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CA3140AE

Part # CA3140AE
Description IC OPAMP GP 4.5MHZ 8DIP
Category IC
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Technical Document


DISCLAIMER: The information provided herein is solely for informational purposes. Customers must be aware of the suitability of this product for their application, and consider that variable factors such as Manufacturer, Product Category, Date Codes, Pictures and Descriptions may differ from available inventory.

7
Bandwidth and Slew Rate
For those cases where bandwidth reduction is desired, for
example, broadband noise reduction, an external capacitor
connected between Terminals 1 and 8 can reduce the open
loop -3dB bandwidth. The slew rate will, however, also be
proportionally reduced by using this additional capacitor.
Thus, a 20% reduction in bandwidth by this technique will
also reduce the slew rate by about 20%.
Figure 5 shows the typical settling time required to reach
1mV or 10mV of the final value for various levels of large
signal inputs for the voltage follower and inverting unity gain
amplifiers. The exceptionally fast settling time characteristics
are largely due to the high combination of high gain and wide
bandwidth of the CA3140; as shown in Figure 6.
Input Circuit Considerations
As mentioned previously, the amplifier inputs can be driven
below the Terminal 4 potential, but a series current limiting
resistor is recommended to limit the maximum input terminal
current to less than 1mA to prevent damage to the input
protection circuitry.
Moreover, some current limiting resistance should be
provided between the inverting input and the output when
the CA3140 is used as a unity gain voltage follower. This
resistance prevents the possibility of extremely large input
FIGURE 4. METHODS OF UTILIZING THE V
CE(SAT)
SINKING CURRENT CAPABILITY OF THE CA3140 SERIES
FIGURE 5A. WAVEFORM FIGURE 5B. TEST CIRCUITS
FIGURE 5. SETTLING TIME vs INPUT VOLTAGE
3
2
4
CA3140
7
6
LOAD
R
L
R
S
MT
2
MT
1
30V
NO LOAD
120V
AC
3
2
4
CA3140
7
6
V+ +HV
LOAD
R
L
SETTLING TIME (µs)
0.1
INPUT VOLTAGE (V)
1.0 10
SUPPLY VOLTAGE: V
S
= ±15V
T
A
= 25
o
C
1mV
10mV 10mV
1mV
1mV1mV
10mV
FOLLOWER
INVERTING
LOAD RESISTANCE (R
L
) = 2k
LOAD CAPACITANCE (C
L
) = 100pF
10
8
6
4
2
0
-2
-4
-6
-8
-10
10mV
3
2
CA3140
6
SIMULATED
LOAD
4
-15V
0.1µF
5.11k
0.1µF
7
+15V
5k
2k
100pF
5k
INVERTING
SETTLING POINT
200
4.99k
D
1
1N914
D
2
1N914
2
CA3140
6
SIMULATED
LOAD
4
-15V
0.1µF
0.1µF
7
+15V
2k
100pF
0.05µF
2k
3
10k
FOLLOWER
CA3140, CA3140A
8
All Intersil semiconductor products are manufactured, assembled and tested under ISO9000 quality systems certification.
Intersil semiconductor products are sold by description only. Intersil Corporation reserves the right to make changes in circuit design and/or specifications at any time with-
out notice. Accordingly, the reader is cautioned to verify that data sheets are current before placing orders. Information furnished by Intersil is believed to be accurate and
reliable. However, no responsibility is assumed by Intersil or its subsidiaries for its use; nor for any infringements of patents or other rights of third parties which may result
from its use. No license is granted by implication or otherwise under any patent or patent rights of Intersil or its subsidiaries.
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signal transients from forcing a signal through the input
