LTC2641/LTC2642
16
26412fd
For more information www.linear.com/LTC2641
APPLICATIONS INFORMATION
such as the LTC6078 is suitable, if the application does
not require linear operation very near to GND, or zero scale
(Figure 2). The LTC6078 typically swings to within 1mV of
GND if it is not required to sink any load current. For an
LSB size of 38µV, 1mV represents 26 missing codes near
zero scale. Linearity will be degraded over a somewhat
larger range of codes above GND. It is also unavoidable
that settling time and transient performance will degrade
whenever a single supply amplifier is operated very close
to GND, or to the positive supply rail.
The small LSB size of a 16-bit DAC, coupled with the tight
accuracy specifications on the LTC2641/LTC2642, means
that the accuracy and input specifications for the external
op amp are critical for overall DAC performance.
Op Amp Specifications and Unipolar DAC Accuracy
Most op amp accuracy specifications convert easily to
DAC accuracy.
Op amp input bias current on the noninverting (+) input is
equivalent to an I
L
loading the DAC V
OUT
pin and therefore
produces a DAC zero-scale error (ZSE) (see Unbuffered
Operation):
ZSE = –I
B
(IN+) • R
OUT
[Volts]
In 16-bit LSBs:
ZSE = I
B
IN
+
( )
6.2k •
66k
V
REF
 LSB
Op amp input impedance, R
IN
, is equivalent to an R
L
loading the LTC2641/LTC2642 V
OUT
pin, and produces
a gain error of:
GE =
–66k
1+
6.2k
R
IN
 LSB
Op amp offset voltage, V
OS
, corresponds directly to DAC
zero code offset error, ZSE:
ZSEV
k
V
LSB
OS
REF
=
[]
66
Temperature effects also must be considered. Over the
–40°C to 85°C industrial temperature range, an offset
voltage temperature coefficient (referenced to 25°C) of
0.6μV/°C will add 1LSB of zero-scale error. Also, I
BIAS
and
the V
OFFSET
error it causes, will typically show significant
relative variation over temperature.
Op amp open-loop gain, A
VOL
, contributes to DAC gain
error (GE):
GE
k
A
LSB
VOL
=
[]
66
Op amp input common mode rejection ratio (CMRR) is an
input-referred error that corresponds to a combination of
gain error (GE) and INL, depending on the op amp archi
-
tecture and operating conditions. A conservative estimate
of total CMRR error is:
Error = 10
CMRR
20
V
CMRR_RANGE
V
REF
66k LSB
where V
CMRR_RANGE
is the voltage range that CMRR (in
dB) is specified over. Op amp Typical Performance Char-
acteristics graphs
are
useful to predict the impact of CMRR
errors on DAC performance. Typically, a precision op amp
will exhibit a fairly linear CMRR behavior (corresponding
to DAC gain error only) over most of the common mode
input range (CMR), and become nonlinear and produce
significant errors near the edge of the CMR.
Rail-to-rail input op amps are a special case, because they
have 2 distinct input stages, one with CMR to GND and
the other with CMR to V
+
. This results in acrossover”
CM input region where operation switches between the
two input stages.
The LTC6078 rail-to-rail input op amp typically exhibits
remarkably low crossover linearity error, as shown in the
V
OS
vs V
CM
Typical Performance Characteristics graphs
(see the LTC6078 data sheet). Crossover occurs at CM
inputs about 1V below V
+
, and an LTC6078 operating as
a unipolar DAC buffer with V
REF
= 2.5V and V
+
= 5V will
typically add only about 1LSB of GE and almost no INL
error due to CMRR. Even in a full rail-to-rail
application,
with
V
REF
= V
+
= 5V, a typical LTC6078 will add only about
1LSB of INL at 16-bits.
