TI1 H08A Lf412 low offset, low drift dual jfet input operational amplifier Datasheet

LF412
LF412 Low Offset, Low Drift Dual JFET Input Operational Amplifier
Literature Number: SNOSBH7D
LF412
Low Offset, Low Drift Dual JFET Input Operational
Amplifier
General Description
Features
These devices are low cost, high speed, JFET input operational amplifiers with very low input offset voltage and guaranteed input offset voltage drift. They require low supply
current yet maintain a large gain bandwidth product and fast
slew rate. In addition, well matched high voltage JFET input
devices provide very low input bias and offset currents. The
LF412 dual is pin compatible with the LM1558, allowing designers to immediately upgrade the overall performance of
existing designs.
These amplifiers may be used in applications such as high
speed integrators, fast D/A converters, sample and hold circuits and many other circuits requiring low input offset voltage
and drift, low input bias current, high input impedance, high
slew rate and wide bandwidth.
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Typical Connection
Connection Diagrams
Internally trimmed offset voltage: 1 mV (max)
Input offset voltage drift: 10 μV/°C (max)
Low input bias current: 50 pA
Low input noise current:
Wide gain bandwidth: 3 MHz (min)
High slew rate: 10V/μs (min)
Low supply current: 1.8 mA/Amplifier
High input impedance: 1012Ω
Low total harmonic distortion ≤0.02%
Low 1/f noise corner: 50 Hz
Fast settling time to 0.01%: 2 μs
Metal Can Package
565642
565641
Ordering Information
X
Y
Z
LF412XYZ
indicates electrical grade
indicates temperature range
“M” for military
“C” for commercial
indicates package type
“H” or “N”
Order Number LF412MH, LF412CH
See NS Package Number H08A
or LF412MH/883 (Note 1)
See NS Package Number H08C
Dual-In-Line Package
565644
Order Number LF412ACN, LF412CN
or LF412MJ/883 (Note 1)
See NS Package Number J08A or N08E
BI-FET II™ is a trademark of National Semiconductor Corporation.
© 2010 National Semiconductor Corporation
5656
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LF412 Low Offset, Low Drift Dual JFET Input Operational Amplifier
January 28, 2010
LF412
Simplified Schematic
1/2 Dual
565643
Note 1: Available per JM38510/11905
Detailed Schematic
565632
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2
LF412
±18V
±30V
(Note 3)
Output Short Circuit
Duration (Note 4)
±19V
±15V
Continuous
Continuous
(Note 5)
670 mW
150°C
152°C/W
115°C
115°C/W
(Note 12)
Tj max
θjA (Typical)
Operating Temp. Range
(Note 6)
(Note 6)
Storage Temp.
−65°C≤TA≤150° −65°C≤TA≤150°
C
C
Range
Lead Temp.
(Soldering, 10 sec.)
260°C
260°C
ESD Tolerance
1700V
1700V
(Note 13)
(Note 11)
LF412A
±22V
±38V
N Package
Power Dissipation
If Military/Aerospace specified devices are required,
please contact the National Semiconductor Sales Office/
Distributors for availability and specifications.
Supply Voltage
Differential Input Voltage
Input voltage Range
H Package
LF412
Absolute Maximum Ratings (Note 2)
DC Electrical Characteristics
(Note 7)
Symbol
Parameter
Conditions
LF412A
Min
LF412
Min
Units
Typ
Max
Typ
Max
VOS
Input Offset Voltage
RS=10 kΩ, TA=25°C
0.5
1.0
1.0
3.0
mV
ΔVOS/ΔT
Average TC of Input
RS=10 kΩ (Note 8)
7
10
7
20
μV/°C
25
100
25
100
pA
2
nA
Offset Voltage
IOS
Input Offset Current
VS=±15V
Tj=25°C
(Note 7, Note 9)
Tj=70°C
VS=±15V
Tj=25°C
(Note 7, Note 9)
Tj=70°C
Tj=125°C
2
Tj=125°C
IB
Input Bias Current
RIN
Input Resistance
Tj=25°C
AVOL
Large Signal Voltage
VS=±15V, VO=±10V,
Gain
RL=2k, TA=25°C
VO
Output Voltage Swing
VCM
Input Common-Mode
25
50
Common-Mode
nA
pA
4
4
nA
50
50
nA
50
1012
50
200
1012
Ω
200
V/mV
25
Over Temperature
25
200
15
200
V/mV
VS=±15V, RL=10k
±12
±13.5
±12
±13.5
V
±16
+19.5
±11
+14.5
V
−11.5
V
Voltage Range
CMRR
25
200
200
−16.5
RS≤10k
80
100
70
100
dB
80
100
70
100
dB
Rejection Ratio
PSRR
Supply Voltage
Rejection Ratio
(Note 10)
IS
Supply Current
VO = 0V, RL = ∞
3.6
5.6
3.6
6.5
mA
Note 2: “Absolute Maximum Ratings” indicate limits beyond which damage to the device may occur. Operating Ratings indicate conditions for which the device
is functional, but do not guarantee specific performance limits.
