50 mA Output Current
Output Swing to 1 V of Rails (150 ⍀ Load)
APPLICATIONS
Video Line Driver
Professional Cameras
Video Switchers
Special Effects
PRODUCT DESCRIPTION
The AD812 is a low power, single supply, dual video amplifier.
Each of the amplifiers have 50 mA of output current and are
optimized for driving one back-terminated video load (150 Ω)
each. Each amplifier is a current feedback amplifier and features gain flatness of 0.1 dB to 40 MHz while offering differen-
tial gain and phase error of 0.02% and 0.02°. This makes the
AD812 ideal for professional video electronics such as cameras
and video switchers.
= 150 ⍀):
L
Low Power Op Amp
AD812
PIN CONFIGURATION
8-Lead Plastic
Mini-DIP and SOIC
The AD812 offers low power of 4.0 mA per amplifier max (VS =
+5 V) and can run on a single +3 V power supply. The outputs
of each amplifier swing to within one volt of either supply rail to
easily accommodate video signals of 1 V p-p. Also, at gains of
+2 the AD812 can swing 3 V p-p on a single +5 V power supply. All this is offered in a small 8-lead plastic DIP or 8-lead
SOIC package. These features make this dual amplifier ideal
for portable and battery powered applications where size and
power is critical.
The outstanding bandwidth of 145 MHz along with 1600 V/µs
of slew rate make the AD812 useful in many general purpose
high speed applications where a single +5 V or dual power sup-
plies up to ±15 V are available. The AD812 is available in the
industrial temperature range of –40°C to +85°C.
0.4
VS = 615V
65V
5V
3V
G = +2
R
= 150V
L
0.3
0.2
0.1
0
–0.1
–0.2
–0.3
NORMALIZED GAIN – dB
–0.4
–0.5
–0.6
100k
1M100M10M
FREQUENCY – Hz
Figure 1. Fine-Scale Gain Flatness vs. Frequency, Gain
= 150
= +2, R
L
Ω
DIFFERENTIAL GAIN
0.08
0.06
0.04
0.02
DIFFERENTIAL PHASE – Degrees
0
6
5
DIFFERENTIAL PHASE
SUPPLY VOLTAGE – 6Volts
Figure 2. Differential Gain and Phase vs. Supply Voltage,
= 150
Gain = +2, R
L
Ω
0.06
0.04
0.02
DIFFERENTIAL GAIN – %
15
1412111013987
REV. B
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
which may result from its use. No license is granted by implication or
otherwise under any patent or patent rights of Analog Devices.
Storage Temperature Range N, R . . . . . . . . . –65°C to +125°C
Operating Temperature Range . . . . . . . . . . . . –40°C to +85°C
Lead Temperature Range (Soldering, 10 sec) . . . . . . . +300°C
NOTES
1
Stresses above those listed under Absolute Maximum Ratings may cause perma-
nent 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.
2
Specification is for device in free air: 8-lead plastic package: θJA = 90°C/Watt;
8-lead SOIC package: θJA = 150°C/Watt.
ORDERING GUIDE
TemperaturePackagePackage
ModelRangeDescriptionOption
AD812AN–40°C to +85°C8-Lead Plastic DIPN-8
AD812AR–40°C to +85°C8-Lead Plastic SOIC SO-8
AD812AR-REEL13" Reel
AD812AR-REEL77" Reel
MAXIMUM POWER DISSIPATION
The maximum power that can be safely dissipated by the
AD812 is limited by the associated rise in junction temperature.
The maximum safe junction temperature for the plastic encapsulated parts is determined by the glass transition temperature
of the plastic, about 150°C. Exceeding this limit temporarily
may cause a shift in parametric performance due to a change in
the stresses exerted on the die by the package. Exceeding a
junction temperature of 175°C for an extended period can result
in device failure.
While the AD812 is internally short circuit protected, this may
not be sufficient to guarantee that the maximum junction temperature (150 degrees) is not exceeded under all conditions. To
ensure proper operation, it is important to observe the derating
curves.
It must also be noted that in high (noninverting) gain configurations (with low values of gain resistor), a high level of input
overdrive can result in a large input error current, which may
result in a significant power dissipation in the input stage. This
power must be included when computing the junction temperature rise due to total internal power.
