AD654
–6–
REV.
and insure the supply, source and load are appropriate. If provision
is made to trim offset, begin by setting the input to 1/10,000 of
full scale. Adjust the offset pot until the output is 1/10,000 of
full scale (for example, 25 Hz for a FS of 250 kHz). This is most
easily accomplished using a frequency meter connected to the
output. The FS input should then be applied and the gain pot
should be adjusted until the desired FS frequency is indicated.
INPUT PROTECTION
The AD654 was designed to be used with a minimum of additional
hardware. However, the successful application of a precision IC
involves a good understanding of possible pitfalls and the use of
suitable precautions. Thus +V
IN
and R
T
pins should not be driven
more than 300 mV below –V
S
. Likewise, Logic Common should
not drop more than 500 mV below –V
S
. This would cause inter-
nal junctions to conduct, possibly damaging the IC. In addition
to the diode shown in Figures 1 and 2 protecting Logic Common,
a second Schottky diode (MBD101) can protect the AD654’s
inputs from “below –V
S
’’ inputs as shown in Figure 5. It is also
desirable not to drive +V
IN
and R
T
above +V
S
. In operation, the
converter will exhibit a zero output for inputs above (+V
S
– 3.5 V).
Also, control currents above 2 mA will increase nonlinearity.
The AD654’s 80 dB dynamic range guarantees operation from a
control current of 1 mA (nominal FS) down to 100 nA (equiva-
lent to 1 mV to 10 V FS). Below 100 nA improper operation of
the oscillator may result, causing a false indication of input
amplitude. In many cases this might be due to short-lived noise
spikes which become added to input. For example, when scaled
to accept an FS input of 1 V, the –80 dB level is only 100 µV, so
when the mean input is only 60 dB below FS (1 mV), noise spikes
of 0.9 mV are sufficient to cause momentary malfunction.
This effect can be minimized by using a simple low-pass filter
ahead of the converter or a guard ring around the R
T
pin. The
filter can be assembled using the bias current compensation
resistor discussed in the previous section. For an FS of 10 kHz,
a single-pole filter with a time constant of 100 ms will be suitable,
but the optimum configuration will depend on the application
and the type of signal processing. Noise spikes are only likely to
be a cause of error when the input current remains near its mini-
mum value for long periods of time; above 100 nA full integration
of additive input noise occurs. Like the inputs, the capacitor
terminals are sensitive to interference from other signals. The
timing capacitor should be located as close as possible to the
AD654 to minimize signal pickup in the leads. In some cases,
guard rings or shielding may be required.
AD654
MBD101
I
IN
Figure 5. Input Protection
DECOUPLING
It is good engineering practice to use bypass capacitors on the
supply-voltage pins and to insert small-valued resistors (10 to
100 ) in the supply lines to provide a measure of decoupling
between the various circuits in the system. Ceramic capacitors
of 0.1 µF to 1.0 µF should be applied between the supply-
voltage pins and analog signal ground for proper bypassing on
the AD654. A proper ground scheme appears in Figure 6.
8
1
7
2
6
3
5
4
AD654
+5V
GND
DIGITAL
P.S.
10V
0.1mF
C
T
R
T
R
PU
f
OUT
AGND
V
IN
Figure 6. Proper Ground Scheme
OUTPUT INTERFACING CONSIDERATION
The output stage’s design allows easy interfacing to all digital logic
families. The output NPN transistor’s emitter and collector are
both uncommitted. The emitter can be tied to any voltage between
–V
S
and 4 volts below +V
S
, and the open collector can be pulled
up to a voltage 36 volts above the emitter regardless of +V
S
. The
high power output stage can sink over 10 mA at a maximum
saturation voltage of 0.4 V. The stage limits the output current
at 25 mA and can handle this limit indefinitely without damag-
ing the device.
NONLINEARITY SPECIFICATION
The preferred method of specifying nonlinearity error is in terms
of maximum deviation from the ideal relationship after calibrat-
ing the converter at full scale. This error will vary with the full
scale frequency and the mode of operation. The AD654 operates
best at a 150 kHz full-scale frequency with a negative voltage input;
the linearity is typically within 0.05%. Operating at higher fre-
quencies or with positive inputs will degrade the linearity as
indicated in the Specifications Table. Typical linearity at various
temperatures is shown in Figure 7.
FULL-SCALE FREQUENCY – kHz
10
0.01
10
MAXIMUM NONLINEARITY – %
1
150 250 350 500
5
0.5
0.10
0.05
f
AMB
= –408C
f
AMB
= 08C TO +858C
Figure 7. Typical Nonlinearities at Different Full-Scale
Frequencies
C
AD654
REV.
