REV. E
AD7701
–9–
C
R
R
A
IN
INTEGRATOR
TO DIGITAL
FILTER
CLOCK
1-BIT DAC
STROBED
COMPARATOR
+V
REF
–V
REF
Figure 9. SEC Basic Charge-Balancing ADC
The term charge-balancing comes from the fact that this system
is a negative feedback loop that tries to keep the net charge on
the integrator capacitor at zero by balancing charge injected by
the input voltage with charge injected by the 1-bit DAC. When
the analog input is zero the only contribution to the integrator
output comes from the 1-bit DAC. For the net charge on the
integrator capacitor to be zero, the DAC output must spend half
its time at +1 V and half its time at –1 V. Assuming ideal com-
ponents, the duty cycle of the comparator will be 50%.
When a positive analog input is applied, the output of the 1-bit
DAC must spend a larger proportion of the time at +1 V, so the
duty cycle of the comparator increases. When a negative input
voltage is applied, the duty cycle decreases.
The AD7701 uses a second-order, sigma-delta modulator and a
sophisticated digital filter that provides a rolling average of the
sampled output. After power-up or if there is a step change in
the input voltage, there is a settling time that must elapse before
valid data is obtained.
DIGITAL FILTERING
The AD7701’s digital filter behaves like an analog filter, with a
few minor differences.
First, since digital filtering occurs after the analog-to-digital
conversion, it can remove noise injected during the conversion
process. Analog filtering cannot do this.
On the other hand, analog filtering can remove noise super-
imposed on the analog signal before it reaches the ADC. Digital
filtering cannot do this and noise peaks riding on signals near
full scale have the potential to saturate the analog modulator
and digital filter, even though the average value of the signal is
within limits. To alleviate this problem, the AD7701 has over-
range headroom built into the sigma-delta modulator and digital
filter that allows overrange excursions of 100 mV. If noise
signals are larger than this, consideration should be given to
analog input filtering, or to reducing the gain in the input
channel so that a full-scale input (2.5 V) gives only a half-scale
input to the AD7701 (1.25 V). This will provide an overrange
capability greater than 100% at the expense of reducing the
dynamic range by one bit (50%).
FILTER CHARACTERISTICS
The cutoff frequency of the digital filter is f
CLK
/409600. At the
maximum clock frequency of 4.096 MHz, the cutoff frequency
of the filter is 10 Hz and the output rate is 4 kHz.
Figure 10 shows the filter frequency response. This is a six-pole
Gaussian response that provides 55 dB of 60 Hz rejection for a
10 Hz cutoff frequency. If the clock frequency is halved to give a
5 Hz cutoff, 60 Hz rejection is better than 90 dB. A normalized
s-domain pole-zero plot of the filter is shown in Figure 11.
The response of the filter is defined by:
Hx
xx x
xx x
()
=
+++ +
++
10693 0 240 0 0555
0 00962 0 00133 0 000154
24 6
810 12
05
...
.. .
.
where
xff f f
dB dB CLKIN
==
33
409600,
and f is the frequency of interest.
f
CLK
= 2MHz
f
CLK
= 1MHz
f
CLK
= 4MHz
1
10
100
FREQUENCY – Hz
20
0
–20
–40
–60
–80
–100
–120
–140
–160
GAIN – dBs
Figure 10. Frequency Response of AD7701 Filter
jw
s
0
j1
j2
–2
–1
–j1
–j2
S1,2 = –1.4663 + j1.8191
S3,4 = –1.7553 + j1.0005
S5,6 = –1.8739 + j0.32272
Figure 11. Normalized Pole-Zero Plot of AD7701 Filter
Since the AD7701 contains this on-chip, low-pass filtering,
there is a settling time associated with step function inputs,
and data will be invalid after a step change until the settling
time has elapsed. The AD7701 is, therefore, unsuitable for
high speed multiplexing, where channels are switched and
converted sequentially at high rates, as switching between chan-
nels can cause a step change in the input. Rather, it is intended
for distributed converter systems using one ADC per channel.
However, slow multiplexing of the AD7701 is possible, pro-
vided that the settling time is allowed to elapse before data for
the new channel is accessed.
REV. E–10–
AD7701
The output settling of the AD7701 in response to a step input
change is shown in Figure 12. The Gaussian response has fast
settling with no overshoot, and the worst-case settling time to
±0.0007% (±0.5 LSB) is 125 ms with a 4.096 MHz master
clock frequency.
