AD811ACHIPS [ADI]

High Performance Video Op Amp; 高性能视频运算放大器
AD811ACHIPS
型号: AD811ACHIPS
厂家: ADI    ADI
描述:

High Performance Video Op Amp
高性能视频运算放大器

运算放大器
文件: 总15页 (文件大小:233K)
中文:  中文翻译
下载:  下载PDF数据表文档文件
High Performance  
Video Op Amp  
a
AD811  
CONNECTION DIAGRAMS  
FEATURES  
High Speed  
20-Lead LCC (E-20A) Package  
8-Lead Plastic (N-8)  
Cerdip (Q-8)  
SOIC (SO-8) Packages  
140 MHz Bandwidth (3 dB, G = +1)  
120 MHz Bandwidth (3 dB, G = +2)  
35 MHz Bandwidth (0.1 dB, G = +2)  
2500 V/s Slew Rate  
25 ns Settling Time to 0.1% (For a 2 V Step)  
65 ns Settling Time to 0.01% (For a 10 V Step)  
Excellent Video Performance (RL =150 )  
0.01% Differential Gain, 0.01؇ Differential Phase  
Voltage Noise of 1.9 nVHz  
20  
1
2
19  
3
NC 4  
18 NC  
17  
NC  
–IN  
+IN  
NC  
+V  
1
2
3
4
8
7
6
5
5
6
7
NC  
–IN  
NC  
NC  
16 +V  
AD811  
S
S
15 NC  
OUTPUT  
NC  
+IN 8  
14 OUTPUT  
–V  
S
AD811  
9
10 1112 13  
NC = NO CONNECT  
NC = NO CONNECT  
Low Distortion: THD = –74 dB @ 10 MHz  
Excellent DC Precision  
3 mV max Input Offset Voltage  
Flexible Operation  
Specified for ؎5 V and ؎15 V Operation  
؎2.3 V Output Swing into a 75 Load (VS = ؎5 V)  
16-Lead SOIC (R-16) Package 20-Lead SOIC (R-20) Package  
NC  
NC  
NC  
–IN  
NC  
+IN  
NC  
1
2
3
4
5
6
7
8
20  
19  
18  
NC  
NC  
NC  
+V  
1
2
3
4
16 NC  
15 NC  
NC  
NC  
+V  
14  
–IN  
NC  
S
APPLICATIONS  
Video Crosspoint Switchers, Multimedia Broadcast  
Systems  
HDTV Compatible Systems  
Video Line Drivers, Distribution Amplifiers  
ADC/DAC Buffers  
DC Restoration Circuits  
Medical—Ultrasound, PET, Gamma and Counter  
Applications  
17  
16  
13 NC  
12  
S
NC  
+IN  
NC  
5
6
7
8
OUTPUT  
15 OUTPUT  
14 NC  
11 NC  
10  
9
–V  
S
NC  
NC  
AD811  
–V  
S
NC  
NC  
13  
12  
11  
NC  
NC  
NC  
9
NC = NO CONNECT  
AD811  
10  
NC  
NC = NO CONNECT  
PRODUCT DESCRIPTION  
The AD811 is also excellent for pulsed applications where tran-  
sient response is critical. It can achieve a maximum slew rate of  
greater than 2500 V/µs with a settling time of less than 25 ns to  
0.1% on a 2 volt step and 65 ns to 0.01% on a 10 volt step.  
The AD811 is a wideband current-feedback operational ampli-  
fier, optimized for broadcast quality video systems. The –3 dB  
bandwidth of 120 MHz at a gain of +2 and differential gain and  
phase of 0.01% and 0.01° (RL = 150 ) make the AD811 an  
excellent choice for all video systems. The AD811 is designed to  
meet a stringent 0.1 dB gain flatness specification to a band-  
width of 35 MHz (G = +2) in addition to the low differential  
gain and phase errors. This performance is achieved whether  
driving one or two back terminated 75 cables, with a low  
power supply current of 16.5 mA. Furthermore, the AD811 is  
specified over a power supply range of ±4.5 V to ±18 V.  
The AD811 is ideal as an ADC or DAC buffer in data acquisi-  
tion systems due to its low distortion up to 10 MHz and its wide  
unity gain bandwidth. Because the AD811 is a current feedback  
amplifier, this bandwidth can be maintained over a wide range  
of gains. The AD811 also offers low voltage and current noise of  
1.9 nV/Hz and 20 pA/Hz, respectively, and excellent dc accu-  
racy for wide dynamic range applications.  
12  
0.20  
0.10  
G = +2  
0.18  
0.09  
RF = 649⍀  
RL = 150⍀  
9
6
3
VS = ؎15V  
FC = 3.58MHz  
100 IRE  
RG = RFB  
0.16  
0.14  
0.12  
0.10  
0.08  
0.06  
0.04  
0.02  
0.08  
0.07  
MODULATED RAMP  
RL = 150⍀  
0.06  
0.05  
0.04  
0.03  
0.02  
0.01  
VS = ؎5V  
PHASE  
0
–3  
–6  
GAIN  
6
1M  
10M  
FREQUENCY – Hz  
100M  
5
7
8
9
10 11 12 13 14 15  
SUPPLY VOLTAGE – Volts  
؎
REV. D  
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.  
One Technology Way, P.O. Box 9106, Norwood, MA 02062-9106, U.S.A.  