–7–
TWO-WIRE TEMPERATURE-TO-FREQUENCY
CONVERSION
Figure 8 shows the AD654 in a two-wire temperature-to-frequency
conversion scheme. The twisted pair transmission line serves the
dual purpose of supplying power to the device and also carrying
frequency data in the form of current modulation.
The positive supply line is fed to the remote V/F through a
140 resistor. This resistor is selected such that the quiescent
current of the AD654 will cause less than one V
BE
to be dropped.
As the V/F oscillates, additional switched current is drawn through
R
L
when Pin 1 goes low. The peak level of this additional cur-
rent causes Q1 to saturate, and thus regenerates the AD654’s
output square wave at the collector. The supply voltage to the
AD654 then consists of a dc level, less the resistive line drop, plus a
one V
BE
p-p square wave at the output frequency of the AD654.
This ripple is reduced by the diode/capacitor combination.
To set up the receiver circuit for a given voltage, the R
S
and R
L
resistances are selected as shown in Table I. CMOS logic stages
can be driven directly from the collector of Q1, and a single TTL
load can be driven from the junction of R
S
and R6.
Table I.
+V
S
R
S
()R
L
()
10 V 270 1.8k
15 V 680 2.7k
Table II.
(+V
S
) R1 () R2 () R3 () R4 () R5 ()
K
10 V 100k 127k
F = 10 Hz/K
15 V 100k 127k
°C
10 V 6.49k 4.02k 1k 95.3k 22.6k
F = 10 Hz/°C
15 V 12.7k 4.02k 1k 78.7k 36.5k
°F
10 V 6.49k 4.42k 1k 154k 22.6k
F = 5.55 Hz/°F
15 V 12.7k 4.42k 1k 105k 36.5k
At the V/F end, the AD592C temperature transducer is inter-
faced with the AD654 in such a manner that the AD654 output
frequency is proportional to temperature. The output frequency
can be sealed and offset from K to °C or °F using the resistor
values shown in Table II. Since temperature is the parameter of
interest, an NPO ceramic capacitor is used as the timing capaci-
tor for low V/F TC.
When scaling per K, resistors R1–R3 and the AD589 voltage
reference are not used. The AD592 produces a 1 µA/K current
output which drives Pin 3 of the AD654. With the timing
capacitor of 0.01 µF this produces an output frequency scaled to
10 Hz/K. When scaling per °C and °F, the AD589 and resistors
R1–R3 offset the drive current at Pin 3 by 273.2 µA for scaling
per °C and 255.42 µA for scaling per °F. This will result in fre-
quencies sealed at 10 Hz/°C and 5.55 Hz/°F, respectively.
OPTOISOLATOR COUPLING
A popular method of isolated signal coupling is via optoelec-
tronic isolators, or optocouplers. In this type of device, the signal is
coupled from an input LED to an output photo-transistor, with
light as the connecting medium. This technique allows dc to be
transmitted, is extremely useful in overcoming ground loop
problems between equipment, and is applicable over a wide
range of speeds and power.
Figure 9 shows a general purpose isolated V/F circuit using a
low cost 4N37 optoisolator. A +5 V power supply is assumed for
both the isolated (+5 V isolated) and local (+5 V local) supplies.
The input LED of the isolator is driven from the collector out-
put of the AD654, with a 9 mA current level established by R1
for high speed, as well as for a 100% current transfer ratio.
5V
(ISOLATED)
R1
390V
4N37
OPTO-ISOLATOR
5V
(LOCAL)
GRN
LED
OSC/
DRIVER
R
T
1kV
V
IN
(0V TO 1V)
C
T
1000pF
AD654
R3
270V
74LS14
Q1
2N3904
R2
120V
V/F OUTPUT
FS = 100kHz
TTL
ISOLATED LOCAL
Figure 9. Optoisolator Interface
OSC/
DRIVER
AD654
V
S
(10V TO 15V)
C
T
0.01mF
f
=
I
T
(10V) C
T
R
T
1mF
1N4148
R4
R5
R1
R2
R3
+
AD589
AD592
140V
R
S
R6
220V
Q1
2N3906
CMOS
OUTPUT
TTL
OUTPUT
(1 LOAD)
1mA/kV
Figure 8. Two-Wire Temperature-to-Frequency Converter
C
AD654
–8–
REV.
At the receiver side, the output transistor is operated in the
photo-transistor mode; that is with the base lead (Pin 6) open.
This allows the highest possible output current. For reasonable
speed in this mode, it is imperative that the load impedance be
as low as possible. This is provided by the single transistor stage
current-to-voltage converter, which has a dynamic load imped-
ance of less than 10 ohms and interfaces with TTL at the output.