PERCENT OF FINAL VALUE
100
80
60
40
20
0
04080120 160
TIME – ms
Figure 12. AD7701 Step Response
USING THE AD7701
SYSTEM DESIGN CONSIDERATIONS
The AD7701 operates differently from successive approxima-
tion ADCs or other integrating ADCs. Since it samples the
signal continuously, like a tracking ADC, there is no need for a
start convert command. The 16-bit output register is updated at
a 4 kHz rate, and the output can be read at any time, either
synchronously or asynchronously.
CLOCKING
The AD7701 requires a master clock input, which may be an
external TTL/CMOS compatible clock signal applied to the
CLKIN pin (CLKOUT not used). Alternatively, a crystal of
the correct frequency can be connected between CLKIN and
CLKOUT, when the clock circuit will function as a crystal
controlled oscillator.
The input sampling frequency, output data rate, filter character-
istics, and calibration time are all directly related to the master
clock frequency, f
CLKIN
, by the ratios given in the specification
table. Therefore, the first step in system design with the AD7701 is
to select a master clock frequency suitable for the bandwidth
and output data rate required by the application.
ANALOG INPUT RANGES
The AD7701 performs conversion relative to an externally
supplied reference voltage that allows easy interfacing to
ratiometric systems. In addition, either unipolar or bipolar input
voltage ranges may be selected using the BP/UP input. With
BP/UP tied low, the input range is unipolar and the span is 0 to
+V
REF
. With BP/UP tied high, the input range is bipolar and the
span is ±V
REF
. In the Bipolar mode, both positive and negative
full scale are directly determined by V
REF
. This offers superior
tracking of positive and negative full scale and better midscale
(bipolar zero) stability than bipolar schemes that simply scale
and offset the input range.
The digital output coding for the unipolar range is unipolar
binary; for the bipolar range it is offset binary. Bit weights for
the Unipolar and Bipolar modes are shown in Table I. The
input voltages and output codes for unipolar and bipolar ranges,
using the recommended +2.5 V reference, are shown in
Table II.
Table I. Bit Weight Table (2.5 V Reference Voltage)
Unipolar Mode Bipolar Mode
µV LSBs % FS ppm FS LSBs % FS ppm FS
10 0.26 0.0004 4 0.13 0.0002 2
19 0.5 0.0008 8 0.26 0.0004 4
38 1.00 0.0015 15 0.5 0.0008 8
76 2.00 0.0031 31 1.00 0.0015 15
153 4.00 0.0061 61 2.00 0.0031 31
Table II. Output Coding
Unipolar Mode Bipolar Mode
Input Relative to Input Relative to
FS and AGND Input (V) FS and AGND Input (V) Output Data
1111 1111 1111 1111
+V
REF
– 1.5 LSB +2.499943 +V
REF
– 1.5 LSB +2.499886 1111 1111 1111 1110
+V
REF
– 2.5 LSB +2.499905 +V
REF
– 2.5 LSB +2.499810 1111 1111 1111 1101
+V
REF
– 3.5 LSB +2.499867 +V
REF
– 3.5 LSB +2.499733 1111 1111 1111 1100
1000 0000 0000 0001
+V
REF
/2 + 0.5 LSB +1.250019 AGND + 0.5 LSB +0.000038 1000 0000 0000 0000
+V
REF
/2 – 0.5 LSB +1.249981 AGND – 0.5 LSB –0.000038 0111 1111 1111 1111
+V
REF
/2 – 1.5 LSB +1.249943 AGND – 1.5 LSB –0.000114 0111 1111 1111 1110
0000 0000 0000 0011
AGND + 2.5 LSB +0.000095 –V
REF
+ 2.5 LSB –2.499810 0000 0000 0000 0010
AGND + 1.5 LSB +0.000057 –V
REF
+ 1.5 LSB –2.499886 0000 0000 0000 0001
AGND + 0.5 LSB +0.000019 –V
REF
+ 0.5 LSB –2.499962 0000 0000 0000 0000
NOTES
1. V
REF
= 2.5 V
2. AGND = 0 V
3. Unipolar Mode, 1 LSB = 2.5 V/655536 = 0.000038 V
4. Bipolar Mode, 1 LSB = 5 V/65536 = 0.000076 V
5. Inputs are voltages at code transitions.
REV. E
AD7701
–11–
INPUT SIGNAL CONDITIONING
Reference voltages from 1 V to 3 V may be used with the AD7701
with little degradation in performance. Input ranges that cannot
be accommodated by this range of reference voltages may be
achieved by input signal conditioning. This may take the form
of gain to accommodate a smaller signal range, or passive attenua-
tion to reduce a larger input voltage range.