Tel: 781/329-4700  
Fax: 781/326-8703  
World Wide Web Site: http://www.analog.com  
© Analog Devices, Inc., 1999  
(@ TA = +25؇C and VS = ؎15 V dc, RLOAD = 150 unless otherwise noted)  
AD811–SPECIFICATIONS  
AD811J/A1  
Typ  
AD811S2  
Typ  
Model  
Conditions  
VS  
Min  
Max  
Min  
Max  
Units  
DYNAMIC PERFORMANCE  
Small Signal Bandwidth (No Peaking)  
–3 dB  
G = +1  
G = +2  
G = +2  
G = +10  
0.1 dB Flat  
G = +2  
RFB = 562  
RFB = 649 Ω  
RFB = 562 Ω  
RFB = 511 Ω  
±15 V  
±15 V  
±5 V  
140  
120  
80  
140  
120  
80  
MHz  
MHz  
MHz  
MHz  
±15 V  
100  
100  
RFB = 562 Ω  
RFB = 649 Ω  
VOUT = 20 V p-p  
VOUT = 4 V p-p  
VOUT = 20 V p-p  
10 V Step, AV = –1  
±5 V  
25  
35  
40  
400  
2500  
50  
65  
25  
3.5  
0.01  
0.01  
–74  
36  
25  
35  
40  
400  
2500  
50  
65  
25  
3.5  
0.01  
0.01  
–74  
36  
MHz  
MHz  
MHz  
V/µs  
V/µs  
ns  
ns  
ns  
ns  
%
Degree  
dBc  
dBm  
dBm  
±15 V  
±15 V  
±5 V  
±15 V  
±15 V  
Full Power Bandwidth3  
Slew Rate  
Settling Time to 0.1%  
Settling Time to 0.01%  
Settling Time to 0.1%  
Rise Time, Fall Time  
Differential Gain  
2 V Step, AV = –1  
RFB = 649, AV = +2  
f = 3.58 MHz  
f = 3.58 MHz  
VOUT = 2 V p-p, AV = +2  
@ fC = 10 MHz  
±5 V  
±15 V  
±15 V  
±15 V  
±15 V  
±5 V  
Differential Phase  
THD @ fC = 10 MHz  
Third Order Intercept4  
±15 V  
43  
43  
INPUT OFFSET VOLTAGE  
Offset Voltage Drift  
±5 V, ±15 V  
0.5  
3
5
0.5  
3
5
mV  
mV  
µV/°C  
TMIN to TMAX  
5
5
INPUT BIAS CURRENT  
–Input  
±5 V, ±15 V  
±5 V, ±15 V  
2
2
5
2
2
5
µA  
µA  
µA  
µA  
TMIN to TMAX  
TMIN to TMAX  
15  
10  
20  
30  
10  
25  
+Input  
TRANSRESISTANCE  
TMIN to TMAX  
VOUT = ±10 V  
RL = ∞  
±15 V  
±15 V  
0.75  
0.5  
1.5  
0.75  
0.75  
0.5  
1.5  
0.75  
MΩ  
MΩ  
RL = 200 Ω  
VOUT = ±2.5 V  
RL = 150 Ω  
±5 V  
0.25  
0.4  
0.125 0.4  
MΩ  
COMMON-MODE REJECTION  
VOS (vs. Common Mode)  
TMIN to TMAX  
TMIN to TMAX  
Input Current (vs. Common Mode)  
VCM = ±2.5  
VCM = ±10 V  
TMIN to TMAX  
±5 V  
±15 V  
56  
60  
60  
66  
1
50  
56  
60  
66  
1
dB  
dB  
µA/V  
3
3
POWER SUPPLY REJECTION  
VOS  
+Input Current  
–Input Current  
VS = ±4.5 V to ±18 V  
TMIN to TMAX  
TMIN to TMAX  
60  
70  
0.3  
0.4  
60  
70  
0.3  
0.4  
dB  
µA/V  
µA/V  
2
2
2
2
TMIN to TMAX  
INPUT VOLTAGE NOISE  
INPUT CURRENT NOISE  
f = 1 kHz  
f = 1 kHz  
1.9  
20  
1.9  
20  
nV/Hz  
pA/Hz  
OUTPUT CHARACTERISTICS  
Voltage Swing, Useful Operating Range5  
±5 V  
±15 V  
±2.9  
±12  
100  
150  
9
±2.9  
±12  
100  
150  
9
V
V
mA  
mA  
Output Current  
Short-Circuit Current  
Output Resistance  
TJ = +25°C  
(Open Loop @ 5 MHz)  
INPUT CHARACTERISTICS  
+Input Resistance  
–Input Resistance  
1.5  
14  
1.5  
14  
MΩ  
Input Capacitance  
Common-Mode Voltage Range  
+Input  
7.5  
±3  
7.5  
±3  
pF  
V
±5 V  
±15 V  
±13  
±13  
V
POWER SUPPLY  
Operating Range  
Quiescent Current  
±4.5  
±18  
16.0  
18.0  
±4.5  
±18  
16.0  
18.0  
V
mA  
mA  
±5 V  
±15 V  
14.5  
16.5  
14.5  
16.5  
TRANSISTOR COUNT  
NOTES  
# of Transistors  
40  
40  
1The AD811JR is specified with ± 5 V power supplies only, with operation up to ±12 volts.  
2See Analog Devices’ military data sheet for 883B tested specifications.  
3FPBW = slew rate/(2 π VPEAK).  
4Output power level, tested at a closed loop gain of two.  
5Useful operating range is defined as the output voltage at which linearity begins to degrade.  
Specifications subject to change without notice.  
REV. D  
–2–  
AD811  
ABSOLUTE MAXIMUM RATINGS1  
MAXIMUM POWER DISSIPATION  
Supply Voltage . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .±18 V  
AD811JR Grade Only . . . . . . . . . . . . . . . . . . . . . . . . .±12 V  
Internal Power Dissipation2 . . . . . . . . Observe Derating Curves  
Output Short Circuit Duration . . . . . Observe Derating Curves  
Common-Mode Input Voltage . . . . . . . . . . . . . . . . . . . . . ±VS  
Differential Input Voltage . . . . . . . . . . . . . . . . . . . . . . . . .±6 V  
Storage Temperature Range (Q, E) . . . . . . . . –65°C to +150°C  
Storage Temperature Range (N, R) . . . . . . . . –65°C to +125°C  
Operating Temperature Range  
AD811J . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .0°C to +70°C  
AD811A . . . . . . . . . . . . . . . . . . . . . . . . . . . . –40°C to +85°C  
AD811S . . . . . . . . . . . . . . . . . . . . . . . . . . . –55°C to +125°C  
Lead Temperature Range (Soldering 60 sec) . . . . . . . . +300°C  
The maximum power that can be safely dissipated by the  
AD811 is limited by the associated rise in junction temperature.  
