33 MHz at gain of −10
Slew rate: 2000 V/μs
20 MHz full power bandwidth, 20 V p-p, R
Fast settling: 100 ns to 0.1% (10 V step)
Differential gain error: 0.03% at 4.4 MHz
Differential phase error: 0.16° at 4.4 MHz
Low offset voltage: 150 μV maximum (B Grade)
Low quiescent current: 6.5 mA
Available in tape and reel in accordance with
EIA-481-A standard
APPLICATIONS
Flash ADC input amplifiers
High speed current DAC interfaces
Video buffers and cable drivers
Pulse amplifiers
= 500 Ω
L
Monolithic Op Amp
AD844
FUNCTIONAL BLOCK DIAGRAMS
1
NULL
–IN
+IN
–V
Figure 1. 8-Lead PDIP (N) and 8-Lead CERDIP (Q) Packages
OFFSETNULL
Figure 2. 16-Lead SOIC (R) Package
AD844
2
3
4
S
TOP VIEW
(Not to Scale)
NC
1
2
3
–IN
4
NC
512
+IN
NC
611
AD844
710
V–
TOP VIEW
89
NC
(Not to Scale)
NC = NO CO NNECT
8
NULL
7
+V
S
OUTPUT
6
TZ
5
16
NC
15
OFFSETNULL
14
V+
13
NC
OUTPUT
TZ
NC
NC
00897-001
00897-002
GENERAL DESCRIPTION
The AD844 is a high speed monolithic operational amplifier
fabricated using the Analog Devices, Inc., junction isolated
complementary bipolar (CB) process. It combines high bandwidth and very fast large signal response with excellent dc
performance. Although optimized for use in current-to-voltage
applications and as an inverting mode amplifier, it is also suitable
for use in many noninverting applications.
The AD844 can be used in place of traditional op amps, but its
current feedback architecture results in much better ac performance, high linearity, and an exceptionally clean pulse response.
This type of op amp provides a closed-loop bandwidth that is
determined primarily by the feedback resistor and is almost
independent of the closed-loop gain. The AD844 is free from
the slew rate limitations inherent in traditional op amps and
other current-feedback op amps. Peak output rate of change can
be over 2000 V/μs for a full 20 V output step. Settling time is
typically 100 ns to 0.1%, and essentially independent of gain.
The AD844 can drive 50 Ω loads to ±2.5 V with low distortion
and is short-circuit protected to 80 mA.
The AD844 is available in four performance grades and three
package options. In the 16-lead SOIC (RW) package, the AD844J
is specified for the commercial temperature range of 0°C to 70°C.
The AD844A and AD844B are specified for the industrial
temperature range of −40°C to +85°C and are available in the
CERDIP (Q) package. The AD844A is also available in an 8-lead
PDIP (N). The AD844S is specified over the military temperature
range of −55°C to +125°C. It is available in the 8-lead CERDIP
(Q) package. A and S grade chips and devices processed to
MIL-STD-883B, Rev. C are also available.
PRODUCT HIGHLIGHTS
1. The AD844 is a versatile, low cost component providing an
excellent combination of ac and dc performance.
2. It is essentially free from slew rate limitations. Rise and fall
times are essentially independent of output level.
3. The AD844 can be operated from ±4.5 V to ±18 V power
supplies and is capable of driving loads down to 50 Ω, as
well as driving very large capacitive loads using an external
network.
4. The offset voltage and input bias currents of the AD844 are
laser trimmed to minimize dc errors; V
μV/°C and bias current drift is typically 9 nA/°C.
5. The AD844 exhibits excellent differential gain and
differential phase characteristics, making it suitable for a
variety of video applications with bandwidths up to 60 MHz.
6. The AD844 combines low distortion, low noise, and low
drift with wide bandwidth, making it outstanding as an
input amplifier for flash analog-to-digital converters (ADCs).
drift is typically 1
OS
Rev. F
Information furnished by Analog Devices is believed to be accurate and reliable. However, no
responsibility is assumed by Analog Devices for its use, nor for any infringements of patents or other
rights of third parties that may result from its use. Specifications subject to change without notice. No
license is granted by implication or otherwise under any patent or patent rights of Analog Devices.
Trademarks and registered trademarks are the property of their respective owners.
Stresses above those listed under Absolute Maximum Ratings
may cause permanent damage to the device. This is a stress
rating only; functional operation of the device at these or any
other conditions above those indicated in the operational
section of this specification is not implied. Exposure to absolute
maximum rating conditions for extended periods may affect
device reliability.
METALLIZATION PHOTOGRAPH
Contact factory for latest dimensions.