Source Resistance
If passive attenuators are used in front of the AD7701, care must
be taken to ensure that the source impedance is sufficiently low.
The AD7701 has an analog input with over 1 G dc input
resistance. In parallel with this, there is a small dynamic load that
varies with the clock frequency (see Figure 13). Each time the
analog input is sampled, a 10 pF capacitor draws a charge packet
of maximum 1 pC (10 pF × 100 mV) from the analog source
A
IN
R1
R2
C
EXT
AGND
AD7701
V
OS
100mV
C
IN
10pF
Figure 13. Equivalent Input Circuit and Input Attenuator
with a frequency f
CLKIN
/256. For a 4.096 MHz CLKIN, this
yields an average current draw of 16 nA. After each sample, the
AD7701 allows 62 clock periods for the input voltage to settle.
The equation that defines settling time is:
VV e
OIN
tRC
=−
[]
1
where
V
O
is the final settled value.
V
IN
is the value of the input signal.
R is the value of the input source resistance.
C is the 10 pF sample capacitor.
t is equal to 62/f
CLKIN
.
From this, the following equation can be developed, which
gives the maximum allowable source resistance, R
S(MAX)
, for
an error of V
E
:
R
S (MAX )
=
62
f
CLKIN
×(10 pF) × ln(100mV /V
E
)
Provided the source resistance is less than this value, the analog
input will settle within the desired error band in the requisite 62
clock periods. Insufficient settling leads to offset errors. These
can be calibrated in system calibration schemes.
If a limit of 10 µV (0.25 LSB at 16 bits) is set for the maximum
offset voltage, then the maximum allowable source resistance is
160 k from the above equation, assuming that there is no
external stray capacitance.
An RC filter may be added in front of the AD7701 to reduce
high frequency noise. With an external capacitor added from
A
IN
to AGND, the following equation will specify the maximum
allowable source resistance:
R
S (Max)
=
62
f
CLKIN
×(
C
IN
+
C
EXT
) × ln
100 mV × C
IN
/(C
IN
+ C
EXT
)
V
E
The practical limit to the maximum value of source resistance is
thermal (Johnson) noise. A practical resistor may be modeled as
an ideal (noiseless) resistor in series with a noise voltage source
or in parallel with a noise current source:
V kTRf Volts
n
= 4
i kTRf R Amperes
n
= 4
where
k is Boltzmann’s constant (1.38 × 10
–23
J/K).
T is temperature in degrees Kelvin (°C + 273).
Active signal conditioning circuits such as op amps generally do
not suffer from problems of high source impedance. Their open-
loop output resistance is normally only tens of ohms and, in any
case, most modern general-purpose op amps have sufficiently
fast closed-loop settling time for this not to be a problem. Offset
voltage in op amps can be eliminated in a system calibration
routine. With the wide dynamic range and small LSB size of the
AD7701, noise can also be a problem, but the digital filter will
reject most broadband noise above its cutoff frequency. How-
ever, in certain applications there may be a need for analog
input filtering.
Antialias Considerations
The digital filter of the AD7701 does not provide any rejection
at integer multiples of the sampling frequency (nf
CLKlN
/256,
where n = 1, 2, 3 . . . ).
With a 4.096 MHz master clock, there are narrow (±10 Hz)
bands at 16 kHz, 32 kHz, 48 kHz, and so on, where noise
passes unattenuated to the output.
However, due to the AD7701’s high oversampling ratio of 800
(16 kHz to 20 Hz), these bands occupy only a small fraction of
the spectrum and most broadband noise is filtered. The reduc-
tion in broadband noise is given by:
e
OUT
= e
IN
2 f
C
/ f
S
= 0.035 e
IN
where
e
lN
and e
OUT
are rms noise terms referred to the input.
f
C
is the filter –3 dB corner frequency (f
CLKIN
/409600).
f
S
is the sampling frequency (f
CLKIN
/256).
Since the ratio of f
S
to f
CLKIN
is fixed, the digital filter reduces
broadband white noise by 96.5% independent of the master
clock frequency.

AD7701ARZ

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Analog to Digital Converters - ADC 16-Bit IC
Lifecycle:
New from this manufacturer.
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