AD743JRZ-16-REEL7

REV. E
AD743
–9–
HOW CHIP PACKAGE TYPE AND POWER DISSIPATION
AFFECT INPUT BIAS CURRENT
As with all JFET input amplifiers, the input bias current of
the AD743 is a direct function of device junction temperature,
I
B
approximately doubling every 10°C. Figure 8 shows the rela-
tionship between the bias current and the junction temperature
for the AD743. This graph shows that lowering the junction
temperature will dramatically improve I
B
.
–60 –40 –20 0 20 40 60 80 100 120 140
10
–12
10
–11
10
–10
10
–9
10
–8
10
–7
10
–6
INPUT BIAS CURRENT (A)
JUNCTION TEMPERATURE (C)
T
A
= 25C
V
S
= ±15V
Figure 8. Input Bias Current vs. Junction Temperature
The dc thermal properties of an IC can be closely approximated
by using the simple model of Figure 9, where current represents
power dissipation, voltage represents temperature, and resistors
represent thermal resistance ( in °C/W).
T
A
P
IN
P
IN
= DEVICE DISSIPATION
T
A
= AMBIENT TEMPERATURE
T
J
= JUNCTION TEMPERATURE
JC
= THERMAL RESISTANCE—JUNCTION TO CASE
CA
= THERMAL RESISTANCE—CASE TO AMBIENT
JA
T
J
CA
JC
Figure 9. Device Thermal Model
From this model, T
J
= T
A
+
JA
P
IN
. Therefore, I
B
can be deter-
mined in a particular application by using Figure 8 together with
the published data for
JA
and power dissipation. The user can
modify
JA
by using of an appropriate clip-on heat sink, such as
the Aavid No. 5801.
JA
is also a variable when using the AD743
in chip form. Figure 10 shows the bias current versus the supply
voltage with
JA
as the third variable. This graph can be used to
predict bias current after
JA
has been computed. Again, bias cur-
rent will double for every 10°C. The designer using the AD743
in chip form (Figure 11) must also be concerned with both
JC
and
CA
, since
JC
can be affected by the type of die mount
technology used.
Typically,
JC
will be in the 3°C/W to 5°C/W range; therefore,
for normal packages, this small power dissipation level may be
ignored. But, with a large hybrid substrate,
JC
will dominate
proportionately more of the total
JA
.
SUPPLY VOLTAGE ( V)
300
0
51510
INPUT BIAS CURRENT (pA)
200
100
T
A
= +25 C
JA
= 165 C/W
JA
= 0 C/W
JA
= 115 C/W
Figure 10. Input Bias Current vs. Supply Voltage
for Various Values of
JA
(DIE MOUNT
TO CASE)
(J TO
DIE MOUNT)
A
A
+
B
=
JC
B
CASE
T
A
T
J
Figure 11. Breakdown of Various Package Thermal
Resistances
REDUCED POWER SUPPLY OPERATION FOR LOWER I
B
Reduced power supply operation lowers I
B
in two ways: first, by
lowering both the total power dissipation and second, by reduc-
ing the basic gate-to-junction leakage (Figure 10). Figure 12
shows a 40 dB gain piezoelectric transducer amplifier, which
operates without an ac-coupling capacitor over the –40°C to
+85°C temperature range. If the optional coupling capacitor is
used, this circuit will operate over the entire –55°C to +125°C
military temperature range.
AD743
*OPTIONAL DC BLOCKING CAPACITOR
**OPTIONAL, SEE TEXT
TRANSDUCER
C
T
C1*
CT**
10k
100
10
8
**
10
8
+5V
–5V
Figure 12. Piezoelectric Transducer
REV. E–10–
AD743
AN INPUT IMPEDANCE COMPENSATED, SALLEN-KEY
FILTER
The simple high-pass filter of Figure 13 has an important source
of error which is often overlooked. Even 5 pF of input capacitance
in amplifier A will contribute an additional 1% of pass-band ampli-
tude error, as well as distortion, proportional to the C/V characteristics
of the input junction capacitance. The addition of the network
designated Z will balance the source impedance—as seen by
A—and thus eliminate these errors.
A
500k
500k
1000pF1000pF
+V
S
–V
S
Z
1000pF
1000pF
500k
500k
Z
Figure 13. Input Impedance Compensated
Sallen-Key Filter
TWO HIGH PERFORMANCE ACCELEROMETER
AMPLIFIERS
Two of the most popular charge-out transducers are hydrophones
and accelerometers. Precision accelerometers are typically cali-
brated for a charge output (pC/g).* Figures 14a and 14b show
two ways in which to configure the AD743 as a low noise charge
amplifier for use with a wide variety of piezoelectric accelerom-
eters. The input sensitivity of these circuits will be determined
by the value of capacitor C1 and is equal to