For the plastic packages, the maximum safe junction tempera-  
ture is +145°C. For the cerdip and LCC packages, the maxi-  
mum junction temperature is +175°C. If these maximums are  
exceeded momentarily, proper circuit operation will be restored  
as soon as the die temperature is reduced. Leaving the device in  
the “overheated” condition for an extended period can result in  
device burnout. To ensure proper operation, it is important to  
observe the derating curves in Figures 17 and 18.  
While the AD811 is internally short circuit protected, this may  
not be sufficient to guarantee that the maximum junction tem-  
perature is not exceeded under all conditions. One important  
example is when the amplifier is driving a reverse terminated  
75 cable and the cable’s far end is shorted to a power supply.  
With power supplies of ±12 volts (or less) at an ambient tem-  
perature of +25°C or less, if the cable is shorted to a supply rail,  
then the amplifier will not be destroyed, even if this condition  
persists for an extended period.  
NOTES  
1Stresses 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.  
28-Lead Plastic Package: θJA = 90°C/W  
8-Lead Cerdip Package: θJA = 110°C/W  
8-Lead SOIC Package: θJA = 155°C/W  
16-Lead SOIC Package: θJA = 85°C/W  
ESD SUSCEPTIBILITY  
20-Lead SOIC Package: θJA = 80°C/W  
20-Lead LCC Package: θJA = 70°C/W  
ESD (electrostatic discharge) sensitive device. Electrostatic  
charges as high as 4000 volts, which readily accumulate on the  
human body and on test equipment, can discharge without  
detection. Although the AD811 features proprietary ESD pro-  
tection circuitry, permanent damage may still occur on these  
devices if they are subjected to high energy electrostatic dis-  
charges. Therefore, proper ESD precautions are recommended  
to avoid any performance degradation or loss of functionality.  
ORDERING GUIDE  
Temperature  
Range  
Package  
Option*  
Model  
AD811AN  
AD811AR-16  
AD811AR-20  
AD811JR  
–40°C to +85°C  
–40°C to +85°C  
–40°C to +85°C  
0°C to +70°C  
N-8  
R-16  
R-20  
SO-8  
Q-8  
METALIZATION PHOTOGRAPH  
Contact Factory for Latest Dimensions.  
Dimensions Shown in Inches and (mm).  
AD811SQ/883B  
5962-9313101MPA  
AD811SE/883B  
5962-9313101M2A  
AD811JR-REEL  
AD811JR-REEL7  
AD811AR-16-REEL  
AD811AR-16-REEL7  
AD811AR-20-REEL  
AD811ACHIPS  
AD811SCHIPS  
–55°C to +125°C  
–55°C to +125°C  
–55°C to +125°C  
–55°C to +125°C  
0°C to +70°C  
Q-8  
E-20A  
E-20A  
SO-8  
SO-8  
R-16  
R-16  
R-20  
Die  
0°C to +70°C  
–40°C to +85°C  
–40°C to +85°C  
–40°C to +85°C  
–40°C to +85°C  
–55°C to +125°C  
Die  
*E = Ceramic Leadless Chip Carrier; N = Plastic DIP; Q = Cerdip; SO (R) =  
Small Outline IC (SOIC).  
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 AD811 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.  
WARNING!  
ESD SENSITIVE DEVICE  
REV. D  
–3–  
AD811–Typical Performance Characteristics  
20  
20  
15  
10  
T
= +25؇C  
A
T
= +25؇C  
A
15  
10  
NO LOAD  
R
= 150⍀  
L
5
0
5
0
0
5
10  
SUPPLY VOLTAGE – ؎Volts  
15  
20  
0
5
10  
SUPPLY VOLTAGE – ؎ Volts  
15  
20  
Figure 1. Input Common-Mode Voltage Range vs. Supply  
Figure 4. Output Voltage Swing vs. Supply  
35  
30  
21  
18  
V
= ؎15V  
S
25  
20  
15  
V
= ؎15V  
15  
S
12  
9
V
= ؎5V  
S
V
= ؎5V  
S
10  
5
6
0
3
10  
100  
1k  
10k  
–60 –40 –20  
0
20  
60  
120 140  
40  
80  
100  
LOAD RESISTANCE – ⍀  
JUNCTION TEMPERATURE – ؇C  
Figure 2. Output Voltage Swing vs. Resistive Load  
Figure 5. Quiescent Supply Current vs. Junction  
Temperature  
10  
10  
8
NONINVERTING INPUT  
؎5 TO ؎15V  
6
4
V
= ؎5V  
S
0
V
= ؎5V  
S
INVERTING  
INPUT  
2
–10  
–20  
–30  
0
–2  
–4  
–6  
V
= ؎15V  
S
V
= ؎15V  
S
–8  
–10  
–60 –40 –20  
0
20  
40  
60  
80  
100 120 140  
–60 –40 –20  
0
20  
40  
60  
80  
100 120 140  
JUNCTION TEMPERATURE – ؇C  
JUNCTION TEMPERATURE – ؇C  
Figure 3. Input Bias Current vs. Junction Temperature  
Figure 6. Input Offset Voltage vs. Junction Temperature  
–4–  
REV. D  
AD811  
2.0  
1.5  
1.0  
250  
200  
150  
V
= ؎15V  
= 200⍀  
S
R
V
L
= ؎10V  
OUT  
V
= ؎15V  
S
0.5  
0
V
= ؎5V  
V
= ؎5V  
100  
50  
S
S
R
V
= 150⍀  
L
= ؎2.5V  
OUT  
–60 –40 –20  
0
20  
40  
60  
80  
100 120 140  
–60  
–40 –20  
0
20  
40  
60  
80  
100 120 140  
JUNCTION TEMPERATURE – ؇C  
JUNCTION TEMPERATURE – ؇C  
