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.
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 ac-
commodated without a large increase in input current. The
maximum differential input voltage is independent of the sup-
ply 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.
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 en-
sure 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 feed-
back pole by minimizing the capacitance from the input to
ground.
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.
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.
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 neg-
ative common-mode voltage swings to within 3V of the neg-
ative 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 sup-
plies. Supply voltages less than these may result in lower gain
bandwidth and slew rate.
9
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