AC Electrical Characteristics
(Note 7)
Symbol
Parameter
LF412A
Conditions
Min
Typ
LF412
Max
Min
Typ
Units
Max
Amplifier to Amplifier
TA=25°C, f=1 Hz-20 kHz
Coupling
(Input Referred)
SR
Slew Rate
VS=±15V, TA=25°C
10
15
8
15
V/μs
GBW
Gain-Bandwidth Product
VS=±15V, TA=25°C
3
4
2.7
4
MHz
−120
3
−120
dB
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LF412
Symbol
Parameter
LF412A
Conditions
Min
THD
Total Harmonic Dist
AV=+10, RL=10k,
VO=20 Vp-p,
BW=20 Hz-20 kHz
en
Equivalent Input Noise
TA=25°C, RS=100Ω,
Voltage
f=1 kHz
Equivalent Input Noise
TA=25°C, f=1 kHz
in
Typ
LF412
Max
Min
Typ
≤0.02
≤0.02
25
25
0.01
0.01
Units
Max
%
Current
Note 3: Unless otherwise specified the absolute maximum negative input voltage is equal to the negative power supply voltage.
Note 4: Any of the amplifier outputs can be shorted to ground indefintely, however, more than one should not be simultaneously shorted as the maximum junction
temperature will be exceeded.
Note 5: For operating at elevated temperature, these devices must be derated based on a thermal resistance of θjA.
Note 6: These devices are available in both the commercial temperature range 0°C≤TA≤70°C and the military temperature range −55°C≤TA≤125°C. The
temperature range is designated by the position just before the package type in the device number. A “C” indicates the commercial temperature range and an
“M” indicates the military temperature range. The military temperature range is available in “H” package only. In all cases the maximum operating temperature is
limited by internal junction temperature Tj max.
Note 7: Unless otherwise specified, the specifications apply over the full temperature range and for VS=±20V for the LF412A and for VS=±15V for the LF412.
VOS, IB, and IOS are measured at VCM=0.
Note 8: The LF412A is 100% tested to this specification. The LF412 is sample tested on a per amplifier basis to insure at least 85% of the amplifiers meet this
specification.
Note 9: The input bias currents are junction leakage currents which approximately double for every 10°C increase in the junction temperature, Tj. Due to limited
production test time, the input bias currents measured are correlated to junction temperature. In normal operation the junction temperature rises above the ambient
temperature as a result of internal power dissipation, PD. Tj=TA+θjA PD where θjA is the thermal resistance from junction to ambient. Use of a heat sink is
recommended if input bias current is to be kept to a minimum.
Note 10: Supply voltage rejection ratio is measured for both supply magnitudes increasing or decreasing simultaneously in accordance with common practice.
VS = ±6V to ±15V.
Note 11: Refer to RETS412X for LF412MH and LF412MJ military specifications.
Note 12: Max. Power Dissipation is defined by the package characteristics. Operating the part near the Max. Power Dissipation may cause the part to operate
outside guaranteed limits.
Note 13: Human body model, 1.5 kΩ in series with 100 pF.
