LTC2436-1
19
24361f
During the conversion period, the undershoot and/or
overshoot of a fast digital signal connected to the
LTC2436-1 pins may severely disturb the analog to digital
conversion process. Undershoot and overshoot can oc-
cur because of the impedance mismatch at the converter
pin when the transition time of an external control signal
is less than twice the propagation delay from the driver to
LTC2436-1. For reference, on a regular FR-4 board, signal
propagation velocity is approximately 183ps/inch for
internal traces and 170ps/inch for surface traces. Thus, a
driver generating a control signal with a minimum transi-
tion time of 1ns must be connected to the converter pin
through a trace shorter than 2.5 inches. This problem
becomes particularly difficult when shared control lines
are used and multiple reflections may occur. The solution
is to carefully terminate all transmission lines close to
their characteristic impedance.
Parallel termination near the LTC2436-1 pin will eliminate
this problem but will increase the driver power dissipation.
A series resistor between 27 and 56 placed near the
driver will also eliminate this problem without additional
power dissipation. The actual resistor value depends upon
the trace impedance and connection topology.
An alternate solution is to reduce the edge rate of the
control signals. It should be noted that using very slow
edges will increase the converter power supply current
during the transition time. The multiple ground pins used
in this package configuration, as well as the differential
input and reference architecture, reduce substantially the
converter’s sensitivity to ground currents.
Particular attention must be given to the connection of the
F
O
signal when the LTC2436-1 is used with an external
conversion clock. This clock is active during the conver-
sion time and the normal mode rejection provided by the
internal digital filter is not very high at this frequency. A
normal mode signal of this frequency at the converter
reference terminals may result into DC gain and INL
errors. A normal mode signal of this frequency at the
converter input terminals may result into a DC offset error.
Such perturbations may occur due to asymmetric capaci-
tive coupling between the F
O
signal trace and the converter
input and/or reference connection traces. An immediate
solution is to maintain maximum possible separation
between the F
O
signal trace and the input/reference sig-
nals. When the F
O
signal is parallel terminated near the
converter, substantial AC current is flowing in the loop
formed by the F
O
connection trace, the termination and the
ground return path. Thus, perturbation signals may be
inductively coupled into the converter input and/or refer-
ence. In this situation, the user must reduce to a minimum
the loop area for the F
O
signal as well as the loop area for
the differential input and reference connections.
Driving the Input and Reference
The input and reference pins of the LTC2436-1 converter
are directly connected to a network of sampling capaci-
tors. Depending upon the relation between the differential
input voltage and the differential reference voltage, these
capacitors are switching between these four pins
transfering small amounts of charge in the process. A
simplified equivalent circuit is shown in Figure 12, where
IN
+
and IN
refer to the selected differential channel and
the unselected channel is omitted for simplicity.
For a simple approximation, the source impedance R
S
driving an analog input pin (IN
+
, IN
, REF
+
or REF
) can be
considered to form, together with R
SW
and C
EQ
(see
Figure␣ 12), a first order passive network with a time
constant τ = (R
S
+ R
SW
) • C
EQ
. The converter is able to
sample the input signal with better than 1LSB accuracy if
the sampling period is at least 11 times greater than the
input circuit time constant τ. The sampling process on the
four input analog pins is quasi-independent so each time
constant should be considered by itself and, under worst-
case circumstances, the errors may add.
When using the internal oscillator (F
O
= LOW), the
LTC2436-1’s front-end switched-capacitor network is
clocked at 69900Hz corresponding to a 14.3µs sampling
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LTC2436-1
20
24361f
period. Thus, for settling errors of less than 1LSB, the
driving source impedance should be chosen such that τ
14.3µs/11 = 1.3µs. When an external oscillator of fre-
quency f
EOSC
is used, the sampling period is 2/f
EOSC
and,
for a settling error of less than 1LSB, τ 0.18/f
EOSC
.
Input Current
If complete settling occurs on the input, conversion re-
sults will be unaffected by the dynamic input current. An
incomplete settling of the input signal sampling process
may result in gain and offset errors, but it will not degrade
the INL performance of the converter. Figure 12 shows the
mathematical expressions for the average bias currents
flowing through the IN
+
and IN
pins as a result of the
sampling charge transfers when integrated over a sub-
stantial time period (longer than 64 internal clock cycles).