Dimensions shown in inches and (millimeters).
INNULLNULL+
0.076
(1.9)
+IN–V
SUBSTRAT E CONNECTED T O +V
Figure 3. Die Photograph
S
0.095
(2.4)
TZOUTPUT
ESD CAUTION
S
S
00897-003
Rev. F | Page 5 of 20
AD844
TYPICAL PERFORMANCE CHARACTERISTICS
TA = 25°C and VS = ±15 V, unless otherwise noted.
70
20
= 25°C
T
A
60
50
–3dB BANDWIDTH ( MHz)
40
30
SUPPLY VOLTAGE (±V)
Figure 4. −3 dB Bandwidth vs. Supply Voltage, R1 = R2 = 500 Ω
Figure 7. Noninverting Input Voltage Swing vs. Supply Voltage
20
= 500Ω
R
L
T
= 25°C
A
15
10
OUTPUT VOLTAGE (V)
5
0
00897-005
SUPPLY VOLTAGE (±V)
20051015
00897-008
Figure 8. Output Voltage Swing vs. Supply Voltage
10
9
8
7
6
SUPPLY CURRENT (mA)
5
VS = ±15V
VS = ±5V
0
–50050100150
TEMPERATURE (° C)
Figure 6. Transresistance vs. Temperature
00897-006
Rev. F | Page 6 of 20
4
TEMPERATURE ( -°C)
140–60 –40 –20020406080 10 0 120
Figure 9. Quiescent Supply Current vs. Temperature and Supply Voltage
00897-009
AD844
2
1
0
–1
INPUT BIAS CURRENT (µA)
–2
–50050100150
TEMPERATURE (° C)
I
BP
I
BN
Figure 10. Inverting Input Bias Current (IBN) and Noninverting Input Bias
Current (I
100
10
1
) vs. Temperature
BP
±5V SUPPLIES
40
35
30
25
20
–3dB BANDWIDTH ( MHz)
15
10
00897-010
VS = ±15V
VS = ±5V
TEMPERATURE (-°C)
140–60 –40 –20020406080100 120
0897-012
Figure 12. –3 dB Bandwidth vs. Temperature, Gain = −1, R1 = R2 = 1 kΩ
OUTPUT IMPEDANCE (Ω)
0.1
0.01
10k100k1M10M100M
FREQUENCY (Hz)
Figure 11. Output Impedance vs. Frequency, Gain = −1, R1 = R2 = 1 kΩ
00897-011
Rev. F | Page 7 of 20
AD844
V
–
INVERTING GAIN-OF-1 AC CHARACTERISTICS
+
0.22µF
S
4.7Ω
R1
5V
100
90
–IN
R2
–
AD844
+
0.22µF
–V
OUTPUT
R
L
4.7Ω
S
C
L
00897-013
Figure 13. Inverting Amplifier, Gain of −1 (R1 = R2)
6
R1 = R2 = 500Ω
0
–6
GAIN (dB)
–12
–18
–24
FREQUENCY (Hz)
R1 = R2 = 1kΩ
100M1M100k10M
Figure 14. Gain vs. Frequency for Gain = −1, RL = 500 Ω, CL = 0 pF
180
10
0
20ns
0897-016
Figure 16. Large Signal Pulse Response, Gain = −1, R1 = R2 = 1 kΩ
500nV
100
90
10
0
20ns
00897-014
Figure 17. Small Signal Pulse Response, Gain = −1, R1 = R2 = 1 kΩ
0897-017
–210
–240
–270
PHASE (Degrees)
–300
–330
R1 = R2 = 1kΩ
FREQUENCY (MHz )
R1 = R2 = 500Ω
25
Figure 15. Phase vs. Frequency for Gain = −1, RL = 500 Ω, CL = 0 pF
500
00897-015
Rev. F | Page 8 of 20
AD844
V
–
INVERTING GAIN-OF-10 AC CHARACTERISTICS
180
–210
R
= 50Ω
L
RL = 500Ω
0.22µF
+
4.7Ω
500Ω
S
–IN
50Ω
–
AD844
+
0.22µF
–V
OUTPUT
R
L
4.7Ω
S
C
L
00897-018
Figure 18. Gain of −10 Amplifier
26
RL = 500Ω
20
= 50Ω
R
14
L
PHASE (Degrees)
–240
–270
–300
–330
25
FREQUENCY (MHz)
Figure 20. Phase vs. Frequency, Gain = −10
500
00897-020
GAIN (dB)
8
2
–4
FREQUENCY (Hz)
100M1M100k10M
00897-019
Figure 19. Gain vs. Frequency, Gain = −10
Rev. F | Page 9 of 20
AD844
INVERTING GAIN-OF-10 PULSE RESPONSE
5V
100
90
10
0
20ns
Figure 21. Large Signal Pulse Response, Gain = –10, RL = 500 Ω
500nV
100
90
10
0
0897-021
20ns
0897-022
Figure 22. Small Signal Pulse Response, Gain = −10, RL = 500 Ω
Rev. F | Page 10 of 20
AD844
–
NONINVERTING GAIN-OF-10 AC CHARACTERISTICS
4.7Ω
+V
50Ω
–IN
S
–V
S
–
AD844
+
4.7Ω
0.22µF
450Ω
0.22µF
100
90
OUTPUT
R
L
C
L
10
00897-023
0
2V
100ns
GAIN (dB)
Figure 23. Noninverting Gain of +10 Amplifier
26
20
14
8
2
–4
FREQUENCY (Hz)
Figure 24. Gain vs. Frequency, Gain = +10
180
–210
–240
R
= 50Ω
L
RL = 500Ω
Figure 26. Noninverting Amplifier Large Signal Pulse Response, Gain = +10,
00897-026
= 500 Ω
R
L
200nV50ns
RL = 500ΩRL = 50Ω
100M1M100k10M
00897-024
100
90
10
0
Figure 27. Small Signal Pulse Response, Gain = +10, R