Typical Performance Characteristics
Input Bias Current
Input Bias Current
565610
565611
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LF412
Supply Current
Positive Common-Mode
Input Voltage Limit
565612
565613
Negative Common-Mode
Input Voltage Limit
Positive Current Limit
565615
565614
Negative Current Limit
Output Voltage Swing
565616
565617
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LF412
Output Voltage Swing
Gain Bandwidth
565619
565618
Bode Plot
Slew Rate
565621
565620
Distortion vs Frequency
Undistorted Output Voltage
Swing
565622
565623
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LF412
Open Loop Frequency
Response
Common-Mode Rejection
Ratio
565625
565624
Power Supply Rejection
Ratio
Equivalent Input Noise
Voltage
565626
565627
Open Loop Voltage Gain
Output Impedance
565628
565629
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LF412
Inverter Settling Time
565630
Pulse Response
RL=2 kΩ, CL=10 pF
Small Signal Inverting
Small Signal Non-Inverting
565636
565637
Large Signal Inverting
Large Signal Non-Inverting
565639
565638
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8
LF412
Current Limit (RL=100Ω)
565640
The amplifiers will drive a 2 kΩ load resistance to ±10V over
the full temperature range. If the amplifier is forced to drive
heavier load currents, however, an increase in input offset
voltage may occur on the negative voltage swing and finally
reach an active current limit on both positive and negative
swings.
Precautions should be taken to ensure that the power supply
for the integrated circuit never becomes reversed in polarity
or that the unit is not inadvertently installed backwards in a
socket as an unlimited current surge through the resulting
forward diode within the IC could cause fusing of the internal
conductors and result in a destroyed unit.
As with most amplifiers, care should be taken with lead dress,
component placement and supply decoupling in order to ensure stability. For example, resistors from the output to an
input should be placed with the body close to the input to
minimize “pick-up” and maximize the frequency of the feedback pole by minimizing the capacitance from the input to
ground.
A feedback pole is created when the feedback around any
amplifier is resistive. The parallel resistance and capacitance
from the input of the device (usually the inverting input) to AC
ground set the frequency of the pole. In many instances the
frequency of this pole is much greater than the expected
3 dB frequency of the closed loop gain and consequently
there is negligible effect on stability margin. However, if the
feedback pole is less than approximately 6 times the expected
3 dB frequency a lead capacitor should be placed from the
output to the input of the op amp. The value of the added
capacitor should be such that the RC time constant of this
capacitor and the resistance it parallels is greater than or
equal to the original feedback pole time constant.
Application Hints
The LF412 series of JFET input dual op amps are internally
trimmed (BI-FET II™) providing very low input offset voltages
and guaranteed input offset voltage drift. These JFETs have
large reverse breakdown voltages from gate to source and
drain eliminating the need for clamps across the inputs.
Therefore, large differential input voltages can easily be accommodated without a large increase in input current. The
maximum differential input voltage is independent of the supply voltages. However, neither of the input voltages should be
allowed to exceed the negative supply as this will cause large
currents to flow which can result in a destroyed unit.
Exceeding the negative common-mode limit on either input
will cause a reversal of the phase to the output and force the
amplifier output to the corresponding high or low state.
Exceeding the negative common-mode limit on both inputs
will force the amplifier output to a high state. In neither case
does a latch occur since raising the input back within the
common-mode range again puts the input stage and thus the
amplifier in a normal operating mode.
Exceeding the positive common-mode limit on a single input
will not change the phase of the output, however, if both inputs
exceed the limit, the output of the amplifier may be forced to
a high state.
The amplifiers will operate with a common-mode input voltage
equal to the positive supply; however, the gain bandwidth and
slew rate may be decreased in this condition. When the negative common-mode voltage swings to within 3V of the negative supply, an increase in input offset voltage may occur.
Each amplifier is individually biased by a zener reference
which allows normal circuit operation on ±6.0V power supplies. Supply voltages less than these may result in lower gain
bandwidth and slew rate.
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LF412
Typical Application
Single Supply Sample and Hold
565631
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LF412
Physical Dimensions inches (millimeters) unless otherwise noted
Metal Can Package (H)
Order Number LF412MH or LF412CH
NS Package Number H08A
11
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LF412
Metal Can Package (H)
Order Number LF412MH/833
NS Package Number H08C
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LF412
Dual-In-Line Package (J)
Order Number LF412MJ/883
NS Package Number J08A
Dual-In-Line Package (N)
Order Number LF412ACN or LF412CN
NS Package Number N08E
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LF412 Low Offset, Low Drift Dual JFET Input Operational Amplifier
Notes
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