LT1994
10
1994fb
Functional Description
The LT1994 is a small outline, wideband, low noise and
low distortion fully-differential amplifi er with accurate
output-phase balancing. The LT1994 is optimized to
drive low voltage, single-supply, differential input ana-
log-to-digital converters (ADCs). The LT1994’s output is
capable of swinging rail-to-rail on supplies as low as 2.5V,
which makes the amplifi er ideal for converting ground
referenced, single-ended signals into V
OCM
referenced
differential signals in preparation for driving low voltage,
single-supply, differential input ADCs. Unlike traditional
op amps which have a single output, the LT1994 has two
outputs to process signals differentially. This allows for
two times the signal swing in low voltage systems when
compared to single-ended output amplifi ers. The balanced
differential nature of the amplifi er also provides even-order
harmonic distortion cancellation, and less susceptibility
to common mode noise (like power supply noise). The
LT1994 can be used as a single-ended input to differential
output amplifi er, or as a differential input to differential
output amplifi er.
The LT1994’s output common mode voltage, defi ned as the
average of the two output voltages, is independent of the
input common mode voltage, and is adjusted by applying
a voltage on the V
OCM
pin. If the pin is left open, there is an
internal resistive voltage divider, which develops a potential
halfway between the V
+
and V
pins. The V
OCM
pin will have
an equivalent Thevenin equivalent resistance of 40k, and a
Thevenin equivalent voltage of half supply. Whenever this
pin is not hard tied to a low impedance ground plane, it
is recommended that a high quality ceramic capacitor is
used to bypass the V
OCM
pin to a low impedance ground
plane (see Layout Considerations in this document). The
LT1994’s internal common mode feedback path forces
accurate output phase balancing to reduce even order
harmonics, and centers each individual output about the
potential set by the V
OCM
pin.
VV
VV
OUTCM OCM
OUT OUT
==
+
+
2
The outputs (OUT
+
and OUT
) of the LT1994 are capable
of swinging rail-to-rail. They can source or sink up to
approximately 85mA of current. Each output is rated to
drive approximately 25pF to ground (12.5pF differentially).
Higher load capacitances should be decoupled with at least
25Ω of series resistance from each output.
Input Pin Protection
The LT1994’s input stage is protected against differential
input voltages that exceed 1V by two pairs of back-to-
back diodes that protect against emitter base breakdown
of the input transistors. In addition, the input pins have
steering diodes to either power supply. If the input pair
is overdriven, the current should be limited to under
10mA to prevent damage to the IC. The LT1994 also has
steering diodes to either power supply on the V
OCM
, and
SHDN pins (Pins 2 and 7) and if exposed to voltages that
exceed either supply, they too should be current limited
to under 10mA.
SHDN Pin
If the SHDN pin (Pin 7) is pulled 2.1V below the positive
supply, an internal current is generated that is used to
power down the LT1994. The pin will have the Thevenin
equivalent impedance of approximately 55kΩ to V
+
. If
the pin is left unconnected, an internal pull-up resistor of
120k will keep the part in normal active operation. Care
should be taken to control leakage currents at this pin to
under 1A to prevent leakage currents from inadvertently
putting the LT1994 into shutdown. In shutdown, all biasing
current sources are shut off, and the output pins OUT
+
and
OUT
will each appear as open collectors with a nonlinear
capacitor in parallel, and steering diodes to either supply.
Because of the nonlinear capacitance, the outputs still have
the ability to sink and source small amounts of transient
current if exposed to signifi cant voltage transients. The
inputs (IN
+
and IN
) have anti-parallel diodes that can
conduct if voltage transients at the input exceed 1V. The
inputs also have steering diodes to either supply. The
turn-on and turn-off time between the shutdown and
active states are on the order of 1s but depends on the
circuit confi guration.
APPLICATIONS INFORMATION
11
1994fb
LT1994
General Amplifi er Applications
As levels of integration have increased and, correspond-
ingly, system supply voltages decreased, there has been
a need for ADCs to process signals differentially in order
to maintain good signal-to-noise ratios. These ADCs are
typically supplied from a single-supply voltage that can
be as low as 2.5V and will have an optimal common mode
input range near mid-supply. The LT1994 makes interfac-
ing to these ADCs trivial, by providing both single-ended
to differential conversion as well as common mode level
shifting. Figure 1 shows a general single-supply application
with perfectly matched feedback networks from OUT
+
and
OUT
. The gain to V
OUTDIFF
from V
INM
and V
INP
is:
VVV
R
R
VV
OUTDIFF OUT OUT
F
I
INP INM
=≈
()
+
–•
Note from the above equation that the differential output
voltage (V
OUT
+
– V
OUT
) is completely independent of
input and output common mode voltages, or the voltage
at the common mode pin. This makes the LT1994 ideally
suited pre-amplifi cation, level shifting, and conversion
of single-ended signals to differential output signals in
preparation for driving differential input ADCs.