Figure 10. Transresistance vs. Junction Temperature  
Figure 7. Short Circuit Current vs. Junction Temperature  
100  
10  
1
10  
100  
10  
1
NONINVERTING CURRENT V = ؎5 TO 15V  
S
V
= ؎5V  
S
1
INVERTING CURRENT V = ؎5 TO 15V  
S
0.1  
V
= ؎15V  
S
VOLTAGE NOISE V = ؎15V  
S
GAIN = +2  
= 649⍀  
R
FB  
VOLTAGE NOISE V = ؎5V  
S
0.01  
10k  
100k  
1M  
10M  
100M  
100  
1k  
10k  
100k  
10  
FREQUENCY – Hz  
FREQUENCY – Hz  
Figure 11. Input Noise vs. Frequency  
Figure 8. Closed-Loop Output Resistance vs. Frequency  
200  
10  
8
10  
V
= 1V p–p  
RISE TIME  
O
V = ؎15V  
160  
120  
80  
40  
0
S
8
6
4
2
60  
40  
20  
0
R = 150⍀  
L
GAIN = +2  
6
BANDWIDTH  
V
V
= ؎15V  
= 1V p–p  
= 150⍀  
S
OVERSHOOT  
O
4
R
L
GAIN = +2  
2
0
PEAKING  
800  
0
400  
400  
600  
1.0k  
1.2k  
1.4k  
1.6k  
600  
1.0k  
1.2k  
1.4k  
1.6k  
800  
VALUE OF FEEDBACK RESISTOR (R ) – ⍀  
FB  
VALUE OF FEEDBACK RESISTOR (R ) – ⍀  
FB  
Figure 12. 3 dB Bandwidth and Peaking vs. Value of RFB  
Figure 9. Rise Time and Overshoot vs. Value of  
Feedback Resistor, RFB  
REV. D  
–5–  
AD811  
110  
100  
90  
25  
20  
15  
10  
649⍀  
649⍀  
150⍀  
V
V
OUT  
IN  
V
= ؎15V  
S
150⍀  
80  
GAIN = +10  
OUTPUT LEVEL FOR 3% THD  
70  
V
= ؎15V  
S
60  
V
= ؎5V  
S
50  
V
= ؎5V  
S
5
0
40  
30  
1k  
10k  
100k  
FREQUENCY – Hz  
1M  
10M  
100k  
1M  
10M  
100M  
FREQUENCY – Hz  
Figure 13. Common-Mode Rejection vs. Frequency  
Figure 16. Large Signal Frequency Response  
80  
–50  
V
= 2V p–p  
OUT  
V
= ؎15V  
= ؎5V  
R
A
= 649⍀  
S
70  
60  
50  
40  
30  
20  
10  
5
F
R
= 100⍀  
L
= +2  
V
GAIN = +2  
–70  
–90  
؎5V SUPPLIES  
V
S
CURVES ARE FOR WORST  
CASE CONDITION WHERE  
ONE SUPPLY IS VARIED  
WHILE THE OTHER IS  
HELD CONSTANT.  
2ND HARMONIC  
3RD HARMONIC  
؎15V SUPPLIES  
–110  
–130  
2ND HARMONIC  
3RD HARMONIC  
1k  
10k  
100k  
1M  
10M  
1k  
10k  
100k  
1M  
10M  
FREQUENCY – Hz  
FREQUENCY – Hz  
Figure 14. Power Supply Rejection vs. Frequency  
Figure 17. Harmonic Distortion vs. Frequency  
2.5  
3.4  
3.2  
T
MAX = +145؇C  
J
3.0  
2.8  
2.6  
2.4  
2.2  
2.0  
1.8  
1.6  
1.4  
1.2  
1.0  
0.8  
T
MAX = +175؇C  
J
16-LEAD SOIC  
2.0  
1.5  
1.0  
0.5  
20-LEAD LCC  
20-LEAD SOIC  
8-LEAD MINI-DIP  
8-LEAD CERDIP  
8-LEAD SOIC  
0.6  
0.4  
–50 –40 –30 –20 –10  
0
10 20 30 40 50 60 70 80 90  
–60 –40 –20  
0
20  
40  
60  
80  
100 120 140  
AMBIENT TEMPERATURE – ؇C  
AMBIENT TEMPERATURE – ؇C  
Figure 15. Maximum Power Dissipation vs. Temperature  
for Plastic Packages  
Figure 18. Maximum Power Dissipation vs. Temperature  
for Hermetic Packages  
–6–  
REV. D  
Typical Characteristics, Noninverting Connection–AD811  
9
G = +1  
R
FB  
R
R
= 150⍀  
6
3
L
=
G
+V  
S
V
= ؎15V  
= 750⍀  
S
R
V
TO  
FB  
OUT  
0.1F  
TEKTRONIX  
P6201 FET  
PROBE  
R
G
0
AD811  
+
V
–3  
–6  
–9  
–12  
IN  
R
L
V
= ؎5V  
S
HP8130  
PULSE  
GENERATOR  
50⍀  
R
= 619⍀  
FB  
–V  
0.1F  
S
1M  
10M  
FREQUENCY – Hz  
100M  
Figure 22. Closed-Loop Gain vs. Frequency, Gain = +1  
Figure 19. Noninverting Amplifier Connection  
26  
1V  
G = +10  
10ns  
V
R
= ؎15V  
S
23  
20  
17  
14  
11  
8
R
= 150⍀  
L
= 511⍀  
FB  
100  
90  
V
IN  
V
R
= ؎5V  
= 442⍀  
S
FB  
10  
V
OUT  
0%  
1V  
1M  
10M  
FREQUENCY – Hz  
100M  
Figure 20. Small Signal Pulse Response, Gain = +1  
Figure 23. Closed-Loop Gain vs. Frequency, Gain = +10  
100mV  
10ns  
1V  
20ns  
100  
90  
100  
90  
V
IN  
V
IN  
10  
10  
V
OUT  
V
OUT  
0%  
0%  
1V  
10V  
Figure 21. Small Signal Pulse Response, Gain = +10  
Figure 24. Large Signal Pulse Response, Gain = +10  
REV. D  
–7–  
AD811–Typical Characteristics, Inverting Connection  
6
R
FB  
V
R
= ؎15V  
= 590⍀  
S
G = –1  
R = 150⍀  
L
+V  
3
0
FB  
S
0.1F  
V
TO  
OUT  
TEKTRONIX  
P6201 FET  
PROBE  
R
V
G
IN  
–3  
–6  
–9  
–12  
HP8130  
PULSE  
GENERATOR  
AD811  
V
R
= ؎5V  
S
R
L
= 562⍀  
FB  
0.1F  
1M  
10M  
FREQUENCY – Hz  
100M  
–V  
S
Figure 25. Inverting Amplifier Connection  
Figure 28. Closed-Loop Gain vs. Frequency, Gain = –1  
26  
G = –10  
1V  
10ns  
V
R
= ؎15V  
23  
20  
17  
14  
11  
8
S
R
= 150⍀  
L
= 511⍀  
FB  
100  
90  
V
IN  
V
R
= ؎5V  
= 442⍀  
S
FB  
10  
V
OUT  
0%  
1V  
1M  
10M  
FREQUENCY – Hz  
100M  
Figure 29. Closed-Loop Gain vs. Frequency, Gain = –10  
Figure 26. Small Signal Pulse Response, Gain = –1  
1V  
20ns  
100mV  
10ns  
100  
90  
