The ICL8038 waveform generator is a monolithic integrated
circuit capable of producing high accuracy sine, square,
triangular, sawtooth and pulse waveforms with a minimum of
external components. The frequency (or repetition rate) can
be selected externally from 0.001Hz to more than 300kHz
using either resistors or capacitors, and frequency
modulation and sweeping can be accomplished with an
external voltage. The ICL8038 is fabricated with advanced
monolithic technology, using Schottky barrier diodes and thin
film resistors, and the output is stable over a wide range of
temperature and supply variations. These devices may be
interfaced with phase locked loop circuitry to reduce
temperature drift to less than 250ppm/
o
C.
Features
• Low Frequency Drift with Temperature. . . . . . .250ppm/oC
CAUTION: Stresses above those listed in “Absolute Maximum Ratings” may cause permanent damage to the device. This is a stress only rating and operationofthe
device at these or any other conditions above those indicated in the operational sections of this specification is not implied.
NOTE:
1. θJA is measured with the component mounted on an evaluation PC board in free air.
= ±10V or +20V, TA = 25oC, RL = 10kΩ, Test Circuit Unless Otherwise Specified (Continued)
SUPPLY
TEST
CONDITIONS
ICL8038CCICL8038BCICL8038AC
UNITSMINTYP MAX MINTYP MAX MINTYP MAX
Sine Wave
AmplitudeV
SINERSINE
THDTHDRS = 1MΩ
= 100kΩ0.20.22-0.20.22-0.20.22-xV
-2.05-1.53-1.01.5%
SUPPLY
(Note 4)
THD AdjustedTHDUse Figure 4-1.5--1.0--0.8-%
NOTES:
2. RA and RB currents not included.
3. V
= 20V; RA and RB = 10kΩ, f ≅ 10kHz nominal; can be extended 1000 to 1. See Figures 5A and 5B.
SUPPLY
4. 82kΩ connected between pins 11 and 12, Triangle Duty Cycle set at 50%. (Use RA and RB.)
5. Figure 1, pins 7 and 8 connected, V
= ±10V. See Typical Curves for T.C. vs V
SUPPLY
SUPPLY
.
6. Not tested, typical value for design purposes only.
Test Conditions
PARAMETERR
A
Supply Current10kΩ10kΩ10kΩ3.3nFClosedCurrent Into Pin 6
Sweep FM Range (Note 7)10kΩ10kΩ10kΩ3.3nFOpenFrequency at Pin 9
Frequency Drift with Temperature10kΩ10kΩ10kΩ3.3nFClosedFrequency at Pin 3
Frequency Drift with Supply Voltage (Note 8)10kΩ10kΩ10kΩ3.3nFClosedFrequency at Pin 9
Output Amplitude (Note 10)
Sine10kΩ10kΩ10kΩ3.3nFClosedPk-Pk Output at Pin 2
Triangle10kΩ10kΩ10kΩ3.3nFClosedPk-Pk Output at Pin 3
Leakage Current (Off) (Note 9)10kΩ10kΩ3.3nFClosedCurrent into Pin 9
Saturation Voltage (On) (Note 9)10kΩ10kΩ3.3nFClosedOutput (Low) at Pin 9
Rise and Fall Times (Note 11)10kΩ10kΩ4.7kΩ3.3nFClosedWaveform at Pin 9
Duty Cycle Adjust (Note 11)
Max50kΩ~1.6kΩ10kΩ3.3nFClosedWaveform at Pin 9
Min~25kΩ50kΩ10kΩ3.3nFClosedWaveform at Pin 9
Triangle Waveform Linearity10kΩ10kΩ10kΩ3.3nFClosedWaveform at Pin 3
Total Harmonic Distortion10kΩ10kΩ10kΩ3.3nFClosedWaveform at Pin 2
NOTES:
7. The hi and lo frequencies can be obtained by connecting pin 8 to pin 7 (fHI) and then connecting pin 8 to pin 6 (fLO). Otherwise apply Sweep
Voltage at pin 8 (2/3V
SUPPLY
+2V) ≤ V
SWEEP
≤ V
SUPPLY
5.3V and 10V with respect to ground.
8. 10V ≤ V+ ≤ 30V, or ±5V ≤ V
SUPPLY
≤±15V.
