient Response, AV = +1
Small Signal Transient Response, AV = +1
20183537
20183533
Large Signal Transient Response, AV = +1
Phase Margin vs. Capacitive Load (Stability)
20183534
20183545
Phase Margin vs. Capacitive Load (Stability)
Positive PSRR vs. Frequency
20183546
20183527
11
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LMV796/LMV797
Typical Performance Characteristics Unless otherwise specified, TA = 25˚C, V– = 0, V+ = Supply
LMV796/LMV797
Typical Performance Characteristics Unless otherwise specified, TA = 25˚C, V– = 0, V+ = Supply
Voltage = 5V, VCM = V+/2. (Continued)
Negative PSRR vs. Frequency
CMRR vs. Frequency
20183556
20183528
Input Common Mode Capacitance vs. VCM
20183576
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ADVANTAGES OF THE LMV796/LMV797
Wide Bandwidth at Low Supply Current
The LMV796 and LMV797 are high performance op amps
that provide a unity gain bandwidth of 17 MHz while drawing
a low supply current of 1.15 mA. This makes them ideal for
providing wideband amplification in portable applications.
Low Input Referred Noise and Low Input Bias Current
The LMV796/LMV797 have a very low input referred voltage
at 1 kHz). A CMOS input stage
noise density (5.8 nV/
ensures a small input bias current (100 fA) and low input
). This is very helpful in
referred current noise (0.01 pA/
maintaining signal fidelity, and makes the LMV796 and
LMV797 ideal for audio and sensor based applications.
20183561
Low Supply Voltage
The LMV796 and the LMV797 have performance guaranteed at 2.5V and 5V supply. The LMV796 family 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 LMV796
and LMV797 are also guaranteed to be operational at 1.8V
supply voltage, for temperatures between 0˚C and 125˚C.
This makes the LMV796 family ideal for usage in low-voltage
commercial applications.
FIGURE 1. Isolation of CL to Improve Stability
INPUT CAPACITANCE AND FEEDBACK CIRCUIT
ELEMENTS
The LMV796 family has a very low input bias current (100 fA)
and a low 1/f noise corner frequency (400 Hz), which makes
it ideal for sensor applications. However, to obtain this performance a large CMOS input stage is used, which adds to
the input capacitance of the op amp, CIN. Though this does
not affect the DC and low frequency performance, at higher
frequencies the input capacitance interacts with the input
and the feedback impedances to create a pole, which results
in lower phase margin and gain peaking. This can be controlled by being selective in the use of feedback resistors, as
well as, by using a feedback capacitance, CF. For example,
in the inverting amplifier shown in Figure 2, if CIN and CF are
ignored and the open loop gain of the op amp is considered
infinite then the gain of the circuit is −R2/R1. An op amp,
however, usually has a dominant pole, which causes its gain
to drop with frequency. Hence, this gain is only valid for DC
and low frequency. To understand the effect of the input
capacitance coupled with the non-ideal gain of the op amp,
the circuit needs to be analyzed in the frequency domain
using a Laplace transform.
RRO and Ground Sensing
Rail-to-rail output swing provides maximum possible dynamic range at the output. 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 LMV796 and
the LMV797 to source more than 40 mA of current at 1.8V
supply. This also limits the performance of the LMV796
family as comparators, and hence the usage of the LMV796
and the LMV797 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.
Small Size
The small footprint of the LMV796 and the LMV797 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 susceptible to noise. By using the physically smaller
LMV796 or LMV797 package, the op amp can be placed
closer to the signal source, reducing noise pickup and increasing signal integrity.
CAPACITIVE LOAD TOLERANCE
The LMV796 and LMV797 can directly drive 120 pF in
unity-gain without oscillation. The unity-gain follower is the
most sensitive configuration to capacitive loading. Direct
capacitive loading reduces the phase margin of amplifiers.
The combination of the amplifier’s output impedance and the
capacitive load induces phase lag. This results in either an
underdamped pulse response or oscillation. To drive a
heavier capacitive load, the circuit in Figure 1 can be used.
20183564
FIGURE 2. Inverting Amplifier
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LMV796/LMV797
In Figure 1, the isolation resistor RISO and the load capacitor
CL form a pole to increase stability by adding more phase
margin to the overall system. The desired performance depends on the value of RISO. The bigger the RISO resistor
value, the more stable VOUT will be. Increased RISO would,
however, result in a reduced output swing and short circuit
current.
Application Information
LMV796/LMV797
Application Information
the circuit. Adding a capacitance of 2 pF removes the peak,
while a capacitance of 5 pF creates a much lower pole and
reduces the bandwidth excessively.
(Continued)
For simplicity, the op amp is modeled as an ideal integrator
with a unity gain frequency of A0 . Hence, its transfer function
(or gain) in the frequency domain is A0/s. Solving the circuit
equations in the frequency domain, ignoring CF for the moment, results in an expression for the gain shown in Equation
(1).
(1)
It can be inferred from the denominator of the transfer function that it has two poles, whose expressions can be obtained by solving for the roots of the denominator and are
shown in Equation (2).