2.0
8-LEAD MINI-DIP PACKAGE
1.5
TJ = +1508C
METALIZATION PHOTO
Dimensions shown in inches and (mm).
0.0783
V+
8
OUT2
7
(1.99)
–IN2
6
5 +IN2
1.0
8-LEAD SOIC PACKAGE
0.5
MAXIMUM POWER DISSIPATION – Watts
0
–5090–40 –30 –20 –10 0 10 20 3050 60 70 8040
AMBIENT TEMPERATURE – 8C
Figure 3. Plot of Maximum Power Dissipation vs.
Temperature
0.0539
(1.37)
4 V–
1
OUT1
2
–IN13+IN1
4
V–
CAUTION
ESD (electrostatic discharge) sensitive device. Electrostatic charges as high as 4000 V readily
accumulate on the human body and test equipment and can discharge without detection.
Although the AD812 features proprietary ESD protection circuitry, permanent damage may
occur on devices subjected to high energy electrostatic discharges. Therefore, proper ESD
precautions are recommended to avoid performance degradation or loss of functionality.
REV. B
–5–
Page 6
AD812–Typical Performance Characteristics
20
15
10
5
COMMON-MODE VOLTAGE RANGE – 6Volts
0
020
5
SUPPLY VOLTAGE – 6Volts
1015
Figure 4. Input Common-Mode Voltage Range vs. Supply
Voltage
20
NO LOAD
15
16
14
VS = 615V
12
10
8
TOTAL SUPPLY CURRENT – mA
6
4
JUNCTION TEMPERATURE – 8C
VS = 65V
140–40–60120806040100200–20
Figure 7. Total Supply Current vs. Junction Temperature
10
TA = +25 C
9
8
10
RL = 150V
OUTPUT VOLTAGE – V p-p
5
0
020
5
SUPPLY VOLTAGE – 6Volts
1015
Figure 5. Output Voltage Swing vs. Supply Voltage
30
615V SUPPLY
25
20
15
10
OUTPUT VOLTAGE – Volts p-p
5
0
1010010k1k
LOAD RESISTANCE – V
65V SUPPLY
Figure 6. Output Voltage Swing vs. Load Resistance
7
6
TOTAL SUPPLY CURRENT – mA
5
20
Figure 8. Total Supply Current vs. Supply Voltage
25
20
15
10
5
0
–5
–10
INPUT BIAS CURRENT – mA
–15
–20
–25
–60
Figure 9. Input Bias Current vs. Junction Temperature
SUPPLY VOLTAGE – 6Volts
JUNCTION TEMPERATURE – 8C
864
–IB, VS = 65V
+IB, VS = 65V, 615V
–IB, VS = 615V
16
141210
140–40120100806040200–20
–6–
REV. B
Page 7
AD812
4
2
0
–2
–4
–6
–8
–10
–12
INPUT OFFSET VOLTAGE – mV
–14
–16
JUNCTION TEMPERATURE – 8C
VS = 65V
VS = 615V
140–40–60120100806040200–20
Figure 10. Input Offset Voltage vs. Junction Temperature
160
140
120
100
80
SHORT CIRCUIT CURRENT – mA
60
40
SINK
SOURCE
JUNCTION TEMPERATURE – 8C
VS = 615V
140–40–60120806040100200–20
Figure 11. Short Circuit Current vs. Junction Temperature
70
60
50
40
OUTPUT CURRENT – mA
30
20
50
SUPPLY VOLTAGE – 6Volts
1510
20
Figure 13. Linear Output Current vs. Supply Voltage
1k
100
10
1
0.1
CLOSED-LOOP OUTPUT RESISTANCE – V
0.01
G = +2
65V
100k100M10M1M10k
S
615V
S
FREQUENCY – Hz
Figure 14. Closed-Loop Output Resistance vs. Frequency
80
70
60
50
VS = 65V
40
OUTPUT CURRENT – mA
30
20
JUNCTION TEMPERATURE – 8C
VS = 615V
140–40–60120806040100200–20
Figure 12. Linear Output Current vs. Junction Temperature
