5
transistor Q11 and its cascode-connected load resistance
provided by PMOS transistors Q3and 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 2kΩresistor connected between the base
and collector of transistor Q11. These internal components
provide sufficient compensation for unity gain operation in
most applications. Ho w ev er, additional compensation, if
desired, ma y be used betw een Terminals 1 and 8.
Bias-Source Cir cuit - At total supply v oltages , some what
above 8.3V, resistor R2and zener diode Z1serve to establish a
voltage of 8.3V across the series-connected circuit, consisting
of resistor R1, diodes D1through 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 f or PMOS transistors Q4 and
Q5 with respect to Terminal 7. A potential of about 2.2V is
de v eloped 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, Q3 are designed to
be identical, the approximately 200µA current in Q1establishes
a similar current in Q2 and Q3 as constant-current sources for
both the first and second amplifier stages, respectiv ely.
At total supply voltages somewhat less than 8.3V, zener diode
Z1 becomes nonconductive and the potential, de veloped
across series-connected R1, D1 - D4, and Q1, varies directly
with variations in supply v oltage. Consequently, the gate bias
f or Q4, Q5 and Q2, Q3 varies in accordance with supply-
voltage variations. This variation results in deterioration of the
power-supply-rejection r atio (PSRR) at total supply voltages
below 8.3V. Operation at total supply voltages below about
4.5V results in seriously degraded perf ormance.
Output Stage - The output stage consists of a drain-loaded
inv erting amplifier using CMOS transistors operating in the
Class A mode. When operating into very high resistance loads,
the output can be s wung within milliv olts of either supply rail.
Because the output stage is a drain-loaded amplifier, its gain is
dependent upon the load impedance. The transfer
characteristics of the output stage for a load returned to the
negative supply r ail are sho wn in Figure 17. Typical op amp
loads are readily driven b y the output stage. Because large-
signal e xcursions are non-linear, requiring feedbac k f or good
wa v eform reproduction, transient delays may be encountered.
As a voltage follower, the amplifier can achieve 0.01% accuracy
le v els , including the negativ e 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
effected with the slider arm positioned in the mid-point of the
potentiometer's total range.
Input Current Variation with Common Mode Input
Voltage
As shown in the Electrical Specifications, the input current f or
the CA3160 Series Op Amps is typically 5pA at TA = 25oC
when Terminals 2 and 3 are at a common-mode potential of
+7.5V with respect to negative supply Terminal 4. Figure 23
contains data showing the v ariation of input current as a
function of common-mode input voltage at TA=25
oC. These
data show that circuit designers can adv antageously 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 pre viously noted, the
input current is essentially the result of the leakage current
through the gate-protection diodes in the input circuit and,
theref ore, 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 f actors. Because the gate-
protection network functions as if it is connected to Terminal 4
potential, and the metal can case of the CA3160 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 CA3160 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 24 provides data on the typical v ariation of input bias
current as a function of temperature in the CA3160.
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
CA3160. 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.
Input Offset Voltage (V
IO
) Variation with DC Bias
vs Device Operating Life
It is well known that the char acteristics of a MOSFET device
can change slightly when a DC gate-source bias potential is
applied to the device for extended time periods. The magnitude
of the change is increased at high temperatures. Users of the
CA3160 should be alert to the possible impacts of this eff ect if
the application of the de vice in v olv es extended operation at
high temperatures with a significant differential DC bias voltage
applied across Terminals 2 and 3. Figure 25 shows typical data
pertinent to shifts in offset voltage encountered with CA3160
de vices in metal can pac kages during life testing. At lo w er
temperatures (metal can and plastic) f or example at 85oC, this
change in voltage is consider ab ly less . In typical linear
applications where the diff erential v oltage is small and
symmetrical, these incremental changes are of about the same
CA3160, CA3160A