9. Oscillation can be halted by forcing pin 10 to +5V or -5V.
10. Output Amplitude is tested under static conditions by forcing pin 10 to 5V then to -5V.
11. Not tested; for design purposes only.
where V
R
B
SUPPLY
R
L
CSW1MEASURE
is the total supply voltage. In Figure 5B, pin 8 should vary between
3
10V
ICL8038
Test Circuit
Detailed Schematic
CURRENT SOURCES
R
EXT
5
2
Q
4
Q
8
46
Q
11
R
4
100
R
13
620
Q
26
7
R
30K
Q
Q
Q
Q
Q
R
1
Q
8
11K
R
2
39K
3
Q
31
32
33
34
9
23
1
Q
Q
6
Q
7
R
40K
30
Q
24
R
11
270
R
12
2.7K
Q
25
BR
Q
12
R
14
27K
R
15
470
Q
FLIP-FLOP
R
100
R
1.8K
29
EXT
4
Q
3
Q
5
Q
9
Q
10
Q
13
R
6
5
100
16
Q
Q
27
28
SW
N.C.
A
10
ICL8038
R
10K
B
R
A
10K
456
7
1
8
C
3300pF
FIGURE 1. TEST CIRCUIT
R
41
Q
35
4K
COMP ARATOR
Q
15
R
7B
15K
Q
Q
19
Q
36
R
41
27K
R
27K
Q
17
Q
16
R
10K
Q
21
20
R
27K
Q
37
Q
38
42
BUFFER AMPLIFIER
Q
14
C
EXT
R
17
4.7K
R
18
4.7K
+
R
L
10K
9
3
R
TRI
2
121110
R
82K
SINE
-10V
6
V+
R
32
R
8
5K
Q
18
R
9
5K
7A
Q
22
R
10
5K
43
Q
39
Q
40
3
11
R
19
800
R
20
2.7K
R
21
Q
10K
Q
41
Q
49
R
22
Q
10K
R
23
2.7K
R
24
R
800
44
1K
2
Q
Q
43
42
R
25
33K
R
28
33K
50
Q
51
Q
SINE CONVERTER
Q
Q
45
44
R
26
33K
R
29
33K
52
Q
53
Q
Q
Q
47
46
R
27
33K
R
30
33K
54
Q
55
Q
5.2K
48
R
33K
R
33K
56
1
R
33
200
R
34
375
R
35
330
45
R
36
1600
31
R
37
330
R
38
375
R
39
200
12
R
40
R
C
EXT
5.6K
82K
Application Information
(See Functional Diagram)
An external capacitor C is charged and discharged by two
current sources. Current source #2 is switched on and off by a
flip-flop, while current source #1 is on continuously. Assuming
that the flip-flop is in a state such that current source #2 is off,
and the capacitor is charged with a current I, the voltage
across the capacitor rises linearly with time.Whenthis voltage
reaches the level of comparator #1 (set at 2/3 of the supply
voltage), the flip-flop is triggered, changes states, and
releases current source #2. This current source normally
carries a current 2I, thus the capacitor is discharged with a
4
net-current I and the voltage across it drops linearly with time.
When it has reached the level of comparator #2 (set at 1/3 of
the supply voltage), the flip-flop is triggered into its original
state and the cycle starts again.
Four waveforms are readily obtainable from this basic
generator circuit. With the current sources set at I and 2I
respectively, the charge and discharge times are equal. Thus
a triangle waveform is created across the capacitor and the
flip-flop produces a square wave. Both waveforms are fed to
buffer stages and are available at pins 3 and 9.
ICL8038
The levels of the current sources can, however, be selected
overa wide range with two external resistors. Therefore,with
the two currents set at values different from I and 2I, an
asymmetrical sawtooth appears at Terminal 3 and pulses
with a duty cycle from less than 1% to greater than 99% are
available at Terminal 9.
The sine wave is created by feeding the triangle wave into a
nonlinear network (sine converter). This network provides a
decreasing shunt impedance as the potential of the triangle
moves toward the two extremes.
Waveform Timing
The
symmetry
external timing resistors. Two possible ways to accomplish
this are shown in Figure 3. Best results are obtained by
keeping the timing resistors R
controls the rising portion of the triangle and sine wave and
the 1 state of the square wave.