REV. B
–7–
30
VS = 615V
25
20
RL = 1kV
15
10
VS = 65V
OUTPUT VOLTAGE – V p-p
5
0
100k1M100M10M
FREQUENCY – Hz
Figure 15. Large Signal Frequency Response
Page 8
AD812
100
INVERTING INPUT
CURRENT NOISE
10
VOLTAGE NOISE – nV/ Hz
1
10
100100k10k1k
VOLTAGE NOISE
NONINVERTING INPUT
FREQUENCY – Hz
CURRENT NOISE
100
10
CURRENT NOISE – pA/ Hz
1
Figure 16. Input Current and Voltage Noise vs. Frequency
90
80
70
60
50
40
30
COMMON-MODE REJECTION – dB
20
10
10k
100k100M10M1M
FREQUENCY – Hz
V
IN
VS = 3V
681V
681V
681V
681V
VS = 615V
V
OUT
Figure 17. Common-Mode Rejection vs. Frequency
0
120
100
80
TRANSIMPEDANCE – dB
60
40
10k100k100M10M1M
GAIN
PHASE
VS = 3V
FREQUENCY – Hz
VS = 615V
VS = 3V
VS = 615V
–45
–90
–135
–180
Figure 19. Open-Loop Transimpedance vs. Frequency
Ω
(Relative to 1
–30
–50
–70
–90
HARMONIC DISTORTION – dBc
–110
–130
1k
)
G = +2
= 2V p-p
V
S
= 615V ; RL = 1kV
V
S
= 65V ; RL = 150V
V
S
VS = 65V
ND
2
HARMONIC
RD
3
HARMONIC
ND
2
RD
3
10k100k1M10M100M
FREQUENCY – Hz
VS = 615V
Figure 20. Harmonic Distortion vs. Frequency
PHASE – Degrees
80
70
60
50
40
30
20
POWER SUPPLY REJECTION – dB
10
0
10k
615V
61.5V
100k100M10M1M
FREQUENCY – Hz
Figure 18. Power Supply Rejection vs. Frequency
10
8
6
4
2
0
–2
–4
–6
OUTPUT SWING FROM 6V TO 0
–8
–10
20
1%
0.1%
SETTLING TIME – ns
0.025%
403050
Figure 21. Output Swing and Error vs. Settling Time
–8–
GAIN = –1
V
= 615V
S
60
REV. B
Page 9
1400
0
15.0
600
200
1.5
400
0
1200
800
1000
13.512.010.59.07.56.04.53.0
SUPPLY VOLTAGE – 6Volts
SLEW RATE – V/ms
G = +2
G = +10
G = –1
G = +1
SLEW RATE – V/ms
1400
1200
1000
800
600
400
200
VS = 615V
= 500V
R
L
AD812
G = +1
G = +2
G = +10
G = –1
0
1
0
OUTPUT STEP SIZE – Vp-p
10
98765432
Figure 22. Slew Rate vs. Output Step Size
2V
100
90
10
0%
2V
50ns
V
IN
V
OUT
Figure 23. Large Signal Pulse Response, Gain = +1,
= 750 Ω, RL = 150 Ω, VS = ±5 V)
(R
F
G = +1
R
= 150V
L
VS = 615V
65V
0
–90
5V
3V
–180
–270
1000
1
0
–1
–2
–3
–4
CLOSED-LOOP GAIN – dB
–5
–6
1
PHASE
GAIN
VS = 615V
65V
5V
3V
10100
FREQUENCY – MHz
Figure 24. Closed-Loop Gain and Phase vs. Frequency,
G = +1
Figure 25. Maximum Slew Rate vs. Supply Voltage
500mV20ns
100
90
10
0%
500mV
Figure 26. Small Signal Pulse Response, Gain = +1,
= 750 Ω, RL = 150 Ω, VS = ±5 V)
(R
F
200
180
160
140
120
PHASE SHIFT – Degrees
100
80
60
–3dB BANDWIDTH – MHz
40
20
0
0
G = +1
R
= 150V
L
PEAKING 1dB
2
RF = 750V
RF = 866V
PEAKING 0.2dB
SUPPLY VOLTAGE – 6Volts
Figure 27. –3 dB Bandwidth vs. Supply Voltage, G = +1
V
IN
V
OUT
20
1816141210864
REV. B
–9–
Page 10
AD812
500mV
100
90
10
0%
5V
50ns
V
IN
V
OUT
Figure 28. Large Signal Pulse Response, Gain = +10,
= 357 Ω, RL = 500 Ω, VS = ±15 V)
(R
F
PHASE
1
GAIN
0
–1
–2
–3
–4