protection network and directly driving the internal constant
current source which could result in positive feedback via the
output terminal. A 3.9k resistor is sufficient.
The typical input current is on 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 7 shows typical input terminal current versus
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
differential input voltages that are sustained over long
periods at elevated 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 9 shows the
typical offset voltage change as a function of various stress
voltages at the maximum rating of 125
o
C (for metal can); at
lower temperatures (metal can and plastic), for example, at
85
o
C, 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.
FIGURE 6. OPEN LOOP VOLTAGE GAIN AND PHASE vs
FREQUENCY
FIGURE 7. INPUT CURRENT vs TEMPERATURE
FIGURE 8. OUTPUT VOLTAGE SWING CAPABILITY AND COMMON MODE INPUT VOLTAGE RANGE vs SUPPLY VOLTAGE
10
1
10
3
10
4
10
5
10
6
10
7
10
8
FREQUENCY (Hz)
OPEN LOOP VOLTAGE GAIN (dB)
100
80
60
40
20
0
SUPPLY VOLTAGE: V
S
= ±15V
T
A
= 25
o
C
10
2
OPEN LOOP PHASE
-75
-90
-105
-120
-135
-150
(DEGREES)
R
L
= 2k,
C
L
= 0pF
R
L
= 2k,
C
L
= 100pF
φOL
SUPPLY VOLTAGE: V
S
= ±15V
TEMPERATURE (
o
C)
-60 -40 -20 0 20 40 60 80 100 120 140
INPUT CURRENT (pA)
1K
100
1
10K
10
SUPPLY VOLTAGE (V+, V-)
0 5 10 15 20 25
-1.5
-2.0
-1.0
-2.5
R
L
=
+V
OUT
AT T
A
= 125
o
C
+V
OUT
AT T
A
= 25
o
C
+V
OUT
AT T
A
= -55
o
C
+V
ICR
AT T
A
= 125
o
C
+V
ICR
AT T
A
= 25
o
C
+V
ICR
AT T
A
= -55
o
C
-3.0
0
-0.5
INPUT AND OUTPUT VOLTAGE EXCURSIONS
FROM TERMINAL 7 (V+)
SUPPLY VOLTAGE (V+, V-)
0 5 10 15 20 25
-V
ICR
AT T
A
= 125
o
C
-V
ICR
AT T
A
= 25
o
C
-V
ICR
AT T
A
= -55
o
C
-V
OUT
FOR
T
A
= -55
o
C to 125
o
C
INPUT AND OUTPUT VOLTAGE EXCURSIONS
FROM TERMINAL 4 (V-)
0
-0.5
0.5
-1.0
-1.5
1.5
1.0
CA3140, CA3140A
9
Super Sweep Function Generator
A function generator having a wide tuning range is shown in
Figure 10. The 1,000,000/1 adjustment range is
accomplished 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
second 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 positive 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 7pF to 60pF 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 11 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 generator’s 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, V
ABC
(voltage between
Terminals 5 and 4 of the CA3080A of the function generator).
Therefore, six decades represent 360mV change in V
ABC
.
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
normal negative temperature coefficient of the CA3080A
V
ABC
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 12 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 10k
potentiometer connected between Terminals 2 and 6 of the
CA3140 and the 9.1k resistor and 10k potentiometer
from Terminal 2 to ground. Two break points are established
by diodes D
1
through D
4
. Positive feedback via D
5
and D
6
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.
7
6
5
4
3
2
0
OFFSET VOLTAGE SHIFT (mV)
0 500 1000 1500 2000 2500 3000 3500 4000 4500
TIME (HOURS)
1
DIFFERENTIAL DC VOLTAGE
(ACROSS TERMINALS 2 AND 3) = 0V
OUTPUT VOLTAGE = V+ / 2
T
A
= 125
o
C
FOR METAL CAN PACKAGES
DIFFERENTIAL DC VOLTAGE
(ACROSS TERMINALS 2 AND 3) = 2V
OUTPUT STAGE TOGGLED
FIGURE 9. TYPICAL INCREMENTAL OFFSET VOLTAGE
SHIFT vs OPERATING LIFE
CA3140, CA3140A
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