100  
90  
V
IN  
V
IN  
10  
10  
V
OUT  
V
OUT  
0%  
0%  
10V  
1V  
Figure 30. Large Signal Pulse Response, Gain = –10  
Figure 27. Small Signal Pulse Response, Gain = –10  
–8–  
REV. D  
AD811  
Achieving the Flattest Gain Response at High Frequency  
Achieving and maintaining gain flatness of better than 0.1 dB at  
frequencies above 10 MHz requires careful consideration of  
several issues.  
APPLICATIONS  
General Design Considerations  
The AD811 is a current feedback amplifier optimized for use in  
high performance video and data acquisition applications. Since  
it uses a current feedback architecture, its closed-loop –3 dB  
bandwidth is dependent on the magnitude of the feedback resis-  
tor. The desired closed-loop gain and bandwidth are obtained  
by varying the feedback resistor (RFB) to tune the bandwidth,  
and varying the gain resistor (RG) to get the correct gain. Table I  
contains recommended resistor values for a variety of useful  
closed-loop gains and supply voltages.  
Choice of Feedback and Gain Resistors  
Because of the above-mentioned relationship between the 3 dB  
bandwidth and the feedback resistor, the fine scale gain flatness  
will, to some extent, vary with feedback resistor tolerance. It is,  
therefore, recommended that resistors with a 1% tolerance be  
used if it is desired to maintain flatness over a wide range of  
production lots. In addition, resistors of different construction  
have different associated parasitic capacitance and inductance.  
Metal-film resistors were used for the bulk of the characteriza-  
tion for this data sheet. It is possible that values other than those  
indicated will be optimal for other resistor types.  
Table I. –3 dB Bandwidth vs. Closed-Loop Gain and  
Resistance Values  
VS = ؎15 V  
Closed-Loop  
Gain  
Printed Circuit Board Layout Considerations  
–3 dB BW  
(MHz)  
As to be expected for a wideband amplifier, PC board parasitics  
can affect the overall closed loop performance. Of concern are  
stray capacitances at the output and the inverting input nodes. If  
a ground plane is to be used on the same side of the board as  
the signal traces, a space (3/16" is plenty) should be left around  
the signal lines to minimize coupling. Additionally, signal lines  
connecting the feedback and gain resistors should be short  
enough so that their associated inductance does not cause  
high frequency gain errors. Line lengths less than 1/4" are  
recommended.  
RFB  
RG  
+1  
+2  
+10  
–1  
–10  
750 Ω  
649 Ω  
511 Ω  
590 Ω  
511 Ω  
140  
120  
100  
115  
95  
649 Ω  
56.2 Ω  
590 Ω  
51.1 Ω  
VS = ؎5 V  
Closed-Loop  
Gain  
–3 dB BW  
(MHz)  
RFB  
RG  
Quality of Coaxial Cable  
+1  
+2  
+10  
–1  
619 Ω  
562 Ω  
442 Ω  
562 Ω  
442 Ω  
80  
80  
65  
75  
65  
Optimum flatness when driving a coax cable is possible only  
when the driven cable is terminated at each end with a resistor  
matching its characteristic impedance. If the coax was ideal,  
then the resulting flatness would not be affected by the length of  
the cable. While outstanding results can be achieved using inex-  
pensive cables, it should be noted that some variation in flatness  
due to varying cable lengths may be experienced.  
562 Ω  
48.7 Ω  
562 Ω  
44.2 Ω  
–10  
VS = ؎10 V  
Closed-Loop  
Gain  
–3 dB BW  
(MHz)  
RFB  
RG  
Power Supply Bypassing  
Adequate power supply bypassing can be critical when optimiz-  
ing the performance of a high frequency circuit. Inductance in  
the power supply leads can form resonant circuits that produce  
peaking in the amplifier’s response. In addition, if large current  
transients must be delivered to the load, then bypass capacitors  
(typically greater than 1 µF) will be required to provide the best  
settling time and lowest distortion. Although the recommended  
0.1 µF power supply bypass capacitors will be sufficient in many  
applications, more elaborate bypassing (such as using two paral-  
leled capacitors) may be required in some cases.  
+1  
+2  
+10  
–1  
–10  
649 Ω  
590 Ω  
499 Ω  
590 Ω  
499 Ω  
105  
105  
80  
105  
80  
590 Ω  
49.9 Ω  
590 Ω  
49.9 Ω  
Figures 11 and 12 illustrate the relationship between the feed-  
back resistor and the frequency and time domain response char-  
acteristics for a closed-loop gain of +2. (The response at other  
gains will be similar.)  