–5
–6
CLOSED-LOOP GAIN (NORMALIZED) – dB
1101000100
5V
3V
5V
3V
FREQUENCY – MHz
VS = 615V
VS = 615V
65V
65V
G = +10
R
= 150V
L
0
–90
–180
–270
PHASE SHIFT – Degrees
Figure 29. Closed-Loop Gain and Phase vs. Frequency,
Gain = +10, R
= 150
L
Ω
50mV
100
90
10
0%
500mV
20ns
V
IN
V
OUT
Figure 31. Small Signal Pulse Response, Gain = +10,
(R
= 357 Ω, RL = 150 Ω, VS = ±5 V)
F
PHASE
1
GAIN
0
–1
–2
–3
–4
–5
–6
CLOSED-LOOP GAIN (NORMALIZED) – dB
1101000100
3V
VS = 615V
5V
5V
3V
FREQUENCY – MHz
G = +10
R
65V
VS = 615V
65V
= 1kV
L
0
–90
–180
–270
–360
PHASE SHIFT – Degrees
Figure 32. Closed-Loop Gain and Phase vs. Frequency,
= 1 k
Gain = +10, R
Ω
L
100
G = +10
90
80
70
60
50
40
30
–3dB BANDWIDTH – MHz
20
10
0
= 150V
R
L
PEAKING 1dB
RF = 154V
216141210864
01820
SUPPLY VOLTAGE – 6Volts
RF = 357V
RF = 649V
Figure 30. –3 dB Bandwidth vs. Supply Voltage,
Gain = +10, R
= 150
L
Ω
110
G = +10
100
90
80
70
60
50
40
–3dB BANDWIDTH – MHz
30
20
10
= 1k
R
L
216141210864
01820
Figure 33. –3 dB Bandwidth vs. Supply Voltage,
Gain = +10, R
–10–
V
RF = 154
V
SUPPLY VOLTAGE – 6Volts
= 1 k
Ω
L
RF = 357
RF = 649
V
V
REV. B
Page 11
AD812
10
90
100
0%
500mV
20ns
500mV
V
IN
V
OUT
2V
100
90
10
0%
2V
50ns
V
IN
V
OUT
Figure 34. Large Signal Pulse Response, Gain = –1,
= 750 Ω, RL = 150 Ω, VS = ±5 V)
(R
F
PHASE
1
GAIN
0
–1
–2
–3
–4
–5
–6
CLOSED-LOOP GAIN (NORMALIZED) – dB
1101000100
FREQUENCY – MHz
VS = 615V
65V
5V
G = –1
= 150V
R
L
3V
VS = 615V
65V
5V
3V
0
–90
–180
–270
PHASE SHIFT – Degrees
Figure 35. Closed-Loop Gain and Phase vs. Frequency,
= 150
Gain = –1, R
L
Ω
Figure 37. Small Signal Pulse Response, Gain = –1,
= 750 Ω, RL = 150 Ω, VS = ±5 V)
(R
F
PHASE
1
GAIN
0
–1
–2
–3
–4
–5
–6
CLOSED-LOOP GAIN (NORMALIZED) – dB
1101000100
VS = 615V
VS = 615V
5V
3V
65V
5V
3V
FREQUENCY – MHz
65V
G = –10
R
= 1kV
L
0
–90
–180
–270
PHASE SHIFT – Degrees
Figure 38. Closed-Loop Gain and Phase vs. Frequency,
= 1 k
Gain = –10, R
Ω
L
130
G = –1
120
R
= 150V
L
110
100
90
80
70
60
–3dB BANDWIDTH – MHz
50
40
30
0
PEAKING # 1.0dB
2
PEAKING # 0.2dB
SUPPLY VOLTAGE – 6Volts
RF = 681V
RF = 715V
Figure 36. –3 dB Bandwidth vs. Supply Voltage,
= 150
Gain = –1, R
L
Ω
REV. B
100
G = –10
90
R
= 1kV
0
0
L
RF = 154V
2
SUPPLY VOLTAGE – 6Volts
RF = 357V
RF = 649V
20
1816141210864
80
70
60
50
40
30
–3dB BANDWIDTH – MHz
20
10
20
1816141210864
Figure 39. –3 dB Bandwidth vs. Supply Voltage,
= 1 k
Gain = –10, R
Ω
L
–11–
Page 12
AD812
General Considerations
The AD812 is a wide bandwidth, dual video amplifier which
offers a high level of performance on less than 5.5 mA per amplifier of quiescent supply current. It is designed to offer outstanding performance at closed-loop inverting or noninverting
gains of one or greater.