Effects of Resistor Pair Mismatch
Figure 2 shows a circuit diagram that takes into consid-
eration that real world resistors will not perfectly match.
Assuming infi nite open-loop gain, the differential output
relationship is given by the equation:
VVV
R
R
V
VV
OUTDIFF OUT OUT
F
I
INDIFF
AVG
ICM
AVG
OCM
=≅+
ΔΔ
+
–•
•– ,
β
β
β
β
where:
R
F
is the average of R
F1
and R
F2
, and R
I
is the average
of R
I1
and R
I2
.
β
AVG
is defi ned as the average feedback factor (or gain)
from the outputs to their respective inputs:
β
AVG
I
IF
I
IF
R
RR
R
RR
=
+
+
+
1
2
2
22
1
11
Δβ is defi ned as the difference in feedback factors:
Δ=
++
β
R
RR
R
RR
I
IF
I
IF
2
22
1
11
Figure 1. Test Circuit Figure 2. Real-World Application
V
OCM
0.1µF
1994 F01
R
I
R
F
R
L
V
+
0.1µF
0.1µF
V
CM
V
SHDN
V
INM
V
INP
V
OUTCM
3
7
6
8
1
2
5
4
V
V
OUT
+
V
IN
V
OUT
V
IN
+
R
BAL
R
BAL
0.1µF
R
I
R
F
R
L
+
+
LT1994V
OCM
1994 F02
R
I2
R
F2
R
L
V
S
V
SHDNB
V
INM
V
INP
+
+
3
7
6
8
1
2
5
4
LT1994V
OCM
V
OCM
V
OUT
+
V
IN
V
OUT
V
IN
+
0.1µF
0.1µF
R
I1
R
F1
R
L
SHDN
APPLICATIONS INFORMATION
LT1994
12
1994fb
V
ICM
is defi ned as the average of the two input voltages,
V
INP
and V
INM
(also called the input common mode
voltage):
VVV
ICM INP INM
=+
()
1
2
and V
INDIFF
is defi ned as the difference of the input
voltages:
V
INDIFF
= V
INP
– V
INM
When the feedback ratios mismatch (Δβ), common mode
to differential conversion occurs.
Setting the differential input to zero (V
INDIFF
= 0), the de-
gree of common mode to differential conversion is given
by the equation:
VVV
VV
V
OUTDIFF OUT OUT
ICM OCM
AVG
INDIFF
z

$
–•
B
B
0
In general, the degree of feedback pair mismatch is a source
of common mode to differential conversion of both signals
and noise. Using 1% resistors or better will provide about
28dB of common mode rejection. Using 0.1% resistors
will provide about 48dB of common mode rejection. A low
impedance ground plane should be used as a reference
for both the input signal source and the V
OCM
pin. A direct
short of V
OCM
to this ground plane or bypassing the V
OCM
with a high quality 0.1µF ceramic capacitor to this ground
plane will further mitigate against common mode signals
from being converted to differential.
Input Impedance and Loading Effects
The input impedance looking into the V
INP
or V
INM
input
of Figure 1 depends on whether or not the sources V
INP
and V
INM
are fully differential. For balanced input sources
(V
INP
= –V
INM
), the input impedance seen at either input
is simply:
R
INP
= R
INM
= R
I
For single-ended inputs, because of the signal imbalance
at the input, the input impedance actually increases over
the balanced differential case. The input impedance looking
into either input is:
RR
R
R
RR
INP INM
I
F
IF
==
+
1
1
2
–•
Input signal sources with non-zero output impedances can
also cause feedback imbalance between the pair of feedback
networks. For the best performance, it is recommended
that the source’s output impedance be compensated for.
If input impedance matching is required by the source,
R1 should be chosen (see Figure 3):
R
RR
RR
INM S
INM S
1=
According to Figure 3, the input impedance looking into
the differential amp (R
INM
) refl ects the single-ended source
case, thus:
R
R
R
RR
INM
I
F
IF
=
+
1
1
2
–•
R2 is chosen to balance R1||R
S
:
R
RR
RR
S
S
2
1
1
=
+
Figure 3. Optimal Compensation for Signal-Source Impedance
1994 F03
R
I
R
F
R
S
V
S
+
+
LT1994
R
I
R
F
R2 = R
S
|| R1
R1 CHOSEN SO THAT R1 || R
INM
= R
S
R2 CHOSEN TO BALANCE R1 || R
S
R1
R
INM
APPLICATIONS INFORMATION

LT1994IDD#TRPBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
High Speed Operational Amplifiers 70MHz Low Noise/Distortion Differential Amplifer
Lifecycle:
New from this manufacturer.
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