The 3 dB bandwidth is somewhat dependent on the power supply  
voltage. As the supply voltage is decreased for example, the  
magnitude of internal junction capacitances is increased, causing  
a reduction in closed-loop bandwidth. To compensate for this,  
smaller values of feedback resistor are used at lower supply  
voltages.  
REV. D  
–9–  
AD811  
Driving Capacitive Loads  
100  
90  
80  
70  
60  
50  
40  
30  
20  
10  
0
The feedback and gain resistor values in Table I will result in  
very flat closed-loop responses in applications where the load  
capacitances are below 10 pF. Capacitances greater than this  
will result in increased peaking and overshoot, although not  
necessarily in a sustained oscillation.  
G = +2  
= ؎15V  
V
S
R
VALUE SPECIFIED  
S
IS FOR FLATTEST  
FREQUENCY RESPONSE  
There are at least two very effective ways to compensate for this  
effect. One way is to increase the magnitude of the feedback  
resistor, which lowers the 3 dB frequency. The other method is  
to include a small resistor in series with the output of the ampli-  
fier to isolate it from the load capacitance. The results of these  
two techniques are illustrated in Figure 32. Using a 1.5 kΩ  
feedback resistor, the output ripple is less than 0.5 dB when driv-  
ing 100 pF. The main disadvantage of this method is that it  
sacrifices a little bit of gain flatness for increased capacitive load  
drive capability. With the second method, using a series resistor,  
the loss of flatness does not occur.  
10  
100  
LOAD CAPACITANCE – pF  
1000  
Figure 33. Recommended Value of Series Resistor vs. the  
Amount of Capacitive Load  
R
FB  
Figure 33 shows recommended resistor values for different load  
capacitances. Refer again to Figure 32 for an example of the  
results of this method. Note that it may be necessary to adjust  
the gain setting resistor, RG, to correct for the attenuation which  
results due to the divider formed by the series resistor, RS, and  
the load resistance.  
+V  
S
0.1F  
R
R
G
R
(OPTIONAL)  
S
V
Applications which require driving a large load capacitance at a  
high slew rate are often limited by the output current available  
from the driving amplifier. For example, an amplifier limited to  
25 mA output current cannot drive a 500 pF load at a slew rate  
greater than 50 V/µs. However, because of the AD811’s 100 mA  
output current, a slew rate of 200 V/µs is achievable when driv-  
ing this same 500 pF capacitor (see Figure 34).  
OUT  
AD811  
V
IN  
C
R
L
L
T
0.1F  
–V  
S
2V  
100ns  
Figure 31. Recommended Connection for Driving a Large  
Capacitive Load  
100  
90  
V
IN  
12  
R
R
= 1.5k⍀  
= 0  
FB  
9
6
S
10  
V
OUT  
3
G = +2  
= ؎15V  
0%  
R
R
= 649⍀  
= 30⍀  
V
FB  
S
R
C
= 10k⍀  
= 100pF  
S
L
L
5V  
0
Figure 34. Output Waveform of an AD811 Driving a  
500 pF Load. Gain = +2, RFB = 649 , RS = 15 ,  
RS = 10 kΩ  
–3  
–6  
1M  
10M  
FREQUENCY – Hz  
100M  
Figure 32. Performance Comparison of Two Methods for  
Driving a Capacitive Load  
–10–  
REV. D  
AD811  
Operation as a Video Line Driver  
The AD811 has been designed to offer outstanding perfor-  
mance at closed-loop gains of one or greater, while driving  
multiple reverse-terminated video loads. The lowest differential  
gain and phase errors will be obtained when using ±15 volt  
power supplies. With ±12 volt supplies, there will be an insig-  
nificant increase in these errors and a slight improvement in  
gain flatness. Due to power dissipation considerations, ±12 volt  
supplies are recommended for optimum video performance.  
Excellent performance can be achieved at much lower supplies  
as well.  
1V  
10ns  
100  
90  
V
IN  
10  
V
OUT  
0%  
The closed-loop gain vs. frequency at different supply voltages  
is shown in Figure 36. Figure 37 is an oscilloscope photograph  
of an AD811 line driver’s pulse response with ±15 volt supplies.  
The differential gain and phase error vs. supply are plotted in  
Figures 38 and 39, respectively.  
1V  
Figure 37. Small Signal Pulse Response, Gain = +2,  
VS = ±15 V  
Another important consideration when driving multiple cables  
is the high frequency isolation between the outputs of the  
cables. Due to its low output impedance, the AD811 achieves  
better than 40 dB of output to output isolation at 5 MHz driv-  
ing back terminated 75 cables.  
0.10  
R = 649⍀  
0.09  
0.08  
0.07  
0.06  
0.05  
0.04  
0.03  
0.02  
0.01  
F
F
= 3.58MHz  
C
100 IRE  
MODULATED  
RAMP  
75CABLE  
649⍀  
649⍀  
V
#1  
OUT  
75⍀  
+V  
75⍀  
S
a. DRIVING A SINGLE, BACK TERMINATED,  
75COAX CABLE  
DRIVING TWO PARALLEL,  
0.1F  
b.  
BACK TERMINATED, COAX CABLES  
75CABLE  
b
V
#2  
OUT  
AD811  
75⍀  
75CABLE  
75⍀  
V
IN  
75⍀  
a
5
6
7
8
9
10  
11  
12  
13  
14  
15  
SUPPLY VOLTAGE – ؎Volts  
0.1F  
Figure 38. Differential Gain Error vs. Supply Voltage for  
the Video Line Driver of Figure 35  
–V  
S
Figure 35. A Video Line Driver Operating at a Gain of +2  
0.20  
12  
R
= 649⍀  
= 3.58MHz  
F
0.18  
0.16  
0.14  
0.12  
0.10  
0.08  
0.06  
0.04  
0.02  
F
C
G = +2  
100 IRE  
MODULATED  
RAMP  
V
R
= ؎15V  
S
R
R
= 150⍀  
= R  
9
6
L
= 649⍀  
FB  
G
FB  
a.DRIVING A SINGLE, BACK TERMINATED,  
75COAX CABLE  
DRIVING TWO PARALLEL,  
b.  