Built on a low cost, complementary bipolar process, and achieving bandwidth in excess of 100 MHz, differential gain and phase
errors of better than 0.1% and 0.1° (into 150 Ω), and output
current greater than 40 mA, the AD812 is an exceptionally
efficient video amplifier. Using a conventional current feedback
architecture, its high performance is achieved through careful
attention to design details.
Choice of Feedback and Gain Resistors
Because it is a current feedback amplifier, the closed-loop bandwidth of the AD812 depends on the value of the feedback resistor. The bandwidth also depends on the supply voltage. In
addition, attenuation of the open-loop response when driving
load resistors less than about 250 Ω will affect the bandwidth.
Table I contains data showing typical bandwidths at different
supply voltages for some useful closed-loop gains when driving a
load of 150 Ω. (Bandwidths will be about 20% greater for load
resistances above a few hundred ohms.)
The choice of feedback resistor is not critical unless it is important to maintain the widest, flattest frequency response. The
resistors recommended in the table are those (metal film values)
that will result in the widest 0.1 dB bandwidth. In those applications where the best control of the bandwidth is desired, 1%
metal film resistors are adequate. Wider bandwidths can be
attained by reducing the magnitude of the feedback resistor (at
the expense of increased peaking), while peaking can be reduced
by increasing the magnitude of the feedback resistor.
Table I. –3 dB Bandwidth vs. Closed-Loop Gain and
Feedback Resistor (R
VS (V)GainRF (⍀)BW (MHz)
±15+1866145
±5+175090
+5+175060
+3+175050
= 150 Ω)
L
+2715100
+1035765
–1715100
–1035760
+268165
+1015445
–171570
–1015445
+268150
+1015435
–171550
–1015435
+268140
+1015430
–171540
–1015425
To estimate the –3 dB bandwidth for closed-loop gains or feedback resistors not listed in the above table, the following two
pole model for the AD812 many be used:
A
=
CL
RGrC
+
FINT
()
2
S
2
π
f
2
G
S RGrC
++
FINT
()
1
+
where:ACL= closed-loop gain
G= 1 + R
F/RG
rIN= input resistance of the inverting input
C
= “transcapacitance,” which forms the open-loop
T
dominant pole with the tranresistance
= feedback resistor
R
F
R
= gain resistor
G
= frequency of second (nondominant) pole
f
2
S= 2
πj
f
Appropriate values for the model parameters at different supply
voltages are listed in Table II. Reasonable approximations for
these values at supply voltages not found in the table can be
obtained by a simple linear interpolation between those tabulated values which “bracket” the desired condition.
Table II. Two-Pole Model Parameters at Various
Supply Voltages
V
S
±15852.5150
±5903.8125
+51054.8105
+31155.595
rIN (⍀)C
(pF)f2 (MHz)
T
As discussed in many amplifier and electronics textbooks (such
as Roberge’s Operational Amplifiers: Theory and Practice), the
–3 dB bandwidth for the 2-pole model can be obtained as:
f
= fN [1 – 2d2 + (2 – 4d2 + 4d4)
3
1/2]1/2
where:
f
=
N
f
2
RGrC
+
()
FINT
12/
and:
d = (1/2) [f
(RF + GrIN) CT]
2
1/2
This model will predict –3 dB bandwidth within about 10 to
15% of the correct value when the load is 150 Ω. However, it is
not an accurate enough to predict either the phase behavior or
the frequency response peaking of the AD812.
