
2-134
CA3140, CA3140A
The typical input current is in the order of 10pA when the
inputs are centered at nominal device dissipation. As the
output supplies load current, device dissipation will increase,
raising the chip temperature and resulting in increased input
current. Figure 16 shows typical input terminal current ver-
sus ambient temperature for the CA3140.
It is well known that MOSFET devices can exhibit slight
changes in characteristics (for example, small changes in
input offset voltage) due to the application of large differen-
tial input voltages that are sustained over long periods at ele-
vated temperatures.
Both applied voltage and temperature accelerate these
changes. The process is reversible and offset voltage shifts
of the opposite polarity reverse the offset. Figure 11 shows
the typical offset voltage change as a function of various
stress voltages at the maximum rating of +125oC (for TO-5);
at lower temperatures (TO-5 and plastic), for example, at
+85oC, this change in voltage is considerably less. In typical
linear applications, where the differential voltage is small and
symmetrical, these incremental changes are of about the
same magnitude as those encountered in an operational
amplifier employing a bipolar transistor input stage.
Super Sweep Function Generator
A function generator having a wide tuning range is shown in
Figure 18. The 1,000,000/1 adjustment range is accom-
plished by a single variable potentiometer or by an auxiliary
sweeping signal. The CA3140 functions as a non-inverting
readout amplifier of the triangular signal developed across
the integrating capacitor network connected to the output of
the CA3080A current source.
Buffered triangular output signals are then applied to a sec-
ond CA3080 functioning as a high speed hysteresis switch.
Output from the switch is returned directly back to the input
of the CA3080A current source, thereby, completing the pos-
itive feedback loop
The triangular output level is determined by the four 1N914
level limiting diodes of the second CA3080 and the resistor
divider network connected to terminal No. 2 (input) of the
CA3080. These diodes establish the input trip level to this
switching stage and, therefore, indirectly determine the
amplitude of the output triangle.
Compensation for propagation delays around the entire loop
is provided by one adjustment on the input of the CA3080.
This adjustment, which provides for a constant generator
amplitude output, is most easily made while the generator is
sweeping. High frequency ramp linearity is adjusted by the
single 7-to-6pF capacitor in the output of the CA3080A.
It must be emphasized that only the CA3080A is
characterized for maximum output linearity in the current
generator function.
Meter Driver and Buffer Amplifier
Figure 19 shows the CA3140 connected as a meter driver
and buffer amplifier. Low driving impedance is required of
the CA3080A current source to assure smooth operation of
the Frequency Adjustment Control. This low-driving
impedance requirement is easily met by using a CA3140
connected as a voltage follower. Moreover, a meter may be
placed across the input to the CA3080A to give a logarithmic
analog indication of the function generators frequency.
Analog frequency readout is readily accomplished by the
means described above because the output current of the
CA3080A varies approximately one decade for each 60mV
change in the applied voltage, VABC (voltage between
terminals 5 and 4 of the CA3080A of the function generator).
Therefore, six decades represent 360mV change in VABC.
Now, only the reference voltage must be established to set
the lower limit on the meter. The three remaining transistors
from the CA3086 Array used in the sweep generator are
used for this reference voltage. In addition, this reference
generator arrangement tends to track ambient temperature
variations, and thus compensates for the effects of the nor-
mal negative temperature coefficient of the CA3080A VABC
terminal voltage.
Another output voltage from the reference generator is used
to insure temperature tracking of the lower end of the
Frequency Adjustment Potentiometer. A large series
resistance simulates a current source, assuring similar
temperature coefficients at both ends of the Frequency
Adjustment Control.
To calibrate this circuit, set the Frequency Adjustment
Potentiometer at its low end. Then adjust the Minimum
Frequency Calibration Control for the lowest frequency. To
establish the upper frequency limit, set the Frequency
Adjustment Potentiometer to its upper end and then adjust
the Maximum Frequency Calibration Control for the
maximum frequency. Because there is interaction among
these controls, repetition of the adjustment procedure may
be necessary. Two adjustments are used for the meter. The
meter sensitivity control sets the meter scale width of each
decade, while the meter position control adjusts the pointer
on the scale with negligible effect on the sensitivity
adjustment. Thus, the meter sensitivity adjustment control
calibrates the meter so that it deflects 1/6 of full scale for
each decade change in frequency.
Sine Wave Shaper
The circuit shown in Figure 20 uses a CA3140 as a voltage
follower in combination with diodes from the CA3019 Array
to convert the triangular signal from the function generator to
a sine-wave output signal having typically less than 2% THD.
The basic zero crossing slope is established by the 10kΩ
potentiometer connected between terminals 2 and 6 of the
CA3140 and the 9.1kΩ resistor and 10kΩ potentiometer
from terminal 2 to ground. Two break points are established
by diodes D1 through D4. Positive feedback via D5 and D6
establishes the zero slope at the maximum and minimum
levels of the sine wave. This technique is necessary because
the voltage follower configuration approaches unity gain
rather than the zero gain required to shape the sine wave at
the two extremes.