= 500 Ω
L
00897-027
–270
PHASE (Degrees)
–300
–330
25
FREQUENCY (MHz)
500
00897-025
Figure 25. Phase vs. Frequency, Gain = +10
Rev. F | Page 11 of 20
AD844
UNDERSTANDING THE AD844
The AD844 can be used in ways similar to a conventional op
amp while providing performance advantages in wideband
applications. However, there are important differences in the
internal structure that need to be understood to optimize the
performance of the AD844 op amp.
OPEN-LOOP BEHAVIOR
Figure 28 shows a current feedback amplifier reduced to essentials. Sources of fixed dc errors, such as the inverting node bias
current and the offset voltage, are excluded from this model.
The most important parameter limiting the dc gain is the
transresistance, R
is analogous to the finite open-loop voltage gain in a conventional op amp.
, which is ideally infinite. A finite value of Rt
t
RESPONSE AS AN INVERTING AMPLIFIER
Figure 29 shows the connections for an inverting amplifier.
Unlike a conventional amplifier, the transient response and the
small signal bandwidth are determined primarily by the value of
the external feedback resistor, R1, rather than by the ratio of
R1/R2 as is customarily the case in an op amp application. This
is a direct result of the low impedance at the inverting input. As
with conventional op amps, the closed-loop gain is −R1/R2.
The closed-loop transresistance is the parallel sum of R1 and R
Because R1 is generally in the range of 500 Ω to 2 kΩ and R
about 3 MΩ, the closed-loop transresistance is only 0.02% to
0.07% lower than R1. This small error is often less than the
resistor tolerance.
t
is
t
.
The current applied to the inverting input node is replicated by
the current conveyor to flow in Resistor R
across R
gain is the ratio R
R
is buffered by the unity gain voltage follower. Voltage
t
. With typical values of Rt = 3 MΩ and
t/RIN
= 50 Ω, the voltage gain is about 60,000. The open-loop
IN
. The voltage developed
t
current gain, another measure of gain that is determined by the
beta product of the transistors in the voltage follower stage (see
Figure 31), is typically 40,000.
+1
I
IN
R
IN
I
IN
Figure 28. Equivalent Schematic
R
t
C
t
+1
The important parameters defining ac behavior are the
transcapacitance, C
, and the external feedback resistor (not
t
shown). The time constant formed by these components is
analogous to the dominant pole of a conventional op amp and
thus cannot be reduced below a critical value if the closed-loop
system is to be stable. In practice, C
is held to as low a value as
t
possible (typically 4.5 pF) so that the feedback resistor can be
maximized while maintaining a fast response. The finite R
IN
also affects the closed-loop response in some applications.
The open-loop ac gain is also best understood in terms of the
transimpedance rather than as an open-loop voltage gain. The
open-loop pole is formed by R
in parallel with Ct. Because Ct is
t
typically 4.5 pF, the open-loop corner frequency occurs at about
12 kHz. However, this parameter is of little value in determining
the closed-loop response.
When R1 is fairly large (above 5 kΩ) but still much less than R
,
t
the closed-loop HF response is dominated by the time constant
R1 C
. Under such conditions, the AD844 is overdamped and
t
provides only a fraction of its bandwidth potential. Because of
the absence of slew rate limitations under these conditions, the
circuit exhibits a simple single-pole response even under large
signal conditions.