The magnitude of the triangle waveform is set at
V
SUPPLY
of all waveforms can be adjusted with the
and RB separate (A). R
A
1
/
3
; therefore the rising portion of the triangle is,
If the duty cycle is to be varied over a small range about 50%
only, the connection shown in Figure 3B is slightly more
convenient.A 1kΩ potentiometer may not allow the duty cycle
to be adjusted through 50% on all devices. If a 50% duty cycle
is required, a 2kΩ or 5kΩ potentiometer should be used.
With two separate timing resistors, the frequency is given by:
FIGURE 3. POSSIBLE CONNECTIONS FOR THE EXTERNAL TIMING RESISTORS
5
ICL8038
Neither time nor frequency are dependent on supply voltage,
even though none of the voltages are regulated inside the
integrated circuit. This is due to the fact that both currents
and thresholds are direct, linear functions of the supply
voltage and thus their effects cancel.
Reducing Distortion
To minimize sine wave distortion the 82kΩ resistor between
pins 11 and 12 is best made variable. With this arrangement
distortion of less than 1% is achievable. To reduce this even
further, two potentiometers can be connected as shown in
Figure 4; this configuration allows a typical reduction of sine
wave distortion close to 0.5%.
V+
1kΩ
R
A
456
7
8
C
FIGURE 4. CONNECTION TO ACHIEVE MINIMUM SINE WAVE
R
B
ICL8038
121110
DISTORTION
1
R
L
9
3
2
10kΩ100kΩ
100kΩ
10kΩ
V- OR GND
Selecting RA, RB and C
For any given output frequency, there is a wide range of RC
combinations that will work, however certain constraints are
placed upon the magnitude of the charging current for
optimum performance. At the low end, currents of less than
1µA are undesirable because circuit leakages will contribute
significant errors at high temperatures. At higher currents
(I > 5mA), transistor betas and saturation voltages will
contribute increasingly larger errors. Optimum performance
will, therefore, be obtained with charging currents of 10µAto
1mA. If pins 7 and 8 are shorted together, the magnitude of
the charging current due to R
R
1
----------------------------------------
I
R
V+ V-–()×
+()
1R2
1
------- -
×
R
A
can be calculated from:
A
0.22 V+ V-–()
------------------------------------==
R
A
and R2 are shown in the Detailed Schematic.
R
1
A similar calculation holds for RB.
The capacitor value should be chosen at the upper end of its
possible range.
Waveform Out Level Control and Power Supplies
The waveform generator can be operated either from a
single power supply (10V to 30V) or a dual power supply
(±5V to ±15V). With a single power supply the averagelevels
of the triangle and sine wave are at exactly one-half of the
supply voltage, while the square wave alternates between
V+ and ground. A split power supply has the advantage that
all waveforms move symmetrically about ground.
The square wave output is not committed. A load resistor
can be connected to a different power supply, as long as the
applied voltage remains within the breakdown capability of
the waveform generator (30V). In this way, the square wave
output can be made TTL compatible (load resistor
connected to +5V) while the waveform generator itself is
powered from a much higher voltage.
Frequency Modulation and Sweeping
The frequency of the waveform generator is a direct function
of the DC voltage at Terminal 8 (measured from V+). By
altering this voltage, frequency modulation is performed. For
small deviations (e.g. ±10%) the modulating signal can be
applied directly to pin 8, merely providing DC decoupling
with a capacitor as shown in Figure 5A. An external resistor
between pins 7 and 8 is not necessary, but it can be used to
increase input impedance from about 8kΩ (pins 7 and 8
connected together), to about (R + 8kΩ).
For larger FM deviations or for frequency sweeping, the
modulating signal is applied between the positive supply
voltage and pin 8 (Figure 5B). In this way the entire bias for
the current sources is created by the modulating signal, and
a very large (e.g. 1000:1) sweep range is created (f = 0 at
V
supply voltage; in this configuration the charge current is no
longer a function of the supply voltage (yet the trigger
thresholds still are) and thus the frequency becomes
dependent on the supply voltage.The potential on Pin 8 may
be swept down from V+ by (
= 0). Care must be taken, however, to regulate the
SWEEP
1
/3 V
SUPPLY
- 2V).
6
ICL8038
V+
R
L
V- OR GND
FM
ICL8038
R
B
R
A
456
7
R
8
C81K
9
3
2
121110
FIGURE 5A. CONNECTIONS FOR FREQUENCY MODULATION
V+
SWEEP
VOLTAGE
ICL8038
R
B
121110
R
A
456
8
C81K
R
L
9
3
2
V- OR GND
FIGURE 5B. CONNECTIONS FOR FREQUENCY SWEEP
FIGURE 5.
