LTC6601-2
16
66012f
APPLICATIONS INFORMATION
FUNCTIONAL DESCRIPTION
The LTC6601 is designed to make the implementation of
high frequency fully-differential fi ltering functions very
easy. A very low noise amplifi er is surrounded by 8 precision
matched resistors and 12 precision matched capacitors
so that a myriad of fi lter transfer functions limited only by
possible combinations and imagination can be confi gured
by hard wiring pins. The amplifi er itself is a wide band, low
noise and low distortion fully-differential amplifi er with ac-
curate output phase balancing. It is optimized for driving low
voltage, single-supply, differential input, analog-to-digital
converters (ADCs). The LTC6601’s outputs are capable
of swinging rail-to-rail on supplies as low as 2.7V, which
makes the amplifi er ideal for converting ground referenced,
single-ended signals into V
OCM
referenced differential
signals. Unlike traditional op amps which have a single
output, the LTC6601 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 and matched surrounding components provide
even-order harmonic distortion cancellation, and less
susceptibility to common mode noise (like power supply
noise). The LTC6601 can be used as a single-ended input
to differential output amplifi er, or as a differential input to
differential output amplifi er.
Figure 3 shows the basic fi lter architecture. The Laplace
transfer function from V
INDIFF
to V
OUTDIFF
is given by the
following generalized equation for a 2nd order lowpass
lter:
V
OUTDIFF
V
INDIFF
=
Gain
1+
s
2πf
O
•Q
+
s
2
2πf
O
()
2
Both Gain and Q of the fi lter are based on component ratios,
which match and track extremely well over temperature.
The corner frequency of the fi lter is a function of an RC
product. This RC product is trimmed to ±1% (typical) and
is not expected to drift by more than ±1% from nominal
over the entire temperature range –40°C to 85°C. As a
result, fully differential fi lters with tight magnitude, phase
tolerance and repeatability are achieved.
Although Figure 3 implies a differential input, the LTC6601
easily accepts single-ended inputs to either input, and will
faithfully replicate the signal at the output in differential
form.
The LTC6601’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 apply-
ing a voltage on the V
OCM
pin. If the pin is left open, there
is an internal resistive voltage divider, which develops a
Figure 3. Basic Filter Topology and Equations
+
+
C1
R3
R2
R2
R3
R1
R1
C2
C1
V
OUT(DIFF)
66012 F03
V
IN(DIFF)
C2
f
O
=
1
2P R2 R3 C1 C2
Q=
C2
C1
R3
R2
1
1+ 1+ GAIN

R3
R2
C2
C1
GAIN =
R2
R1
f
3dB
=
f
O
6089 3568 Q
4
1788 Q
2
+ 447
()
+ 1.287 10
5
•2Q
2
1
()
507.6 Q
Q =
0.2236 f
O
2.109 10
5
9.891 10
12
•f
3dB
4
5.486 10
9
•f
O
4
()
+ 120 5.526 10
9
•f
3dB
2
+ 3.082 10
6
•f
O
2
()
16 f
O
2
8.29 10
9
•f
3dB
2
+ 4.127 10
9
•f
O
2
()
6.638 10
10
•f
3dB
4
()
LTC6601-2
17
66012f
APPLICATIONS INFORMATION
potential halfway between the V
+
and V
pins. Whenever
this pin is not hard tied to a low impedance ground plane,
a high quality ceramic capacitor should be used to bypass
the V
OCM
pin to a low impedance ground plane (see Layout
Considerations). The LTC6601’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.
V
OUTCM
= V
OCM
=
V
OUT
+
+ V
OUT
2
The outputs (OUT
+
and OUT
) of the LTC6601 are capable
of swinging rail-to-rail. They can source or sink up to ap-
proximately 75mA of current. Load capacitances should
be decoupled with at least 25Ω of series resistance from
each output.
The LTC6601 Electrical Characteristics table specifi es an
input referred offset. This specifi cation actually lumps volt-
age offsets due to offset bias currents (I
OS
), and amplifi er
voltage offset into one specifi cation. To refer this specifi ca-
tion to the output, you simply multiply the specifi cation
by the noise gain the LTC6601 is confi gured in:
V
OSODIFF
= 1 + Gain
where Gain is the closed loop gain in the particular fi lter
application:
Gain =
R2
R1
COMPONENT INPUT PIN PROTECTION
All of the LTC6601 pins with the exception of V
+
and V
are
protected with steering diodes to either power supply. In
the event that a pin is driven beyond the supply rails, the
excess current should be limited to under 10mA to prevent
damage to the IC.