In Figure 29, R3 is used to properly terminate the input if desired.
R3 in parallel with R2 gives the terminated resistance. As R1 is
lowered, the signal bandwidth increases, but the time constant
R1 C
becomes comparable to higher order poles in the closed-
t
loop response. Therefore, the closed-loop response becomes
complex, and the pulse response shows overshoot. When R2
00897-028
is much larger than the input resistance, R
the feedback current in R1 is delivered to this input, but as R2
becomes comparable to R
, less of the feedback is absorbed at
IN
, at Pin 2, most of
IN
Pin 2, resulting in a more heavily damped response. Consequently,
for low values of R2, it is possible to lower R1 without causing
instability in the closed-loop response. Tabl e 3 lists combinations
of R1 and R2 and the resulting frequency response for the circuit
of Figure 29. Figure 16 shows the very clean and fast ±10 V
pulse response of the AD844.
R1
V
IN
OPTIONAL
R2
R3
Figure 29. Inverting Amplifier
AD844
R
L
V
OUT
C
L
0897-029
Rev. F | Page 12 of 20
AD844
K
+
Table 3. Gain vs. Bandwidth
Gain R1 R2 BW (MHz) GBW (MHz)
−1 1 kΩ 1 kΩ 35 35
−1 500 Ω 500 Ω 60 60
−2 2 kΩ 1 kΩ 15 30
−2 1 kΩ 500 Ω 30 60
−5 5 kΩ 1 kΩ 5.2 26
−5 500 Ω 100 Ω 49 245
−10 1 kΩ 100 Ω 23 230
−10 500 Ω 50 Ω 33 330
−20 1 kΩ 50 Ω 21 420
−100 5 kΩ 50 Ω 3.2 320
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 external scaling resistor, R1, in Figure 30. 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 compensated
for the fastest response at unity gain, so the pole due to R1 and
C
reduces the already narrow phase margin of the system. For
S
example, if R1 is 2.5 kΩ, a C
quency 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 determined by R1 but by the
input resistance, R
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:
OUT
where:
K is a factor very close to unity and represents the finite dc gain
of the amplifier.
Td is the dominant pole.
Tn is the nuisance pole.
K
=
t
Td = KR1C
Tn = RINCS (assuming RIN << R1)
, of the current source, which may be a
S
of 15 pF places this pole at a fre-
S
. Because this is about 50 Ω for the AD844,
IN
IV++=
sig
R
t
1RR
+
t
R1
()
()
Td
ss
11
Tn
R1
I
SIG
C
S
Figure 30. Current-to-Voltage Converter
AD844
R
L
V
OUT
C
L
0897-030
CIRCUIT DESCRIPTION OF THE AD844
A simplified schematic is shown in Figure 31. 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 transistors 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 feedback op amp, the input resistance
is 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 operating
at supply voltages of only ±6 V. Current limiting (not shown)
ensures safe operation under short-circuited conditions.
+V
7
S
I
B
INOUTPUT
I
B
–IN
TZ
6523
–V
Using typical values of R1 = 1 kΩ and R
= 3 MΩ, K = 0.9997; in
t
other words, the gain error is only 0.03%. This is much less than
Figure 31. Simplified Schematic
4
S
0897-031
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
is fairly stable with temperature and supply
t
voltages, and consequently the effect of finite gain is negligible
unless high value feedback resistors are used. Because that
results in slower response times than are possible, the relatively
low value of R
in the AD844 is rarely a significant source of error.
t
Rev. F | Page 13 of 20
AD844
V
It is important to understand that the low input impedance at
the inverting input is locally generated and does not depend on
feedback. This is very different from the virtual ground of a
conventional operational amplifier used in the current summing
mode, which is essentially an open circuit until the loop settles.
In the AD844, transient current at the input does not cause
voltage spikes at the summing node while the amplifier is
settling. Furthermore, all of the transient current is delivered
to the slewing (TZ) node (Pin 5) via a short signal path (the
grounded base stages and the wideband current mirrors).