20183560
FIGURE 4. Gain Peaking Eliminated by CF
(2)
Equation (2) shows that as the values of R1 and R2 are
increased, the magnitude of the poles, and hence the bandwidth of the amplifier, is reduced. This theory is verified by
using different values of R1 and R2 in the circuit shown in
Figure 1 and by comparing their frequency responses. In
Figure 3 the frequency responses for three different values
of R1 and R2 are shown. When both R1 and R2 are 1 kΩ, the
response is flattest and widest; whereas, it narrows and
peaks significantly when both their values are changed to
10 kΩ or 30 kΩ. So it is advisable to use lower values of R1
and R2 to obtain a wider and flatter response. Lower resistances also help in high sensitivity circuits since they add
less noise.
AUDIO PREAMPLIFIER WITH BAND PASS FILTERING
With low input referred voltage noise, low supply voltage and
current, and a low harmonic distortion, the LMV796 family is
ideal for audio applications. Its wide unity gain bandwidth
allows it to provide large gain for a wide range of frequencies
and it can be used to design a preamplifier to drive a load of
as low as 600Ω with less than 0.01% distortion. Two amplifier circuits are shown in Figure 5 and Figure 6. Figure 5 is
an inverting amplifier, with a 10 kΩ feedback resistor, R2,
and a 1kΩ input resistor, R1, and hence provides a gain of
−10. Figure 6 is a non-inverting amplifier, using the same
values of R1and R2, and provides a gain of 11. In either of
these circuits, the coupling capacitor CC1 decides the lower
frequency at which the circuit starts providing gain, while the
feedback capacitor CF decides the frequency at which the
gain starts dropping off. Figure 7 shows the frequency response of the inverting amplifier with different values of CF.
20183559
FIGURE 3. Gain Peaking Caused by Large R1, R2
20183565
A way of reducing the gain peaking is by adding a feedback
capacitance CF in parallel with R2. This introduces another
pole in the system and prevents the formation of pairs of
complex conjugate poles which cause the gain to peak.
Figure 4 shows the effect of CF on the frequency response of
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FIGURE 5. Inverting Audio Preamplifier
14
high gain. A typical transimpedance amplifier is shown in
Figure 8. The output voltage of the amplifier is given by the
equation VOUT = −IINRF. Since the output swing of the amplifier is limited, RF should be selected such that all possible
values of IIN can be detected.
(Continued)
The LMV796/LMV797 have a large gain-bandwidth product
(17 MHz), which enables high gains at wide bandwidths. A
rail-to-rail output swing at 5.5V supply allows detection and
amplification of a wide range of input currents. A CMOS input
stage with negligible input current noise and low input voltage noise allows the LMV796/LMV797 to provide high fidelity amplification for wide bandwidths. These properties make
the LMV796/LMV797 ideal for systems requiring wide-band
transimpedance amplification.
20183566
FIGURE 6. Non-inverting Audio Preamplifier
20183569
FIGURE 8. Photodiode Transimpedance Amplifier
As mentioned earlier, the following parameters are used to
design a transimpedance amplifier: the amplifier gainbandwidth product, A0; the amplifier input capacitance, CCM;
the photodiode capacitance, CD; the transimpedance gain
required, RF; and the amplifier output swing. Once a feasible
RF is selected using the amplifier output swing, these numbers can be used to design an amplifier with the desired
transimpedance gain and a maximally flat frequency response.
20183558
FIGURE 7. Frequency Response of the Inverting Audio
Preamplifier
An essential component for obtaining a maximally flat response is the feedback capacitor, CF. The capacitance seen
at the input of the amplifier, CIN, combined with the feedback
capacitor, RF, generate a phase lag which causes gainpeaking and can destabilize the circuit. CIN is usually just the
sum of CD and CCM. The feedback capacitor CF creates a
pole, fP in the noise gain of the circuit, which neutralizes the
zero in the noise gain, fZ, created by the combination of RF
and CIN. If properly positioned, the noise gain pole created
by CF can ensure that the slope of the gain remains at 20
dB/decade till the unity gain frequency of the amplifier is
reached, thus ensuring stability. As shown in Figure 9, fP is
positioned such that it coincides with the point where the
noise gain intersects the op amp’s open loop gain. In this
case, fP is also the overall −3 dB frequency of the transimpedance amplifier. The value of CF needed to make it so is
given by Equation (3). A larger value of CF causes excessive
reduction of bandwidth, while a smaller value fails to prevent
gain peaking and instability.
TRANSIMPEDANCE AMPLIFIER
CMOS input op amps are often used in transimpedance
applications as they have an extremely high input impedance. A transimpedance amplifier converts a small input
current into a voltage. This current is usually generated by a
photodiode. The transimpedance gain, measured as the
ratio of the output voltage to the input current, is expected to
be large and wide-band. Since the circuit deals with currents
in the range of a few nA, low noise performance is essential.
The LMV796/LMV797 are CMOS input op amps providing
wide bandwidth and low noise performance, and are hence
ideal for transimpedance applications.