BIAS Pin
The LTC6601 has a BIAS pin (Pin 3) whose function is to
tailor both performance and power of the LTC6601. The
pin has a Thevenin equivalent impedance of approximately
150kΩ to a voltage source whose potential is 1.15V above
the V
supply. This pin has fi xed logic levels relative to V
(see the Electrical Characteristics table), and can be driven
by an external source keeping in mind its equivalent input
impedance and equivalent input voltage. If the BIAS pin is
oated, care should be taken to control external leakage
currents to this pin to under 1A to prevent putting the
LTC6601 an undesired state.
If BIAS is tied to the positive supply, the LTC6601 dif-
ferential fi lter will be in a fully active state confi gured for
highest performance (lowest noise and lowest distortion).
If the BIAS pin is fl oated or left unconnected, the LTC6601
lter will be in a fully active state, with amplifi er currents
reduced and performance scaled back to preserve power
consumption. If the BIAS pin is tied to the most negative
supply (V
), the LTC6601 will be placed into a low power
shutdown mode with amplifi er outputs disabled. In this
state, the LTC6601 draws approximately 450µA.
In low power shutdown, all internal biasing current sources
are shut off, and the output pins, OUT
+
and OUT
, will each
appear as open collectors with a non-linear capacitor in
parallel and steering diodes to either supply. The turn-on
and turn-off time constant between states are on the order
of 0.4s. Using this function to wire-OR outputs together
is not recommended.
General Design and Usage
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 which
can be as low as 3V (2.7V min), and will have an optimal
common mode input range near mid-supply. The LTC6601
makes interfacing to these ADCs easy, by providing anti-
alias fi ltering, single-ended to differential conversion and
common mode level shifting (translation). Figure 3 shows
a general application of this. The low frequency gain to
V
OUTDIFF
from V
IN
is simply:
V
OUTDIFF
= V
OUT
+
–V
OUT
R2
R1
•V
INDIFF
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
LTC6601-2
18
66012f
LTC6601 ideally suited for pre-amplifi cation, level shift-
ing and conversion of single-ended signals to differential
output signals for driving differential input ADCs.
INPUT IMPEDANCE
Calculating the low frequency input impedance of the
LTC6601 depends on how the inputs are driven (whether
they are driven from a single-ended or a differential
source).
Figure 4 shows a simplifi ed low frequency equivalent
circuit of the LTC6601. For balanced input sources (V
INP
= –V
INM
), the low frequency input impedance is given by
the equation:
R
INP
= R
INM
= R1
The differential input impedance is simply:
R
INDIFF
= 2 • R1
For single-ended inputs (V
INM
= 0), the input impedance
actually increases over the balanced differential case due
to the fact the summing node (at the junction of R1, R2
and R3) moves in phase with V
INP
to bootstrap the input
impedance. Referring to Figure 4 with V
INM
= 0, the input
impedance looking into either input is:
R
INP
=R
INM
R1
1–
1
2
R2
R1+R2
Input and Output Common Mode Voltage Range
The input common mode voltage is defi ned as the average
of the two inputs:
V
INCM
=
V
INP
+ V
INM
2
The lower limit of the input common mode range is dic-
tated by the ESD protection diodes at the input. While it
is possible for the inputs to swing below V
, the diodes
will conduct if the inputs are taken a diode drop below V
.
The upper limit of the input common mode range varies
as a function of the fi lter confi guration (GAIN), V
OCM
po-
tential, and whether or not the inputs are single-ended or
differential. While it is possible to exceed the upper limit
of the common mode range, doing so will degrade fi lter
linearity. Referring to Figure 4, for linear operation, the
summing junction where R1, R2 and R3 merge together
should be prevented from swinging to within 1.4V of the
V
+
power supply.
For the general case, the upper input common mode volt-
age limit should be constrained to:
V
OCM
R1
R1+R2
+ V
INCM
R2
R1+R2
V
+
1.4V
Or equivalently:
V
INCM
1+
R1
R2
V
+
1.4V
()
R1
R2
•V
OCM
The specifi cations for input common mode range (V
INCMR
)
are based on these constraints with R1 = R2 = 100, and
V
OCM
= mid-supply. Substituting the numbers for a single
3V power supply, (V
+
= 3V, V
= 0V) with V
OCM
=1.5V, and
R1 = R2 = 100, into the above equation, the input com-
mon mode range (V
INCMR
) is between the two limits:
0V ≤ V
INCM
≤ 1.7V
which is as is specifi ed for a 3V supply.
APPLICATIONS INFORMATION
+
R2
V
OUT
V
OUT
+
V
OCM
V
OUTDIFF
0.1µF
66012 F04
R1
R
INP
V
INP
V
INM
R1
R2
R3
R3
+
+
+
R
INM
Figure 4. Input Impedance

LTC6601CUF-2#TRPBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Differential Amplifiers Low Power, Low Distortion, 0.5% Tolerance, Pin Configurable Filter/Amplifier
Lifecycle:
New from this manufacturer.
Delivery:
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