The effect of this input dynamic current can be analyzed
using the test circuit of Figure 13. The C
PAR
capacitor
includes the LTC2436-1 pin capacitance (5pF typical) plus
the capacitance of the test fixture used to obtain the results
shown in Figures 14 and 15. A careful implementation can
bring the total input capacitance (C
IN
+ C
PAR
) closer to 5pF
thus achieving better performance than the one predicted
Figure 13. An RC Network at IN
+
and IN
Figure 14. +FS Error vs R
SOURCE
at IN
+
or IN
(Small C
IN
)
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C
IN
24361 F13
V
INCM
+ 0.5V
IN
R
SOURCE
IN
+
LTC2436-1
C
PAR
20pF
C
IN
V
INCM
– 0.5V
IN
R
SOURCE
IN
C
PAR
20pF
R
SOURCE
()
1 10 100 1k 10k 100k
+FS ERROR (LSB)
24361 F14
3
0
1
2
V
CC
= 5V
REF
+
= 5V
REF
= GND
IN
+
= 5V
IN
= 2.5V
F
O
= GND
T
A
= 25°C
C
IN
= 0.01µF
C
IN
= 0.001µF
C
IN
= 100pF
C
IN
= 0pF
Figure 12. LTC2436-1 Equivalent Analog Input Circuit
V
REF
+
V
IN
+
V
CC
R
SW
(TYP)
20k
I
LEAK
I
LEAK
V
CC
I
LEAK
I
LEAK
V
CC
R
SW
(TYP)
20k
C
EQ
18pF
(TYP)
R
SW
(TYP)
20k
I
LEAK
I
IN
+
V
IN
I
IN
I
REF
+
I
REF
24361 F12
I
LEAK
V
CC
I
LEAK
I
LEAK
SWITCHING FREQUENCY
f
SW
= 69.900Hz INTERNAL OSCILLATOR (F
O
= LOW OR HIGH)
f
SW
= 0.5 • f
EOSC
EXTERNAL OSCILLATOR
V
REF
R
SW
(TYP)
20k
IIN
VV V
R
IIN
VV V
R
I REF
VV V
R
V
VR
I REF
VV V
R
V
VR
where
AVG
IN INCM REFCM
EQ
AVG
IN INCM REFCM
EQ
AVG
REF INCM REFCM
EQ
IN
REF EQ
AVG
REF INCM REFCM
EQ
IN
REF EQ
+
+
()
=
+−
()
=
−+
()
=
•− +
()
=
−• +
+
05
05
15
05
15
05
2
2
.
.
.
.
.
.
::
./
./
V REF REF
V
REF REF
VININ
V
IN IN
R M INTERNAL OSCILLATOR Hz Hz Notch F LOW
R f EXTERNAL OSCILLATOR
REF
REFCM
IN
INCM
EQ O
EQ EOSC
=−
=
+
=−
=
==
()
=•
()
+−
+−
+−
+−
2
2
397 50 60
0 555 10
12
LTC2436-1
21
24361f
by Figures 14 and 15. For simplicity, two distinct situa-
tions can be considered.
For relatively small values of input capacitance (C
IN
<
0.01µF), the voltage on the sampling capacitor settles
almost completely and relatively large values for the
source impedance result in only small errors. Such values
for C
IN
will deteriorate the converter offset and gain
performance without significant benefits of signal filtering
and the user is advised to avoid them. Nevertheless, when
small values of C
IN
are unavoidably present as parasitics
of input multiplexers, wires, connectors or sensors, the
LTC2436-1 can maintain its accuracy while operating with
relative large values of source resistance as shown in
Figure 16. +FS Error vs R
SOURCE
at IN
+
or IN
(Large C
IN
)
Figure 17. –FS Error vs R
SOURCE
at IN
+
or IN
(Large C
IN
)
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R
SOURCE
()
0
100 200 300 400 500 600 700 800 9001000
+FS ERROR (LSB)
24361 F16
20
16
12
8
4
0
V
CC
= 5V
REF
+
= 5V
REF
= GND
IN
+
= 3.75V
IN
= 1.25V
F
O
= GND
T
A
= 25°C
C
IN
= 0.01µF
C
IN
= 0.1µF
C
IN
= 1µF, 10µF
R
SOURCE
()
0
100 200 300 400 500 600 700 800 9001000
FS ERROR (LSB)
24361 F17
0
–4
–8
–12
–16
–20
V
CC
= 5V
REF
+
= 5V
REF
= GND
IN
+
= 1.25V
IN
= 3.75V
F
O
= GND
T
A
= 25°C
C
IN
= 0.01µF
C
IN
= 0.1µF
C
IN
= 1µF, 10µF
Figure 15. –FS Error vs R
SOURCE
at IN
+
or IN
(Small C
IN
)
R
SOURCE
()
1 10 100 1k 10k 100k
FS ERROR (LSB)
24361 F15
0
–3
–2
–1
V
CC
= 5V
REF
+
= 5V
REF
= GND
IN
+
= GND
IN
= 2.5V
F
O
= GND
T
A
= 25°C
C
IN
= 0.01µF
C
IN
= 0.001µF
C
IN
= 100pF
C
IN
= 0pF
Figures 14 and 15. These measured results may be slightly
different from the first order approximation suggested
earlier because they include the effect of the actual second
order input network together with the nonlinear settling
process of the input amplifiers. For small C
IN
values, the
settling on IN
+
and IN
occurs almost independently and
there is little benefit in trying to match the source imped-
ance for the two pins.
Larger values of input capacitors (C
IN
> 0.01µF) may be
required in certain configurations for antialiasing or gen-
eral input signal filtering. Such capacitors will average the
input sampling charge and the external source resistance
will see a quasi constant input differential impedance.
When F
O
= LOW (internal oscillator and 50Hz/60Hz notch),
the typical differential input resistance is 2M which will
generate a gain error of approximately 1LSB at full scale
for each 60 of source resistance driving IN
+
or IN
.
When F
O
is driven by an external oscillator with a fre-
quency f
EOSC
(external conversion clock operation), the
typical differential input resistance is 0.28 • 10
12
/f
EOSC
and each ohm of source resistance driving IN
+
or IN
will
result in 1.11 • 10
–7
• f
EOSC
LSB gain error at full scale. The
effect of the source resistance on the two input pins is
additive with respect to this gain error. The typical +FS and
–FS errors as a function of the sum of the source resis-
tance seen by IN
+
and IN
for large values of C
IN
are shown
in Figures 16 and 17.

LTC2436-1CGN#PBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Analog to Digital Converters - ADC 2-Ch Diff In 16-B No Lat DS ADC
Lifecycle:
New from this manufacturer.
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