USING A STAND-ALONE FREQUENCY COUNTER/LED
DISPLAY DRIVER FOR VOLTMETER APPLICATIONS
Figure 10 shows the AD654 used with a stand-alone frequency
counter/LED display driver. With C
T
= 1000 pF and R
T
= 1 k
the AD654 produces an FS frequency of 100 kHz when V
IN
=
+1 V. This signal is fed into the ICM7226A, a universal counter
system that drives common anode LEDs. With the FUNCTION
pin tied to D1 through a 10 k resistor the ICM7226A counts the
frequency of the signal at A
IN
. This count period is selected by
the user and can be 10 ms, 100 ms, 1s, or 10 seconds, as shown on
Pin 21. The longer the period selected, the more resolution the
count will have. The ICM7226A then displays the frequency on
the LEDs, driving them directly as shown. Refreshing of the LEDs
is handled automatically by the ICM7226. The entire circuit op-
erates on a single +5 V supply and gives a meter with 3, 4, or 5
digit resolution.
40
39
38
37
36
35
34
33
32
31
30
29
28
27
26
25
24
23
22
21
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
8
7
6
5
1
2
3
4
V
IN
(0V TO 1V)
5V 5V
1kV
1000pF
500V
825V
1kV
AD654
DI PIN 30
10kV
30kV
5V
5V
10MHz
CRYSTAL
22MV
39pF 39pF
5V 5V
10kV
5V
D1 (10ms)
D2 (100ms)
D3 (1s)
D4 (10s)
4
8
8
D.P. g e d c b af
LED
OVERFLOW
INDICATOR
D8 D7 D6 D5 D4 D3 D2 D1
AIN
HOLD
NC
OSL JN
OSL OUT
NC
D1
D2
D3
D4
D5
V+
D6
D7
D8
RANGE
ICM7226A
FUNCTION
dp
e
g
a
GND
d
b
c
f
+
N
C
= N
O
CO
NNE
C
T
Figure 10. AD654 With Stand-Alone Frequency Counter/
LED Display Driver
Longer count periods not only result in the count having more
resolution, they also serve as an integration of noisy analog signals.
For example, a normal-mode 60 Hz sine wave riding on the input
of the AD654 will result in the output frequency increasing on
the positive half of the sine wave and decreasing on the negative
half of the sine wave. This effect is cancelled by selecting a count
period equal to an integral number of noise signal periods. A
100 ms count period is effective because it not only has an inte-
gral number of 60 Hz cycles (6), it also has an integral number
of 50 Hz cycles (5). This is also true of the 1 second and 10 sec-
ond count period.
AD654-BASED ANALOG-TO-DIGITAL CONVERSION
USING A SINGLE CHIP MICROCOMPUTER
The AD654 can serve as an analog-to-digital converter when
used with a single component microcomputer that has an inter-
val timer/event counter such as the 8048. Figure 11 shows the
AD654, with a full-scale input voltage of +1 V and a full-scale
output frequency of 100 kHz, connected to the timer/counter
input Pin T1 of the 8048. Such a system can also operate on a
single +5 V supply.
The 8748 counter is negative edge triggered; after the STRT
CNT instruction is executed subsequent high to low transitions
on T1 increment the counter. The maximum rate at which the
counter may be incremented is once per three instruction cycles;
using a 6 MHz crystal, this corresponds to once every 7.5 µs, or
a maximum frequency of 133 kHz. Because the counter overflows
every 256 counts (8 bits), the timer interrupt is enabled. Each
overflow then causes a jump to a subroutine where a register is
incremented. After the STOP TCNT instruction is executed, the
number of overflows that have occurred will be the number in
this register. The number in this register multiplied by 256 plus
the number in the counter will be the total number of negative
edges counted during the count period. The count period is
handled simply by decrementing a register the number of times
necessary to correspond to the desired count time. After the
register has been decremented the required number of times the
STOP TCNT instruction is executed.
The total number of negative edges counted during the count
period is proportional to the input voltage. For example, if a 1 V
full-scale input voltage produces a 100 kHz signal and the count
period is 100 ms, then the total count will be 10,000. Scaling
from this maximum is then used to determine the input voltage,
i.e., a count of 5000 corresponds to an input voltage of 0.5 V.
As with the ICM7226, longer count times result in counts hav-
ing more resolution; and they result in the integration of noisy
analog signals.
C

AD654JRZ

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Voltage to Frequency & Frequency to Voltage SYNC V/F CONVERTR
Lifecycle:
New from this manufacturer.
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