AD844JRZ-16 Analog Devices Inc, AD844JRZ-16 Datasheet - Page 9

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AD844JRZ-16

Manufacturer Part Number
AD844JRZ-16
Description
IC OPAMP CF 60MHZ 80MA 16SOIC
Manufacturer
Analog Devices Inc
Datasheets

Specifications of AD844JRZ-16

Slew Rate
2000 V/µs
Amplifier Type
Current Feedback
Number Of Circuits
1
-3db Bandwidth
60MHz
Current - Input Bias
200pA
Voltage - Input Offset
50µV
Current - Supply
6.5mA
Current - Output / Channel
80mA
Voltage - Supply, Single/dual (±)
±4.5 V ~ 18 V
Operating Temperature
0°C ~ 70°C
Mounting Type
Surface Mount
Package / Case
16-SOIC (0.300", 7.5mm Width)
Op Amp Type
High Speed
No. Of Amplifiers
1
Bandwidth
60MHz
Supply Voltage Range
± 4.5V To ± 18V
Amplifier Case Style
SOIC
No. Of Pins
16
Operating Temperature Range
0°C To
Lead Free Status / RoHS Status
Lead free / RoHS Compliant
Output Type
-
Gain Bandwidth Product
-
Lead Free Status / RoHS Status
Lead free / RoHS Compliant, Lead free / RoHS Compliant

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Part Number
Manufacturer
Quantity
Price
Part Number:
AD844JRZ-16
Manufacturer:
ADI
Quantity:
184
Part Number:
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Manufacturer:
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Quantity:
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Gain
–1
–1
–2
–2
–5
–5
–10
–10
–20
–100
+100
Response as an I-V Converter
The AD844 works well as the active element in an operational
current-to-voltage converter, used in conjunction with an exter-
nal scaling resistor, R1, in Figure 3. This analysis includes the
stray capacitance, C
high speed DAC. Using a conventional op amp, this capacitance
forms a “nuisance pole” with R1 that destabilizes the closed-
loop response of the system. Most op amps are internally com-
pensated for the fastest response at unity gain, so the pole due
to R1 and C
system. For example, if R1 were 2.5 kΩ, a C
place this pole at a frequency of about 4 MHz, well within the
response range of even a medium speed operational amplifier.
In a current feedback amp, this nuisance pole is no longer deter-
mined by R1 but by the input resistance, R
50 Ω for the AD844, the same 15 pF forms a pole at 212 MHz
and causes little trouble. It can be shown that the response of
this system is:
where K is a factor very close to unity and represents the finite
dc gain of the amplifier, Td is the dominant pole, and Tn is the
nuisance pole:
Using typical values of R1 = 1 kΩ and R
in other words, the “gain error” is only 0.03%. This is much less
than the scaling error of virtually all DACs and can be absorbed,
if necessary, by the trim needed in a precise system.
In the AD844, R
voltages, and consequently the effect of finite “gain” is negli-
gible unless high value feedback resistors are used. Since that
would result in slower response times than are possible, the
relatively low value of R
cant source of error.
REV. E
Td = KR1C
Tn = R
K
=
R
t
IN
R
+ 1
C
R1
1 kΩ
500 Ω
2 kΩ
1 kΩ
5 kΩ
500 Ω
1 kΩ
500 Ω
1 kΩ
5 kΩ
5 kΩ
t
R
S
S
t
reduces the already narrow phase margin of the
(assuming R
V
t
OUT
is fairly stable with temperature and supply
S
, of the current source, which might be a
R2
1 kΩ
500 Ω
1 kΩ
500 Ω
1 kΩ
100 Ω
100 Ω
50 Ω
50 Ω
50 Ω
50 Ω
=
t
in the AD844 will rarely be a signifi-
I
IN
sig
Table I.
<< R1)
(
1
+
s
BW (MHz) GBW (MHz)
35
60
15
30
5.2
49
23
33
21
3.2
9
Td
K R
)(
1
t
1
+
= 3 MΩ, K is 0.9997;
IN
s
Tn
. Since this is about
)
S
of 15 pF would
35
60
30
60
26
245
230
330
420
320
900
–9–
Circuit Description of the AD844
A simplified schematic is shown in Figure 4. The AD844 differs
from a conventional op amp in that the signal inputs have
radically different impedance. The noninverting input (Pin 3)
presents the usual high impedance. The voltage on this input is
transferred to the inverting input (Pin 2) with a low offset
voltage, ensured by the close matching of like polarity transis-
tors operating under essentially identical bias conditions. Laser
trimming nulls the residual offset voltage, down to a few
tens of microvolts. The inverting input is the common emitter
node of a complementary pair of grounded base stages and
behaves as a current summing node. In an ideal current feed-
back op amp, the input resistance would be zero. In the AD844,
it is about 50 Ω.
A current applied to the inverting input is transferred to a
complementary pair of unity-gain current mirrors that deliver
the same current to an internal node (Pin 5) at which the full
output voltage is generated. The unity-gain complementary
voltage follower then buffers this voltage and provides the load
driving power. This buffer is designed to drive low impedance
loads, such as terminated cables, and can deliver ± 50 mA into a
50 Ω load while maintaining low distortion, even when operat-
ing at supply voltages of only ± 6 V. Current limiting (not
shown) ensures safe operation under short circuited conditions.
+IN
3
Figure 3. Current-to-Voltage Converter
I
I
B
B
I
SIG
Figure 4. Simplified Schematic
C
S
2
–IN
TZ
AD844
5
R1
R
L
AD844
C
V
L
OUT
7
6
4
+V
OUT
–V
S
S

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