NONINVERTING GAIN OF 100
The AD844 provides very clean pulse response at high
noninverting gains. Figure 32 shows a typical configuration
providing a gain of 100 with high input resistance. The feedback
resistor is kept as low as practicable to maximize bandwidth,
and a peaking capacitor (C
further extend the bandwidth. Figure 33 shows the small signal
response with C
= 3 nF, RL = 500 Ω, and supply voltages of
PK
either ±5 V or ±15 V. Gain bandwidth products of up to
900 MHz can be achieved in this way.
) can optionally be added to
PK
The current available to charge the capacitance (about 4.5 pF) at
the TZ node is always proportional to the input error current,
and the slew rate limitations associated with the large signal
response of the op amps do not occur. For this reason, the rise
and fall times are almost independent of signal level. In practice,
the input current eventually causes the mirrors to saturate.
When using ±15 V supplies, this occurs at about 10 mA (or
±2200 V/μs). Because signal currents are rarely this large,
classical slew rate limitations are absent.
This inherent advantage is lost if the voltage follower used
to buffer the output has slew rate limitations. The AD844 is
designed to avoid this problem, and as a result, the output
buffer exhibits a clean large signal transient response, free
from anomalous effects arising from internal saturation.
RESPONSE AS A NONINVERTING AMPLIFIER
Because current feedback amplifiers are asymmetrical with
regard to their two inputs, performance differs markedly in
noninverting and inverting modes. In noninverting modes, the
large signal high speed behavior of the AD844 deteriorates at
low gains because the biasing circuitry for the input system (not
shown in Figure 31) is not designed to provide high input
voltage slew rates.
However, good results can be obtained with some care. The
noninverting input does not tolerate a large transient input; it
must be kept below ±1 V for best results. Consequently, this
mode is better suited to high gain applications (greater than
×10). Figure 23 shows a noninverting amplifier with a gain of 10
and a bandwidth of 30 MHz. The transient response is shown in
Figure 26 and Figure 27. To increase the bandwidth at higher
gains, a capacitor can be added across R2 whose value is
approximately (R1/R2) × C
.
t
The offset voltage of the AD844 is laser trimmed to the 50 μV
level and exhibits very low drift. In practice, there is an
additional offset term due to the bias current at the inverting
input (I
), which flows in the feedback resistor (R1). This can
BN
optionally be nulled by the trimming potentiometer shown in
Figure 32.
+
S
4.7Ω
OFFSET
TRIM
C
3nF
R2
4.99Ω
PK
20Ω
1
2
8
AD844
V
IN
3
4
4.7Ω
–V
S
Figure 32. Noninverting Amplifier Gain = 100, Optional Offset Trim Is Shown
46
40
34
GAIN (dB)
28
22
7
0.22µF
R1
499Ω
0.22µF
6
VS = ±15V
VS = ±5V
R
L
00897-032
16
100k1M20M10M
FREQUENCY (Hz)
00897-040
Figure 33. AC Response for Gain = 100, Configuration Shown in Figure 32
Rev. F | Page 14 of 20
AD844
USING THE AD844
BOARD LAYOUT
As with all high frequency circuits considerable care must be
used in the layout of the components surrounding the AD844.
A ground plane, to which the power supply decoupling capacitors are connected by the shortest possible leads, is essential to
achieving clean pulse response. Even a continuous ground plane
exhibits finite voltage drops between points on the plane, and
this must be kept in mind when selecting the grounding points.
In general, decoupling capacitors should be taken to a point
close to the load (or output connector) because the load
currents flow in these capacitors at high frequencies. The +IN
and −IN circuits (for example, a termination resistor and Pin 3)
must be taken to a common point on the ground plane close to
the amplifier package.
Use low impedance 0.22 μF capacitors (AVX SR305C224KAA
or equivalent) wherever ac coupling is required. Include either
ferrite beads and/or a small series resistance (approximately
4.7 Ω) in each supply line.
INPUT IMPEDANCE
At low frequencies, negative feedback keeps the resistance at the
inverting input close to zero. As the frequency increases, the
impedance looking into this input increases from near zero to
the open-loop input resistance, due to bandwidth limitations,
making the input seem inductive. If it is desired to keep the
input impedance flatter, a series RC network can be inserted
across the input. The resistor is chosen so that the parallel sum
of it and R2 equals the desired termination resistance. The capacitance is set so that the pole determined by this RC network is
about half the bandwidth of the op amp. This network is not
important if the input resistor is much larger than the termination
used, or if frequencies are relatively low. In some cases, the
small peaking that occurs without the network can be of use in
extending the −3 dB bandwidth.