Typical Applications
The sine wave output has a relatively high output impedance
(1kΩ Typ). The circuit of Figure 6 provides buffering, gain
and amplitude adjustment. A simple op amp follower could
also be used.
V+
ICL8038
R
B
AMPLITUDE
2
100K
+
741
-
20K
R
A
456
7
8
With a dual supply voltage the external capacitor on Pin 10 can
be shorted to ground to halt the ICL8038 oscillation. Figure 7
shows a FET switch, diode ANDed with an input strobe signal
to allow the output to always start on the same slope.
V+
R
A
45
7
8
ICL8038
R
B
9
1N914
2
1011
C
2N4392
-15V
1N914
100K
OFF
15K
ON
STROBE
+15V (+10V)
-15V (-10V)
FIGURE 7. STROBE TONE BURST GENERATOR
To obtain a 1000:1 Sweep Range on the ICL8038 the
voltage across external resistors R
and RB must decrease
A
to nearly zero. This requires that the highest voltage on
control Pin 8 exceed the voltageat the top of R
and RBby a
A
few hundred mV. The Circuit of Figure 8 achieves this by
using a diode to lower the effective supply voltage on the
ICL8038. The large resistor on pin 5 helps reduce duty cycle
variations with sweep.
The linearity of input sweep voltage versus output frequency
can be significantly improved by using an op amp as shown
in Figure 10.
+10V
1N457
DUTY CYCLE
15K
9
3
10K
FREQ.
0.1µF
1K
4.7K
546
8
4.7K
ICL8038
1110
C
4.7K
FIGURE 6. SINE WAVE OUTPUT BUFFER AMPLIFIERS
7
2
121110
20K
≈15M
V-
0.0047µF
DISTORTION
100K
-10V
FIGURE 8. VARIABLE AUDIO OSCILLATOR, 20Hz TO 20kHzY
ICL8038
V1+
INPUT
DETECTOR
HIGH FREQUENCY
SYMMETRY
1,000pF
+15V
-
741
+
-V
IN
10kΩ
OFFSET
DUTY
CYCLE
FREQUENCY
ADJUST
45
7
9
8
ICL8038
TIMING
CAP.
PHASE
VCO
IN
AMPLIFIER
DEMODULATED
FM
R
2
LOW PASS
FILTER
R
1
FM BIAS
SQUARE
WAVE
OUT
FIGURE 9. WAVEFORM GENERATOR USED AS STABLE VCO IN A PHASE-LOCKED LOOP
1MΩ
9
3
2
50µF
15V
SINE WAVE
DISTORTION
10kΩ
100kΩ
+
1N753A
(6.2V)
1kΩ
1kΩ
P
4
500Ω
4.7kΩ
456
8
FUNCTION GENERATOR
3,900pF
4.7kΩ
ICL8038
121110
100kΩ
100kΩ
LOW FREQUENCY
SYMMETRY
-
+
+15V
741
6
3
2
1
121110
SINE WAVE
ADJ.
V2+
TRIANGLE
OUT
SINE WAVE
OUT
SINE WAVE
ADJ.
V-/GND
SINE WAVE
OUTPUT
-15V
FIGURE 10. LINEAR VOLTAGE CONTROLLED OSCILLATOR
Use in Phase Locked Loops
Its high frequency stability makes the ICL8038 an ideal
building block for a phase locked loop as shown in Figure 9.
In this application the remaining functional blocks, the phase
detector and the amplifier, can be formed by a number of
available ICs (e.g., MC4344, NE562).
In order to match these building blocks to each other, two
steps must be taken. First, two different supply voltages are
used and the square wave output is returned to the supply of
the phase detector. This assures that the VCO input voltage
will not exceed the capabilities of the phase detector. If a
smaller VCO signal is required, a simple resistive voltage
divider is connected between pin 9 of the waveform
generator and the VCO input of the phase detector.
8
Second, the DC output level of the amplifier must be made
compatible to the DC lev el required at the FM input of the
waveform generator (pin 8, 0.8V+). The simplest solution here
is to provide a voltage divider to V+ (R
, R2 as shown) if the
1
amplifier has a lower output lev el, or to g round if its level is
higher. The divider can be made part of the low-pass filter.