Printed Circuit Board Layout Guidelines
As with all wideband amplifiers, printed circuit board parasitics
can affect the overall closed-loop performance. Most important
for controlling the 0.1 dB bandwidth are stray capacitances at
the output and inverting input nodes. Increasing the space between
signal lines and ground plane will minimize the coupling. Also,
signal lines connecting the feedback and gain resistors should be
kept short enough that their associated inductance does not
cause high frequency gain errors.
–12–
REV. B
Page 13
AD812
AD812
8
4
R
G
R
F
V
IN
R
T
V
O
R
L
C
L
R
S
+V
S
0.1mF
1.0mF
0.1mF
1.0mF
–V
S
Power Supply Bypassing
Adequate power supply bypassing can be very important when
optimizing the performance of high speed circuits. Inductance
in the supply leads can (for example) contribute to resonant
circuits that produce peaking in the amplifier’s response. In
addition, if large current transients must be delivered to a load,
then large (greater than 1 µF) bypass capacitors are required to
produce the best settling time and lowest distortion. Although
0.1 µF capacitors may be adequate in some applications, more
elaborate bypassing is required in other cases.
When multiple bypass capacitors are connected in parallel, it is
important to be sure that the capacitors themselves do not form
resonant circuits. A small (say 5 Ω) resistor may be required in
series with one of the capacitors to minimize this possibility.
As discussed below, power supply bypassing can have a significant impact on crosstalk performance.
Achieving Low Crosstalk
Measured crosstalk from the output of amplifier 2 to the input
of amplifier 1 of the AD812 is shown in Figure 40. The crosstalk
from the output of amplifier 1 to the input of amplifier 2 is a few
dB better than this due to the additional distance between critical signal nodes.
A carefully laid-out PC board should be able to achieve the level
of crosstalk shown in the figure. The most significant contributors to difficulty in achieving low crosstalk are inadequate power
supply bypassing, overlapped input and/or output signal paths,
and capacitive coupling between critical nodes.
The bypass capacitors must be connected to the ground plane at
a point close to and between the ground reference points for the
two loads. (The bypass of the negative power supply is particularly important in this regard.) There are two amplifiers in the
package, and low impedance signal return paths must be pro-
vided for each load. (Using a parallel combination of 1 µF,
0.1 µF, and 0.01 µF bypass capacitors will help to achieve opti-
mal crosstalk.)
The input and output signal return paths must also be kept from
overlapping. Since ground connections are not of perfectly zero
impedance, current in one ground return path can produce a
voltage drop in another ground return path if they are allowed
to overlap.
Electric field coupling external to (and across) the package can
be reduced by arranging for a narrow strip of ground plane to be
run between the pins (parallel to the pin rows). Doing this on
both sides of the board can reduce the high frequency crosstalk
by about 5 dB or 6 dB.
Driving Capacitive Loads
When used with the appropriate output series resistor, any load
capacitance can be driven without peaking or oscillation. In
most cases, less than 50 Ω is all that is needed to achieve an
extremely flat frequency response. As illustrated in Figure 44,
the AD812 can be very attractive for driving largely capacitive
loads. In this case, the AD812’s high output short circuit
current allows for a 150 V/µs slew rate when driving a 510 pF
capacitor.