3
BACK TERMINATED, COAX CABLES  
V
= ؎5V  
S
R
= 562⍀  
FB  
b
0
–3  
–6  
a
5
6
7
8
9
10  
11  
12  
13  
14  
15  
1
10  
FREQUENCY – MHz  
100  
SUPPLY VOLTAGE – ؎Volts  
Figure 39. Differential Phase Error vs. Supply Voltage for  
the Video Line Driver of Figure 35  
Figure 36. Closed-Loop Gain vs. Frequency, Gain = +2  
REV. D  
–11–  
AD811  
An 80 MHz Voltage-Controlled Amplifier Circuit  
The gain can be increased to 20 dB (×10) by raising R8 and R9  
to 1.27 k, with a corresponding decrease in –3 dB bandwidth  
to about 25 MHz. The maximum output voltage under these  
conditions will be increased to ±9 V using ±12 V supplies.  
The voltage-controlled amplifier (VCA) circuit of Figure 40  
shows the AD811 being used with the AD834, a 500 MHz,  
4-quadrant multiplier. The AD834 multiplies the signal input  
by the dc control voltage, VG. The AD834 outputs are in the  
form of differential currents from a pair of open collectors,  
ensuring that the full bandwidth of the multiplier (which ex-  
ceeds 500 MHz) is available for certain applications. Here,  
the AD811 op amp provides a buffered, single-ended ground-  
referenced output. Using feedback resistors R8 and R9 of  
511 , the overall gain ranges from –70 dB, for VG = 0 dB to  
+12 dB, (a numerical gain of four), when VG = +1 V. The over-  
all transfer function of the VCA is:  
The gain-control input voltage, VG, may be a positive or nega-  
tive ground-referenced voltage, or fully differential, depending  
on the user’s choice of connections at Pins 7 and 8. A positive  
value of VG results in an overall noninverting response. Revers-  
ing the sign of VG simply causes the sign of the overall response  
to invert. In fact, although this circuit has been classified as a  
voltage-controlled amplifier, it is also quite useful as a general-  
purpose four-quadrant multiplier, with good load-driving capa-  
bilities and fully-symmetrical responses from X- and Y-inputs.  
V
OUT = 4 (X1 – X2)(Y1 – Y2)  
The AD811 and AD834 can both be operated from power  
supply voltages of ±5 V. While it is not necessary to power them  
from the same supplies, the common-mode voltage at W1 and  
W2 must be biased within the common-mode range of the  
AD811’s input stage. To achieve the lowest differential gain and  
phase errors, it is recommended that the AD811 be operated  
from power supply voltages of ±10 volts or greater. This VCA  
circuit is designed to operate from a ±12 volt dual power  
supply.  
which reduces to VOUT = 4 VG VIN using the labeling conven-  
tions shown in Figure 40. The circuit’s –3 dB bandwidth of  
80 MHz, is maintained essentially constant—independent of  
gain. The response can be maintained flat to within ±0.1 dB  
from dc to 40 MHz at full gain with the addition of an optional  
capacitor of about 0.3 pF across the feedback resistor R8. The  
circuit produces a full-scale output of ±4 V for a ±1 V input,  
and can drive a reverse-terminated load of 50 or 75 to ±2 V.  
FB  
+12V  
C1  
0.1F  
R1 100⍀  
R8*  
+
V
G
R2 100⍀  
8
7
6
5
R4  
182⍀  
R6  
294⍀  
X2  
X1 +V  
W1  
S
U1  
AD834  
U3  
AD811  
V
OUT  
–V  
3
S
Y1 Y2  
W2  
4
R7  
294⍀  
R5  
182⍀  
R
L
1
2
V
IN  
R9*  
R3  
249⍀  
C2  
0.1F  
–12V  
FB  
*R8 = R9 = 511FOR X4 GAIN  
= 1.27kFOR X10 GAIN  
Figure 40. An 80 MHz Voltage-Controlled Amplifier  
–12–  
REV. D  
AD811  
A Video Keyer Circuit  
The bias currents required at the output of the multipliers are  
provided by R8 and R9. A dc-level-shifting network comprising  
R10/R12 and R11/R13 ensures that the input nodes of the  
AD811 are positioned at a voltage within its common-mode  
range. At high frequencies C1 and C2 bypass R10 and R11  
respectively. R14 is included to lower the HF loop gain, and is  
needed because the voltage-to-current conversion in the  
AD834s, via the Y2 inputs, results in an effective value of the  
feedback resistance of 250 ; this is only about half the value  
required for optimum flatness in the AD811’s response. (Note  
that this resistance is unaffected by G: when G = 1, all the  
feedback is via U1, while when G = 0 it is all via U2). R14  
reduces the fractional amount of output current from the multi-  
pliers into the current-summing inverting input of the AD811,  
by sharing it with R8. This resistor can be used to adjust the  
bandwidth and damping factor to best suit the application.  
By using two AD834 multipliers, an AD811, and a 1 V dc  
source, a special form of a two-input VCA circuit called a  
video keyer can be assembled. “Keying” is the term used in  
reference to blending two or more video sources under the  
control of a third signal or signals to create such special effects  
as dissolves and overlays. The circuit shown in Figure 41 is a  
two-input keyer, with video inputs VA and VB, and a control  
input VG. The transfer function (with VOUT at the load) is  
given by:  
VOUT = G VA + (1–G) VB  
where G is a dimensionless variable (actually, just the gain of  
the “A” signal path) that ranges from 0 when VG = 0, to 1  
when VG = +1 V. Thus, VOUT varies continuously between VA  
and VB as G varies from 0 to 1.  