This application not only provides for a free-running
frequency with very low temperature drift, but is also has the
unique feature of producing a large reconstituted sinewave
signal with a frequency identical to that at the input.
For further information, see Harris Application Note AN013,
“Everything You Always Wanted to Know About the ICL8038”.
ICL8038
Definition of Terms
Supply Voltage (V
SUPPLY
V+ to V-.
Supply Current. The supply current required from the
power supply to operate the device, excluding load currents
and the currents through R
Frequency Range. The frequency range at the square wave
output through which circuit operation is guaranteed.
Sweep FM Range. The ratio of maximum frequency to
minimum frequency which can be obtained by applying a
sweep voltage to pin 8. For correct operation, the sweep
voltage should be within the range:
2
(
/3 V
SUPPLY
+ 2V) < V
). The total supply voltage from
and RB.
A
< V
SWEEP
SUPPLY
Typical Performance Curves
20
FM Linearity. The percentage deviation from the best fit
straight line on the control voltage versus output frequency
curve.
Output Amplitude. The peak-to-peak signal amplitude
appearing at the outputs.
Saturation Voltage. The output voltage at the collector of
Q
when this transistor is turned on. It is measured for a
23
sink current of 2mA.
Rise and Fall Times. The time required for the square wave
output to change from 10% to 90%, or 90% to 10%, of its
final value.
Triangle Waveform Linearity. The percentage deviation
from the best fit straight line on the rising and falling triangle
waveform.
Total Harmonic Distortion. The total harmonic distortion at
the sine wave output.
1.03
1.02
15
10
SUPPLY CURRENT (mA)
5
5 1015202530
SUPPLY VOLTAGE (V)
-55oC
25oC
125oC
1.01
1.00
0.99
NORMALIZED FREQUENCY
0.98
51015202530
SUPPLY VOLTAGE (V)
FIGURE 11. SUPPLY CURRENT vs SUPPLY VOLTAGEFIGURE 12. FREQUENCY vs SUPPLY VOLTAGE
1.03
1.02
1.01
1.00
0.99
NORMALIZED FREQUENCY
0.98
10
30
20
10
20
30
200
150
100
TIME (ns)
50
125oC
25
-55
o
C
o
C
RISE TIME
FALL TIME
125oC
o
25
C
o
-55
C
-50-2502575125
TEMPERATURE (oC)
0
LOAD RESISTANCE (kΩ)
FIGURE 13. FREQUENCY vs TEMPERATUREFIGURE 14. SQUARE WAVE OUTPUT RISE/FALL TIME vs
LOAD RESISTANCE
9
1064208
ICL8038
Typical Performance Curves
2
1.5
125oC
25
-55
LOAD CURRENT (mA)
SATURATION VOLTAGE
1.0
0.5
0
o
C
o
C
(Continued)
FIGURE 15. SQUARE WAVE SATURATIONVOLTAGEvs LOAD
CURRENT
1.2
1.1
1.0
LOAD CURRENT
0.9
0.8
LOAD CURRENT TO V+
NORMALIZED PEAK OUTPUT VOLTAGE
1064208
FIGURE 16. TRIANGLE WAVE OUTPUT VOLTAGE vs LOAD
CURRENT
10.0
-
TO V
LOAD CURRENT (mA)
125oC
25oC
-55oC
16642010201814128
1.0
0.9
0.8
0.7
NORMALIZED OUTPUT VOLTAGE
0.6
FREQUENCY (Hz)
10K1K100101M100K
FIGURE 17. TRIANGLE WAVE OUTPUT VOLTAGE vs
FREQUENCY
1.1
1.0
0.9
NORMALIZED OUTPUT VOLTAGE
1.0
LINEARITY (%)
0.1
0.01
FREQUENCY (Hz)
10K1K100101M100K
FIGURE 18. TRIANGLE WAVE LINEARITY vs FREQUENCY
12
10
8
6
4
DISTORTION (%)
2
UNADJUSTED
ADJUSTED
10K1K100101M100K
FREQUENCY (Hz)
0
100101M100K
1K
FREQUENCY (Hz)
10K
FIGURE 19. SINE WAVE OUTPUT VOLTAGE vs FREQUENCYFIGURE 20. SINE WAVE DISTORTION vs FREQUENCY
10
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