Figure 41. Circuit for Driving a Capacitive Load
–10
–20
–30
–40
–50
–60
–70
CROSSTALK – dB
–80
–90
–100
–110
100k
1M100M10M
FREQUENCY – Hz
Figure 40. Crosstalk vs. Frequency
REV. B
RL = 150V
12
–3
CLOSED-LOOP GAIN – dB
–6
Figure 42. Response to a Small Load Capacitor at ±5 V
–13–
V
= 65V
S
G = +2
R
= 750V
F
= 1kV
R
L
CL = 10pF
9
6
3
0
1
RS = 50V
101000100
FREQUENCY – MHz
RS = 0
RS = 30V
Page 14
AD812
V
= 615V
S
G = +2
= 750V
R
F
= 1kV
R
12
9
6
3
0
–3
CL = 510pF, RS = 15V
–6
CLOSED-LOOP GAIN – dB
–9
1
101000100
FREQUENCY – MHz
CL = 150pF, RS = 30V
Figure 43. Response to Large Load Capacitor, VS = ±15 V
L
1V
100
90
10
0%
2V
50ns
V
IN
V
OUT
Figure 45. 6 dB Overload Recovery; G = 10, RL = 500 Ω,
= ±5 V
V
S
5V
100
90
10
0%
5V
100ns
V
IN
V
OUT
Figure 44. Pulse Response of Circuit of Figure 41 with
= 510 pF, RL = 1 kΩ, RF = RG = 715 Ω, RS = 15
C
L
Ω
Overload Recovery
There are three important overload conditions to consider.
They are due to input common mode voltage overdrive, input
current overdrive, and output voltage overdrive. When the
amplifier is configured for low closed-loop gains, and its input
common-mode voltage range is exceeded, the recovery time will
be very fast, typically under 10 ns. When configured for a higher
gain, and overloaded at the output, the recovery time will also
be short. For example, in a gain of +10, with 6 dB of input
overdrive, the recovery time of the AD812 is about 10 ns.
In the case of high gains with very high levels of input overdrive,
a longer recovery time may occur. For example, if the input
common-mode voltage range is exceeded in a gain of +10, the
recovery time will be on the order of 100 ns. This is primarily
due to current overloading of the input stage.
As noted in the warning under “Maximum Power Dissipation,”
a high level of input overdrive in a high noninverting gain circuit
can result in a large current flow in the input stage. For differential input voltages of less than about 1.25 V, this will be internally limited to less than 20 mA (decreasing with supply voltage).
For input overdrives which result in higher differential input
voltages, power dissipation in the input stage must be considered. It is recommended that external diode clamps be used in
cases where the differential input voltage is expected to exceed
1.25 V.
High Performance Video Line Driver
At a gain of +2, the AD812 makes an excellent driver for a back-
terminated 75 Ω video line. Low differential gain and phase
errors and wide 0.1 dB bandwidth can be realized over a wide
range of power supply voltage. Outstanding gain and group
delay matching are also attainable over the full operating supply
voltage range.
R
G
75V
CABLE
V
IN
75V
+V
S
8
AD812
4
R
F
0.1mF
0.1mF
75V
75V
CABLE
75V
V
OUT
–V
S
Figure 46. Gain of +2 Video Line Driver (RF = RG from
Table I)
–14–
REV. B
Page 15
AD812
–0.1
–0.6
1M100M10M
–0.2
–0.3
–0.4
–0.5
0
0.1
NORMALIZED GAIN – dB
100k
FREQUENCY – Hz
0.2
0.3
0.4
G = +2
R
L
= 150V
5V
3V
VS = 615V
65V
1.0
0
–1.0
10100
–0.2
–0.4
–0.6
–0.8
0.2
0.4
0.6
0.8
GAIN MATCH – dB
1
FREQUENCY – MHz
1000
VS = 3V
R
F
= 681V
G = +2
R
L
= 150V
VS = 615V
R
F
= 715V
PHASE
3V
1
GAIN
0
–1
–2
–3
–4
–5
CLOSED-LOOP GAIN – dB
–6
1101000100
5V
5V
3V
FREQUENCY –MHz
G = +2
R
= 150
L
VS = 615V
65V
VS = 615V
6
5V
90
0
V
–90
–180
–270
PHASE SHIFT – Degrees
Figure 47. Closed-Loop Gain and Phase vs. Frequency for
the Line Driver
120
G = +2
110
R
= 150V
L
100
PEAKING # 1dB
90
80
70
60
50
–3dB BANDWIDTH – MHz
40
30
20
2
0
NO PEAKING
SUPPLY VOLTAGE – 6Volts
RF = 590V
= 715V
R
F
= 750V
R
F
1816141210864
20
Figure 48. –3 dB Bandwidth vs. Supply Voltage,
= 150
Gain = +2, R
L
Ω
Figure 50. Fine-Scale Gain Flatness vs. Frequency,
= 150
Gain = +2, R
L
Ω
Figure 51. Closed-Loop Gain Matching vs. Frequency,
Gain = +2, R
= 150
L
Ω
Figure 49. Differential Gain and Phase vs. Supply Voltage,
Gain = +2, R
REV. B
DIFFERENTIAL GAIN
0.08
0.06
DIFFERENTIAL PHASE
0.04
0.02
DIFFERENTIAL PHASE – Degrees
0
6
5
= 150
L
SUPPLY VOLTAGE – 6Volts
Ω
0.06
0.04
0.02
DIFFERENTIAL GAIN – %
15
1412111013987
8
6
4
2
0
0.4
0.2
GROUP DELAY – ns
0
–0.2
–0.4
100k
DELAY
DELAY MATCHING
VS = 3V TO 615V
1M10M
FREQUENCY – Hz
3V
5V
65V
615V
100M
Figure 52. Group Delay and Group Delay Matching vs.