LTC2641/LTC2642
17
26412fd
For more information www.linear.com/LTC2641
Op Amp Specifications and Bipolar DAC Accuracy
The op amp contributions to unipolar DAC error discussed
above apply equally to bipolar operation. The bipolar ap
-
plication circuit gains up the DAC span, and all errors, by
a factor of 2. Since the LSB size also doubles, the errors
in LSBs are identical in unipolar and bipolar modes.
One added error in bipolar mode comes from I
B
(IN
),
which flows through R
FB
to generate an offset. The full
bias current offset error becomes:
V
OFFSET
= (I
B
(IN
) • R
FB
– I
B
(IN
+
) • R
OUT
• 2) [Volts]
So:
VIIN kIIN k
k
V
OFFSET BB
REF
=
()
+
()•–()•.
28 12 4
33
[]
LSB
Settling Time with Op Amp Buffer
When using an external op amp, the output settling time
will still include the single pole settling on the LTC2641/
LTC2642 V
OUT
node, with time constant R
OUT
• (C
OUT
+
C
L
) (see Unbuffered V
OUT
Settling Time). C
L
will include
the buffer input capacitance and PC board interconnect
capacitance.
The external buffer amplifier adds another pole to the output
response, with a time constant equal to (fbandwidth/2π).
For example, assume that C
L
is maintained at the same
value as above, so that the V
OUT
node time constant is
83ns = 1μs/12. The output amplifier pole will also have a
time constant of 83ns if the closed-loop bandwidth equals
(1/2π • 83ns) = 1.9MHz. The effective time constant of
two cascaded single-pole sections is approximately the
root square sum of the individual time constants, or2
• 83ns = 117ns, and 1/2 LSB settling time will be ~12 •
117ns = 1.4μs. This represents an ideal case, with no slew
limiting and ideal op amp phase margin. In practice, it
will take a considerably faster amplifier, as well as careful
attention to maintaining good phase margin, to approach
the unbuffered settling time of 1μs.
The output settling time
for bipolar applications (Fig-
ure
3) will be somewhat increased due to the feedback
resistor network R
FB
and R
INV
(each 28k nominal). The
parasitic capacitance, C
P
, on the op amp (–) input node
will introduce a feedback loop pole with a time constant
of (C
P
• 28k/2). A small feedback capacitor, C1, should be
included, to introduce a zero that will partially cancel this
pole. C1 should nominally be <C
P
, typically in the range
of 5pF to 10pF . This will restore the phase margin and
improve coarse settling time, but a pole-zero doublet will
unavoidably leave a slower settling tail, with a time con
-
stant of roughly (C
P
+ C1) • 28k/2, which will limit 16-bit
settling time to be greater than 2µs.
Reference and GND Input
The LTC2641/LTC2642 operates with external voltage refer
-
ences from 2
V to V
DD
, and linearity, offset and gain errors
are virtually unchanged vs V
REF
. Full 16-bit performance
can be maintained if appropriate guidelines are followed
when selecting and applying the reference. The LTC2641/
LTC2642’s very low gain error tempco of 0.1ppm/°C, typ
-
ical, corresponds
to less than 0.5LSB variation over the
–40°C to 85°C temperature range. In practice, this means
that
the overall gain error tempco will be determined almost
entirely by the external reference tempco.
The DAC voltage-switching modeinverted” resistor lad
-
der architecture used in the LTC2641/LTC2642 exhibits a
reference
input resistance (R
REF
) that is code dependent
(see the Typical Performance curves I
REF
vs Input Code).
In unipolar mode, the minimum R
REF
is 14.8k (at code
871Chex, 34,588 decimal) and the the maximum R
REF
is
300k at code 0000hex (zero scale). The maximum change
in I
REF
for a 2.5V reference is 160µA. Since the maximum
occurs near midscale, the INL error is about one half of the
change on V
REF
, so maintaining an INL error of <0.1LSB
requires a reference load regulation of (1.53ppm • 2/160µA)
= 19 [ppm/mA]. This implies a reference output impedance
of 48mΩ, including series wiring resistance.