AD844
Figure 34. Feedforward Network for Large Capacitive Loads
100
90
10
0
Figure 35. Driving 1000 pF C
6
5
750Ω
5V
22pF
500ns
with Feedforward Network of Figure 34
L
SETTLING TIME
Settling time is measured with the circuit of Figure 36. This
circuit employs a false summing node, clamped by the two
Schottky diodes, to create the error signal and limit the input
signal to the oscilloscope. For measuring settling time, the ratio
of R6/R5 is equal to R1/R2. For unity gain, R6 = R5 = 1 kΩ, and
= 500 Ω. For the gain of −10, R5 = 50 Ω, R6 = 500 Ω, and RL
R
L
was not used because the summing network loads the output
with approximately 275 Ω. Using this network in a unity-gain
configuration, settling time is 100 ns to 0.1% for a –5 V to +5 V
step with C
= 10 pF.
L
TO SCOPE
(TEK 7A11 FET PROBE)
V
OUT
C
L
00897-034
00897-035
DRIVING LARGE CAPACITIVE LOADS
Capacitive drive capability is 100 pF without an external network. With the addition of the network shown in Figure 34,
the capacitive drive can be extended to over 10,000 pF, limited
by internal power dissipation. With capacitive loads, the output
speed becomes a function of the overdriven output current limit.
Because this is roughly ±100 mA, under these conditions, the
maximum slew rate into a 1000 pF load is ±100 V/μs. Figure 35
shows the transient response of an inverting amplifier (R1 =
R2 = 1 kΩ) using the feedforward network shown in Figure 34,
driving a load of 1000 pF.
Rev. F | Page 15 of 20
R5
D1D2
V
IN
R3
NOTES
1. D1, D2 IN6263 O R EQUIVALENT SCHOTT KY DIODE.
R2
Figure 36. Settling Time Test Fixture
R6
AD844
R1
V
OUT
R
L
C
L
00897-036
AD844
V
V
DC ERROR CALCULATION
Figure 37 shows a model of the dc error and noise sources for
the AD844. The inverting input bias current, I
feedback resistor. I
in the resistance at Pin 3 (R
, the noninverting input bias current, flows
BP
), and the resulting voltage (plus
P
any offset voltage) appears at the inverting input. The total
error, V
Because I
, at the output is:
O
R1
()
PBP
O
and IBP are unrelated both in sign and magnitude,
BN
OS
⎛
RIVRIV
+++=1
⎜
R2
⎝
inserting a resistor in series with the noninverting input does
not necessarily reduce dc error and may actually increase it.
V
R2
N
I
NN
I
NP
R
IN
I
BN
I
BP
V
⎞
⎟
⎠
R1
OS
, flows in the
BN
R1I
+
BNINBN
IN
50Ω
HP8753A
NETWORK
ANALYZER
EXT
TRIG
SYNC OUT
HP3314A
STAIRCASE
GENERATOR
0.3
0.2
+5
2.2µF
3
7
6
2
4
2.2µF
–5V
50Ω
300Ω
300Ω
Z
= 50Ω
O
Figure 38. The AD844 as a Cable Driver
OUT
V
V
IN
IN
470Ω
RF IN
OUT
INRF OUT
HP11850C
SPLITTER
OUT
(TERMINATO R)
50Ω
OUT
Figure 39. Differential Gain/Phase Test Setup
IRE = 7.14mV
V
OUT
R
L
50Ω
CIRCUIT
UNDER
TEST
0897-038
V
OUT
0897-039
R
P
AD844
Figure 37. Offset Voltage and Noise Model for the AD844
NOISE
Noise sources can be modeled in a manner similar to the dc bias
currents, but the noise sources are I
induced noise at the output, V
2
()()()
ON
2
VRIV
, INP, VN, and the amplifier
NN
, is:
ON
2
R1
⎛
⎜
⎝
⎞
1R1I
++=
R2
+
⎟
NNNPNP
⎠
2
Overall noise can be reduced by keeping all resistor values to a
minimum. With typical numbers, R1 = R2 = 1 kΩ, R
= 2 nV/√Hz, INP = 10 pA/√Hz, INN = 12 pA/√Hz, and VON
V
N
= 0 Ω,
P
calculates to 12 nV/√Hz. The current noise is dominant in this
case, because it is in most low gain applications.
VIDEO CABLE DRIVER USING ±5 V SUPPLIES
The AD844 can be used to drive low impedance cables. Using
±5 V supplies, a 100 Ω load can be driven to ±2.5 V with low
distortion. Figure 38 shows an illustrative application that
provides a noninverting gain of +2, allowing the cable to be
reverse-terminated while delivering an overall gain of +1 to the
load. The −3 dB bandwidth of this circuit is typically 30 MHz.
Figure 39 shows a differential gain and phase test setup. In video
applications, differential-phase and differential-gain characteristics are often important. Figure 40 shows the variation in phase as
the load voltage varies. Figure 41 shows the gain variation.
