8-158
Reducing Distortion
To minimize sine wave distortion the 82kΩ resistor between
pins 11 and 12 is best made variable. With this arrangement
distor tion 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%.
Selecting RA, RB and C
For any given output frequency, there is a wide range of RC
combinations that will work, however cer tain constraints are
placed upon the magnitude of the charging current for opti-
mum performance. At the low end, currents of less than 1µA
are undesirable because circuit leakages will contribute sig-
nificant errors at high temperatures. At higher currents
(I > 5mA), transistor betas and saturation voltages will con-
tribute increasingly larger errors. Optimum performance will,
therefore, be obtained with charging currents of 10µA to
1mA. If pins 7 and 8 are shor ted together, the magnitude of
the charging current due to RA can be calculated from:
R1 and R2 are shown in the Detailed Schematic.
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 sin-
gle power supply (10V to 30V) or a dual power supply (±5V
to ±15V). With a single power supply the average levels of
the triangle and sine wave are at exactly one-half of the sup-
ply 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 con-
nected to +5V) while the waveform generator itself is pow-
ered 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 con-
nected 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
VSWEEP = 0). Care must be taken, however, to regulate the
supply voltage; in this configuration the charge current is no
longer a function of the supply v oltage (yet the trigger thresh-
olds still are) and thus the frequency becomes dependent on
the supply voltage. The potential on Pin 8 may be swept
down from V+ by (1/3 VSUPPLY - 2V).
ICL8038
456
9
2
121110
8
7
C100kΩ
RARL
V- OR GND
3
RB
V+
1kΩ
110kΩ100kΩ
10kΩ
FIGURE 4. CONNECTION TO ACHIEVE MINIMUM SINE WAVE
DISTORTION
IR1V+ V-–()×
R
1
R
2
+()
---------------------------------------- 1
RA
--------
×0.22 V+ V-–()
R
A
------------------------------------==
C 81K
ICL8038
456
9
2
121110
8
7
RARL
V- OR GND
3
RB
V+
R
FM
FIGURE 5A. CONNECTIONS FOR FREQUENCY MODULATION
C 81K
ICL8038
456
9
2
121110
8
RARL
V- OR GND
3
RB
V+
SWEEP
VOLTAGE
FIGURE 5B. CONNECTIONS FOR FREQUENCY SWEEP
FIGURE 5.
ICL8038