Frequency, G = +2, R
= 150
L
Ω
–15–
Page 16
AD812
Operation Using a Single Supply
The AD812 will operate with total supply voltages from 36 V
down to 2.4 V. With proper biasing (see Figure 53), it can be an
outstanding single supply video amplifier. Since the input and
output voltage ranges extend to within 1 volt of the supply rails,
it will handle a 1.3 V p-p signal on a single 3.3 V supply, or a
3 V p-p signal on a single 5 V supply. The small signal, 0.1 dB
bandwidths will exceed 10 MHz in either case, and the large
signal bandwidths will exceed 6 MHz.
The capacitively coupled cable driver in Figure 53 will achieve
outstanding differential gain and phase errors of 0.07% and 0.06
degrees respectively on a single 5 V supply. Resistor R2, in this
circuit, is selected to optimize the differential gain and phase by
operating the amplifier in its most linear region. To optimize the
circuit for a 3 V supply, a value of 8 kΩ is recommended for R2.
V
C2
1mF
IN
C3
30mF
2mF
11.8kV
649V
R1
9kV
C1
R2
R3
1kV
AD812
649V
8
4
+V
S
C
OUT
47mF
75V
75V
CABLE
75V
V
OUT
PHASE
0.5
GAIN
0
–0.5
–1.0
–1.5
–2.0
–2.5
CLOSED-LOOP GAIN – dB
–3.0
–3.5
1101000100
FREQUENCY – MHz
VS = 5V
90
0
–90
–180
–270
Figure 54. Closed-Loop Gain and Phase vs. Frequency,
Circuit of Figure 53
100
1V
90
50ns
V
IN
PHASE SHIFT – Degrees
C1859b–0–9/98
Figure 53. Biasing for Single Supply Operation
Dimensions shown in inches and (mm).
8-Lead Plastic DIP
(N-8)
0.39 (9.91)
0.165 60.01
(4.19 60.25)
0.125 (3.18)
MIN
0.018 60.003
(0.46 +0.08)
8
14
PIN 1
0.10
(2.54)
BSC
5
0.25
(6.35)
0.060 (1.52)
0.015 (0.38)
0.033 (0.84)
NOM
SEATING
PLANE
0.325 (8.25)
0.300 (7.62)
0.195 (4.95)
0.115 (2.93)
0.015 (0.381)
0.008 (0.204)
10
0%
Figure 55. Pulse Response of the Circuit of Figure 53 with
= 5 V
V
S
OUTLINE DIMENSIONS
0.1574 (4.00)
0.1497 (3.80)
0.0098 (0.25)
0.0040 (0.10)
SEATING
PLANE
500mV
0.1968 (5.00)
0.1890 (4.80)
85
PIN 1
0.0500
(1.27)
BSC
8-Lead Plastic SOIC
(SO-8)
0.2440 (6.20)
41
0.2284 (5.80)
0.0688 (1.75)
0.0532 (1.35)
0.0192 (0.49)
0.0138 (0.35)
0.0098 (0.25)
0.0075 (0.19)
88
08
0.0196 (0.50)
0.0099 (0.25)
0.0500 (1.27)
0.0160 (0.41)
3 458
V
OUT
PRINTED IN U.S.A.
–16–
REV. B
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