0.1
DIFFERENTIAL PHASE (Degrees)
–0.1
–0.2
–0.3
0
365472
V
(IRE)
OUT
90180
00897-040
00897-037
Figure 40. Differential Phase for the Circuit of Figure 38
0.06
IRE = 7.14mV
0.04
0.02
0
–0.02
DIFFERENTIAL GAIN (%)
–0.04
–0.06
0189365472
V
(IRE)
OUT
0
00897-041
Figure 41. Differential Gain for the Circuit of Figure 38
Rev. F | Page 16 of 20
AD844
V
V
1
+15V
MSB
2
3
–15V
4
5
6
DIGITAL
INPUTS
*POWER SUPPLY BYPASS CAPACITORS.
AD568
7
8
9
10
11
LSB
12
TOP VIEW
(Not to Scale)
(VCC)
REFCOM
(VEE)
I
BPO
I
OUT
ACOM
LCOM
SPAN
SPAN
THCOM
V
24
23
22
21
20
19
R
L
18
17
16
15
14
13
TH
0.22µF*
0.22µF*
7
2
AD844
3
100pF
6
4
Figure 42. High Speed DAC Amplifier
GROUND
–5V
0.22µF*
0.22µF*
R
I
+15V
–15V
V
OUT
ANALOG
SUPPLY
GROUND
DIGITAL
SUPPLY
0897-042
HIGH SPEED DAC BUFFER
The AD844 performs very well in applications requiring currentto-voltage conversion. Figure 42 shows connections for use with
the AD568 current output DAC. In this application, the bipolar
offset is used so that the full-scale current is ±5.12 mA, which
generates an output of ±5.12 V using the 1 kΩ application resistor
on the AD568. Figure 43 shows the full-scale transient response.
Care is needed in power supply decoupling and grounding
techniques to achieve the full 12-bit accuracy and realize the
fast settling capabilities of the system. The AD568 data sheet
should be consulted for more complete details about its use.
The AD844 is an excellent choice as an output amplifier for the
AD539 multiplier, in all of its connection modes. (See the
AD539 data sheet for full details.) Figure 44 shows a simple
multiplier providing the output:
VV
V
W
where V
X
to 3.2 V (maximum), and V
±2 V full scale but capable of operation up to ±4.2 V.
The peak output in this configuration is thus ±6.7 V. Using all
four of the internal application resistors provided on the AD539
in parallel results in a feedback resistance of 1.5 kΩ, at which
value the bandwidth of the AD844 is about 22 MHz, and is
essentially independent of V
INPUTS
V
*
X
0V TO 3
*
V
Y
±2V FS
3nF
INPUT
GND
0.22µF
*VX AND VY INPUTS MAY O PTIONAL LY BE TERMI NATED;
TYPICALL Y BY USING A 50Ω OR 75Ω RESISTOR TO GROUND.
YX
−= (1)
V
2
is the gain control input, a positive voltage from 0 V
is the signal voltage, nominally
Y
. The gain at VX = 3.16 V is 4 dB.
X
+
S
AD844
7
4
10Ω
TYP +6V
AT 15µA
6
=
V
W
–V
TYP –6V
AT 15µA
OUTPUT
V
W
–V
XVY
2V
S
10Ω10Ω
0.22µF0.22µF
1
2
3
AD539
4
TOP VIEW
5
(Not to Scale)
6
7
8
10Ω
16
15
14
13
12
11
10
9
2
3
0.22µF
Figure 44. 20 MHz VGA Using the AD539
00897-044
Rev. F | Page 17 of 20
AD844
Figure 45 shows the small signal response for a 50 dB gain control
range (V
= 10 mV to 3.16 V). At small values of VX, capacitive
X
feedthrough on the PC board becomes troublesome and very
careful layout techniques are needed to minimize this problem.
A ground strip between the pins of the AD539 is helpful in this
regard. Figure 46 shows the response to a 2 V pulse on V
V
= 1 V, 2 V, and 3 V. For these results, a load resistor of 500 Ω
X
for
Y
was used and the supplies were ±9 V. The multiplier operates
from supplies between ±4.5 V and ±16.5 V.
Disconnecting Pin 9 and Pin 16 on the AD539 alters the
denominator in Equation 1 to 1 V, and the bandwidth is
approximately 10 MHz, with a maximum gain of 10 dB.
Using only Pin 9 or Pin 16 results in a denominator of 0.5 V,
a bandwidth of 5 MHz, and a maximum gain of 16 dB.