Usually, a transimpedance amplifier is designed on the basis
of the current source driving the input. A photodiode is a very
common capacitive current source, which requires transimpedance gain for transforming its miniscule current into easily detectable voltages. The photodiode and the amplifier’s
gain are selected with respect to the speed and accuracy
required of the circuit. A faster circuit would require a photodiode with lesser capacitance and a faster amplifier. A more
sensitive circuit would require a sensitive photodiode and a
15
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LMV796/LMV797
Application Information
LMV796/LMV797
Application Information
formula in Equation (3), since the parasitic capacitance of
the board and the feedback resistor RF had to be accounted
for.
(Continued)
TABLE 1.
(3)
Transimpedance, ATI
CIN
CF
−3 dB Frequency
470000
50 pF 1.5 pF
350 kHz
470000
100 pF 2.0 pF
250 kHz
470000
200 pF 3.0 pF
150 kHz
47000
50 pF 4.5 pF
1.5 MHz
47000
100 pF 6.0 pF
1 MHz
47000
200 pF 9.0 pF
700 kHz
20183584
FIGURE 9. CF Selection for Stability
Calculating CF from Equation (3) can sometimes return unreasonably small values ( < 1 pF), especially for high speed
applications. In these cases, it is often more practical to use
the circuit shown in Figure 10 in order to allow more reasonable values. In this circuit, the capacitance CF' is (1+ RB/RA)
times the effective feedback capacitance, CF. A larger capacitor can now be used in this circuit to obtain a smaller
effective capacitance.
For example, if a CF of 0.5 pF is needed, while only a 5 pF
capacitor is available, RB and RA can be selected such that
RB/RA = 9. This would convert a CF' of 5 pF into a CF of
0.5 pF. This relationship holds as long as RA << RF.
20183577
FIGURE 11. Frequency Response for ATI = 470000
20183571
20183578
FIGURE 10. Obtaining Small CF from Large CF'
FIGURE 12. Frequency Response for ATI = 47000
LMV796 AS A TRANSIMPEDANCE AMPLIFIER
The LMV796 was used in the designs for a number of
amplifiers with varying transimpedance gains and source
capacitances. The gains, bandwidths and feedback capacitances of the circuits created are summarized in Table 1. The
frequency responses are presented in Figure 11 and Figure
12. The feedback capacitances are slightly different from the
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HIGH GAIN WIDEBAND TRANSIMPEDANCE
AMPLIFIER USING THE LMV797
The LMV797 dual, low noise, wide bandwidth, CMOS input
op amp IC can be used for compact, robust and integrated
solutions for sensing and amplifying wide-band signals obtained from sensitive photodiodes. One of the two op amps
available can be used to obtain transimpedance gain while
16
(Continued)
SENSOR INTERFACES
the other can be used for amplifying the output voltage to
further enhance the transimpedance gain. The wide bandwidth of the op amps (17 MHz) ensures that they are capable
of providing high gain for a wide range of frequencies. The
) allows the amplifier to
low input referred noise (5.8 nV/
deliver an output with a high SNR (signal to noise ratio). The
small 8-pin MSOP footprint saves space on printed circuit
boards and allows ease of design in portable products.
The circuit shown in Figure 13, has the first op amp acting as
a transimpedance amplifier with a gain of 47000, while the
second stage provides a voltage gain of 10. This provides a
total transimpedance gain of 470000 with a −3 dB bandwidth
of about 1.5 MHz, for a total input capacitance of 50 pF. The
frequency response for the circuit is shown in Figure 14
The low input bias current and low input referred noise of the
LMV796 and LMV797 make them ideal for sensor interfaces.
These circuits are required to sense voltages of the order of
a few µV and currents amounting to less than a nA hence,
the op amp needs to have low voltage noise and low input
bias current. Typical applications include infra-red (IR) thermometry, thermocouple amplifiers and pH electrode buffers.
Figure 15 is an example of a typical circuit used for measuring IR radiation intensity, often used for estimating the temperature of an object from a distance. The IR sensor generates a voltage proportional to I, which is the intensity of the
IR radiation falling on it. As shown in Figure 15, K is the
constant of proportionality relating the voltage across the IR
sensor (VIN) to the radiation intensity, I. The resistances RA
and RB are selected to provide a high gain to amplify this
voltage, while CF is added to filter out the high frequency
noise.
20183586
FIGURE 13. 1.5 MHz Transimpedance Amplifier, with
ATI = 470000
20183572
FIGURE 15. IR Radiation Sensor
20183579
FIGURE 14. 1.5 MHz Transimpedance Amplifier
Frequency Response
17
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LMV796/LMV797
Application Information
LMV796/LMV797
Physical Dimensions
inches (millimeters) unless otherwise noted
5-Pin SOT23
NS Package Number MF05A
8-Pin MSOP
NS package Number MUA08A
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18
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LMV796/LMV797 17 MHz, Low Noise, CMOS Input, 1.8V Operational Amplifiers
Notes
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