V
Q
C
OUT
OUT
=
1
The ratio of capacitor C1 to the internal capacitance (C
T
) of the
transducer determines the noise gain of this circuit (1 + C
T
/C1).
The amplifier’s voltage noise will appear at its output amplified
by this amount. The low frequency bandwidth of these circuits
will be dependent on the value of resistor R1. If a T network is
used, the effective value is R1(1 + R2/R3).
AD743
R2
9k
R1
110M
(5 22M)
OUTPUT
0.8mV/pC*
C1
1250pF
R3
1k
B AND K MODEL
4370 OR
EQUIVALENT
*pC = PICOCOULOMBS
g = EARTH’S GRAVITATIONAL CONSTANT
Figure 14a. Basic Accelerometer Circuit
AD743
R3
1k
R2
9k
R4
18M
R1
110M
(5 22M)
R5
18M
OUTPUT
0.8mV/pC
C1
1250pF
C3
2.2F
C2
2.2F
B AND K MODEL
4370 OR
EQUIVALENT
AD711
Figure 14b. Accelerometer Circuit Using a DC
Servo Amplifier
A dc servo loop (Figure 14b) can be used to assure a dc output
which is <10 mV, without the need for a large compensating
resistor when dealing with bias currents as large as 100 nA. For
optimal low frequency performance, the time constant of the
servo loop (R4C2 = R5C3) should be
Time Cons R
R
R
Ctant ≥+
10 1 1
2
3
1
LOW NOISE HYDROPHONE AMPLIFIER
Hydrophones are usually calibrated in the voltage out mode.
The circuits of Figures 15a and 15b can be used to amplify the
output of a typical hydrophone. Figure 15a shows a typical
dc-coupled circuit. The optional resistor and capacitor serve
to counteract the dc offset caused by bias currents flowing through
resistor R1. Figure 15b, a variation of the original circuit, has a
low frequency cutoff determined by an RC time constant equal to
Time Cons t
C
C
tan =
××
1
2 100πΩ
R2
1900
R4*
10
8
R1
10
8
R3
100
OUTPUT
AD743
*OPTIONAL, SEE TEXT
INPUT SENSITIVITY = –179 dB re. 1V/Pa**
**1V PER MICROPASCAL
B AND K TYPE 8100
HYDROPHONE
C
T
C1*
Figure 15a. Basic Hydrophone Amplifier
REV. E
AD743
–11–
R2
1900
R4*
R1
10
8
R3
100
OUTPUT
AD743
*OPTIONAL, SEE TEXT
INPUT SENSITIVITY = –179 dB re. 1V/Pa**
**1V PER MICROPASCAL
B AND K TYPE 8100
HYDROPHONE
C
T
C
C
C1*
Figure 15b. AC-Coupled, Low Noise
Hydrophone Amplifier
R5
100k
R1
10
8
R4*
10
8
OUTPUT
DC OUTPUT 1mV FOR I
B
(AD743) 100nA
C
T
C1*
AD743
R2
1900
R6
1M
R7
16M
16M
*OPTIONAL, SEE TEXT
C2
0.27F
R3
100
B AND K
TYPE 8100
HYDROPHONE
AD711K
Figure 15c. Hydrophone Amplifier Incorporating a
DC Servo Loop
where the dc gain is 1 and the gain above the low frequency cutoff
(1/(2πC
C
(100 ))) is the same as the circuit of Figure 15a. The
circuit of Figure 15c uses a dc servo loop to keep the dc output
at 0 V and to maintain full dynamic range for I
B
up to 100 nA.
The time constant of R7 and C2 should be larger than that of
R1 and C
T
for a smooth low frequency response.
The transducer shown has a source capacitance of 7500 pF. For
smaller transducer capacitances (300 pF), the lowest noise can
be achieved by adding a parallel RC network (R4 = R1, C1 = C
T
)
in series with the inverting input of the AD743.
BALANCING SOURCE IMPEDANCES
As mentioned previously, it is good practice to balance the
source impedances (both resistive and reactive) as seen by the
inputs of the AD743. Balancing the resistive components will
optimize dc performance over temperature because balancing
will mitigate the effects of any bias current errors. Balancing
input capacitance will minimize ac response errors due to the
amplifier’s input capacitance and, as shown in Figure 16, noise
performance will be optimized. Figure 17 shows the required
external components for noninverting (A) and inverting (B)
configurations.
INPUT CAPACITORS (pF)
RTI VOLTAGE NOISE (nV/Hz)
40
30
20
10
10 100 1000
UNBALANCED
BALANCED
2.9nV/Hz
Figure 16. RTI Voltage Noise vs. Input Capacitance
OUTPUT
R1
R2
R
B
C
B
C
S
R
S
NONINVERTING
CONNECTION
A
A
C
B
= C
S
R
B
= R
S
FOR
R
S
>> R1 OR R2
OUTPUT
R1
C
S
C
F
C
B
R
S
R
B
INVERTING
CONNECTION
B
B
C
B
= C
F
C
S
R
B
= R1 R
S
Figure 17. Optional External Components for Balancing Source Impedances

AD743JRZ-16-REEL7

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Precision Amplifiers LOW NOISE BIFET IC
Lifecycle:
New from this manufacturer.
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