4
VX = 3.15V
–6
= 1.0V
V
X
–16
= 0.316V
V
X
–26
GAIN (dB)
–36
–46
–56
= 0.10V
V
X
= 0.032V
V
X
FREQUENCY (Hz)
60M1M100k10M
00897-045
Figure 45. VGA AC Response
1V1V50ns
100
90
10
0
00897-046
Figure 46. VGA Transient Response with V
= 1 V, 2 V, and 3 V
X
Rev. F | Page 18 of 20
AD844
OUTLINE DIMENSIONS
0.400 (10.16)
0.365 (9.27)
0.355 (9.02)
0.210 (5.33)
0.150 (3.81)
0.130 (3.30)
0.115 (2.92)
0.022 (0.56)
0.018 (0.46)
0.014 (0.36)
MAX
8
1
0.100 (2.54)
0.070 (1.78)
0.060 (1.52)
0.045 (1.14)
BSC
5
4
0.280 (7.11)
0.250 (6.35)
0.240 (6.10)
0.015
(0.38)
MIN
SEATING
PLANE
0.005 (0.13)
MIN
0.060 (1.52)
MAX
0.015 (0.38)
GAUGE
PLANE
0.325 (8.26)
0.310 (7.87)
0.300 (7.62)
0.430 (10.92)
MAX
0.195 (4.95)
0.130 (3.30)
0.115 (2.92)
0.014 (0.36)
0.010 (0.25)
0.008 (0.20)
CONTROLL ING DIMENS IONS ARE IN INCHES; MILLIMETER DI MENSIONS
(IN PARENTHESES) ARE ROUNDED-OF F INCH EQUI VALENTS FOR
REFERENCE ONLY AND ARE NOT APPROPRI ATE FOR USE IN DESIGN.
CORNER LEADS MAY BE CONFIGURED AS WHOL E OR HALF LEADS.
CONTROLLING DIMENSIONS ARE IN INCHES; MILLIMETER DIMENSIONS
(IN PARENTHESES) ARE ROUNDED-OFF INCH EQUIVALENTS FOR
REFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE IN DESIGN.
CONTROLL ING DIMENS IONS ARE IN MILLIM ETERS; INCH DI MENSIONS
(IN PARENTHESES) ARE ROUNDED-O FF MIL LIMETE R EQUIVALENTS FOR
REFERENCE ONLY AND ARE NOT APPROPRI ATE FOR USE IN DESIGN.
COMPLIANT TO JEDEC STANDARDS MS-013- AA
0
.
0
2
9
5
0
0
9
8
0
.
1.27 (0.0500)
0.40 (0.0157)
)
45°
)
032707-B
Figure 49. 16-Lead Standard Small Outline Package [SOIC_W]
Wide Body
(RW-16)
Dimensions shown in millimeters and (inches)
ORDERING GUIDE
Model Temperature Range Package Description Package Option
AD844AN −40°C to +85°C 8-Lead Plastic Dual In-Line Package [PDIP] N-8
AD844ANZ
AD844ACHIPS −40°C to +85°C Die
AD844AQ −40°C to +85°C 8-Lead Ceramic Dual In-Line Package [CERDIP] Q-8
AD844BQ −40°C to +85°C 8-Lead Ceramic Dual In-Line Package [CERDIP] Q-8
AD844JR-16 0°C to 70°C 16-Lead Standard Small Outline Package [SOIC_W] RW-16
AD844JR-16-REEL 0°C to 70°C 16-Lead SOIC_W, 13” Tape and Reel RW-16
AD844JR-16-REEL7 0°C to 70°C 16-Lead SOIC_W, 7” Tape and Reel RW-16
AD844JRZ-16
AD844JRZ-16-REEL
AD844JRZ-16-REEL7
AD844SCHIPS −55°C to +125°C Die
AD844SQ −55°C to +125°C 8-Lead Ceramic Dual In-Line Package [CERDIP] Q-8
AD844SQ/883B −55°C to +125°C 8-Lead Ceramic Dual In-Line Package [CERDIP] Q-8
5962-8964401PA
1
Z = RoHS Compliant Part.
2
Refer to the DESC drawing for tested specifications.
1
−40°C to +85°C 8-Lead Plastic Dual In-Line Package [PDIP] N-8
1
0°C to 70°C 16-Lead Standard Small Outline Package [SOIC_W] RW-16
1
0°C to 70°C 16-Lead SOIC_W, 13” Tape and Reel RW-16
1
0°C to 70°C 16-Lead SOIC_W, 7” Tape and Reel RW-16
2
−55°C to +125°C 8-Lead Ceramic Dual In-Line Package [CERDIP] Q-8