3-6
PMOS transistors Q3 and Q5. The source of bias potentials
for these PMOS transistors is described later. Miller Effect
compensation (roll off) is accomplished by means of the
30pF capacitor and 2kΩ resistor connected between the
base and collector of transistor Q11. These internal compo-
nents provide sufficient compensation for unity gain opera-
tion in most applications. However, additional compensation,
if desired, may be used between Terminals 1 and 8.
Bias-Source Circuit
At total supply voltages, somewhat above 8.3V, resistor R2
and zener diode Z 1 serve to estab lish a v oltage of 8.3V across
the series connected circuit, consisting of resistor R1, diodes
D1 through D4, and PMOS transistor Q1. A tap at the junction
of resistor R1 and diode D4 provides a gate bias potential of
about 4.5V for PMOS transistors Q4 and Q5 with respect to
Terminal 7. A potential of about 2.2V is developed across
diode connected PMOS transistor Q1 with respect to Terminal
7 to provide gate bias for PMOS transistors Q2 and Q3. It
should be noted that Q1 is “mirror connected” to both Q2 and
Q3. Since transistors Q1, Q2 and Q3 are designed to be iden-
tical, the approximately 200µA current in Q1 establishes a
similar current in Q2 and Q3 as constant current sources for
both the first and second amplifier stages, respectively.
At total supply voltages somewhat less than 8.3V, zener diode
Z1 becomes non-conductive and the potential, developed
across series connected R1, D1-D4, and Q1 varies directly
with variations in supply voltage. Consequently, the gate bias
for Q4, Q5 and Q2, Q3 varies in accordance with supply
voltage variations. This variation results in deterioration of the
power supply rejection ration (PSRR) at total supply voltages
below 8.3V. Operation at total supply voltages below about
4.5V results in seriously degraded performance.
Output Stage
The output stage consists of a drain loaded inver ting ampli-
fier using CMOS transistors operating in the Class A mode.
When operating into very high resistance loads, the output
can be swung within millivolts of either supply rail. Because
the output stage is a drain loaded amplifier, its gain is depen-
dent upon the load impedance. The transfer characteristics
of the output stage for a load returned to the negative supply
rail are shown in Figure 20. Typical op-amp loads are readily
driven by the output stage. Because large signal excursions
are nonlinear, requiring feedback for good waveform repro-
duction, transient delays may be encountered. As a voltage
follower, the amplifier can achieve 0.01% accuracy levels,
including the negative supply rail.
Offset Nulling
Offset voltage nulling is usually accomplished with a 100,000Ω
potentiometer connected across Terminals 1 and 5 and with the
potentiometer slider arm connected to Terminal 4. A fine offset
null adjustment usually can be aff ected with the slider arm posi-
tioned in the mid point of the potentiometer’s total range .
Input Current Variation with Common Mode Input Voltage
As shown in the Table of Electrical Specifications, the input
current for the CA5160 Series Op Amps is typically 5pA at
TA = 25oC when Ter minals 2 and 3 are at a common-mode
potential of +7.5V with respect to negative supply Terminal
4. Figure 1 contains data showing the variation of input
current as a function of common-mode input voltage at
TA=25
o
C. These data show that circuit designers can
advantageously exploit these characteristics to design
circuits which typically require an input current of less than
1pA, provided the common-mode input voltage does not
exceed 2V. As previously noted, the input current is
essentially the result of the leakage current through the gate-
protection diodes in the input circuit and, therefore, a
function of the applied voltage. Although the finite resistance
of the glass terminal-to-case insulator of the metal can
package also contributes an increment of leakage current,
there are useful compensating factors. Because the gate-
protection network functions as if it is connected to Ter minal
4 potential, and the metal can case of the CA5160 is also
internally tied to Terminal 4, input terminal 3 is essentially
“guarded” from spurious leakage currents.
Input Current Variation with Temperature
The input current of the CA5160 series circuits is typically
5pA at 25oC . The major portion of this input current is due to
leakage current through the gate protective diodes in the
input circuit. As with any semiconductor-junction device,
including op amps with a junction-FET input stage, the
leakage current approximately doubles for every 10oC
increase in temperature. Figure 2 provides data on the
typical variation of input bias current as a function of
temperature in the CA5160.
In applications requiring the lowest practical input current
and incremental increases in current because of “warm-up”
effects, it is suggested that an appropriate heat sink be used
with the CA5160. In addition, when “sinking” or “sourcing”
significant output current the chip temperature increases,
causing an increase in the input current. In such cases, heat-
sinking can also very markedly reduce and stabilize input
current variations.
10
7.5
5
2.5
0-101234567
INPUT CURRENT (pA)
INPUT VOLTAGE (V)
TA = 25oC
15V
TO
5V
V+
V-
0V
TO
-10V
CA5160
2
3
6
7
8
4
PA
VIN
FIGURE 1. CA5160 INPUT CURRENT vs COMMON MODE
VOLTAGE
CA5160, CA5160A