To prevent output glitches from occurring when resistor
ladder branches switch from GND to V
REF
, the reference
input must maintain low impedance at higher frequencies.
A 0.1μF ceramic capacitor with short leads between REF
and GND provides high frequency bypassing. A surface
mount ceramic chip capacitor is preferred because it has
the lowest inductance. An additionalF between
REF
and
GND provides low frequency bypassing. The circuit
APPLICATIONS INFORMATION
LTC2641/LTC2642
18
26412fd
For more information www.linear.com/LTC2641
will benefit from even higher bypass capacitance, as long
as the external reference remains stable with the added
capacitive loading.
Digital Inputs and Interface Logic
All of the digital inputs include Schmitt-trigger buffers to
accept slow transition interfaces. This means that opto
-
cuplers can interface directly to the LTC2641/LTC2642
without additional external logic. Digital input hysteresis
is typically 150mV.
The digital inputs are compatible with TTL/CMOS-logic
levels. However, rail-to-rail (CMOS) logic swings are
preferred, because operating the logic inputs away from
the supply rails generates additional I
DD
and GND current,
(see Typical Performance Characteristic graph Supply
Current vs Logic Input Voltage).
Digital feedthrough is only 0.2nV•s typical, but it is always
preferred to keep all logic inputs static except when loading
a new code into the DAC.
Board Layout for Precision
Even a small amount of board leakage can degrade
accuracy. The 6nA leakage current into V
OUT
needed to
generate 1LSB offset error corresponds to 833MΩ leakage
resistance from a 5V supply.
The V
OUT
node is relatively sensitive to capacitive noise
coupling, so minimum trace length, appropriate shielding
and clean board layout are imperative here.
Temperature differences at the DAC, op
amp or reference
pins can easily generate tens of microvolts of thermocou-
ple voltages. Analog signal traces should be short, close
together
and away from heat dissipating components. Air
currents across the board can also generate thermocouples.
The PC board should have separate areas for the analog and
digital sections of the circuit. A single, solid ground plane
should be used, with analog and digital signals carefully
routed over separate areas of the plane. This keeps digital
signals away from sensitive analog signals and minimizes
the interaction between digital ground currents and the
analog section of the ground plane.
Astar ground” area should be established by attaching
the LTC2641/LTC2642 GND pin, V
REF
GND and the DAC
V
OUT
GND reference terminal to the same area on the
GND plane. Care should be taken to ensure that no large
GND return current paths flow through thestar GND”
area. In particular, the resistance from the LTC2641 GND
pin to the point where the V
REF
input source connects to
the ground plane should be as low as possible. Excessive
resistance here will be multiplied by the code dependent
I
REF
current to produce an INL error similar to the error
produced by V
REF
source resistance. For the LTC2641 in
the S8 package both GND pins, Pin 2 and Pin 7 should
be tied to the same GND plane.
Sources of ground return current in the analog area include
op amp power supply bypass capacitors and the GND
connection for single supply amps. A useful technique
for minimizing errors is to use a separate board layer for
power ground return connections, and reserve one ground
plane layer for low current “signal” GND connections.
Thesignal”, orstar” GND plane must connected to the
“power” GND plane at a single point, which should be
located near the LTC2641/LTC2642 GND pin.
If separate analog and digital ground areas exist it is neces
-
sary to connect them at a single location, which should be
fairly
close to the DAC for digital signal integrity. In some
systems, large GND return currents can flow between the
digital and analog GNDs, especially if different PC boards
are involved. In such cases the digital and analog ground
connection point should not be made right at thestar”
GND area, so the highly sensitive analog signals are not
corrupted. If forced to choose, always place
analog ground
quality
ahead of digital signal ground. (A few mV of noise
APPLICATIONS INFORMATION

LTC2641IDD-12#PBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Digital to Analog Converters - DAC Single Unipolar12-bit Unbuffered Vout DACs
Lifecycle:
New from this manufacturer.
Delivery:
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