Circuit operation is straightforward. Consider first the signal  
path through U1, which handles video input VA. Its gain is  
clearly zero when VG = 0 and the scaling we have chosen  
ensures that it is unity when VG = +1 V; this takes care of the  
first term of the transfer function. On the other hand, the VG  
input to U2 is taken to the inverting input X2 while X1 is  
biased at an accurate +1 V. Thus, when VG = 0, the response  
to video input VB is already at its full-scale value of unity,  
whereas when VG = +1 V, the differential input X1–X2 is zero.  
This generates the second term.  
To generate the 1 V dc needed for the “1–G” term an AD589  
reference supplies 1.225 V ± 25 mV to a voltage divider consist-  
ing of resistors R2 through R4. Potentiometer R3 should be  
adjusted to provide exactly +1 V at the X1 input.  
In this case, we have shown an arrangement using dual supplies  
of ±5 V for both the AD834 and the AD811. Also, the overall  
gain in this case is arranged to be unity at the load, when it is  
driven from a reverse-terminated 75 line. This means that the  
“dual VCA” has to operate at a maximum gain of 2, rather  
C1  
+5V  
R7  
R14  
0.1F  
SETUP FOR DRIVING  
REVERSE-TERMINATED LOAD  
SEE TEXT  
45.3⍀  
R10  
2.49k⍀  
Z
V
OUT  
O
R5  
TO PIN 6  
AD811  
113⍀  
V
R6  
226⍀  
G
Z
200⍀  
200⍀  
O
(0 TO +1V dc)  
TO Y2  
8
7
6
5
X2  
X1 +V  
W1  
S
+5V  
R1  
INSET  
R8  
29.4⍀  
U1  
AD834  
R12  
6.98k⍀  
U4  
1.87k⍀  
AD589  
+5V  
Y1 Y2 –V  
W2  
4
S
R2  
174⍀  
2
1
3
V
A
FB  
C3  
0.1F  
(؎1V FS)  
–5V  
–5V  
+5V  
R3  
100⍀  
LOAD  
GND  
U3  
AD811  
R9  
29.4⍀  
R13  
6.98k⍀  
8
7
6
5
V
OUT  
R4  
1.02k⍀  
X2  
W1  
X1 +V  
S
C4  
0.1F  
C2  
0.1F  
U1  
AD834  
Y1 Y2 –V  
W2  
4
S
LOAD  
GND  
FB  
2
1
3
R11  
2.49k⍀  
V
B
–5V  
–5V  
(؎1V FS)  
Figure 41. A Practical Video Keyer Circuit  
REV. D  
–13–  
AD811  
than 4 as in the VCA circuit of Figure 40. However, this cannot  
be achieved by lowering the feedback resistor, since below a  
critical value (not much less than 500 ) the AD811’s peaking  
may be unacceptable. This is because the dominant pole in the  
open-loop ac response of a current-feedback amplifier is con-  
trolled by this feedback resistor. It would be possible to operate  
at a gain of X4 and then attenuate the signal at the output.  
Instead, we have chosen to attenuate the signals by 6 dB at the  
input to the AD811; this is the function of R8 through R11.  
R14 = 49.9⍀  
0
–10  
–20  
–30  
–40  
–50  
–60  
–70  
–80  
GAIN  
R14 = 137⍀  
ADJACENT  
CHANNEL  
FEEDTHROUGH  
Figure 42 is a plot of the ac response of the feedback keyer,  
when driving a reverse terminated 50 cable. Output noise and  
adjacent channel feedthrough, with either channel fully off and  
the other fully on, is about –50 dB to 10 MHz. The feedthrough  
at 100 MHz is limited primarily by board layout. For VG = +1 V,  
the –3 dB bandwidth is 15 MHz when using a 137 resistor for  
R14 and 70 MHz with R14 = 49.9 . For further information  
regarding the design and operation of the VCA and video keyer  
circuits, refer to the application note “Video VCA’s and Keyers  
Using the AD834 & AD811” by Brunner, Clarke, and Gilbert,  
available FREE from Analog Devices.  
10k  
100k  
1M  
FREQUENCY – Hz  
10M  
100M  
Figure 42. A Plot of the AC Response of the Video Keyer  
–14–  
REV. D  
AD811  
OUTLINE DIMENSIONS  
Dimensions shown in inches and (mm).  
8- Lead Plastic DIP (N) Package  
20-Lead LCC (E-20A) Package  
0.082 ± 0.018  
(2.085 ± 0.455)  
0.39 (9.91)  
MAX  
0.350 ± 0.008 SQ  
(8.89 ± 0.20) SQ  
0.040 x 45°  
(1.02 x 45°)  
REF 3 PLCS  
8
5
0.31  
(7.87)  
0.25  
(6.35)  
1
4
0.025 ± 0.003  
(0.635 ± 0.075)  
PIN 1  
0.30 (7.62)  
REF  
NO. 1 PIN  
INDEX  
0.10 (2.54)  
BSC  
0.035 ؎ 0.01  
(0.89 ؎ 0.25)  
0.050  
(1.27)  
0.165 ؎ 0.01  
(4.19 ؎ 0.25)  
0.011 ؎0.003  
(0.28 ؎ 0.08)  
0.020 x 45°  
(0.51 x 45°)  
REF  
0.18 ؎0.03  
(4.57 ؎ 0.75)  
0.125 (3.18)  
MIN  
15؇  
0؇  
0.018 ؎0.003  
(0.46 ؎ 0.08)  
SEATING  
PLANE  
0.033  
(0.84)  
NOM  
16-Lead SOIC (R-16) Package  
8-Lead Cerdip (Q) Package  
9
16  
0.005 (0.13) 0.055 (1.4)  
0.299 (7.60)  
0.291 (7.40)  
MIN  
MAX  
8
5
0.419 (10.65)  
PIN 1  
0.404 (10.26)  
8
0.310 (7.87)  
0.220 (5.59)  
1
PIN 1  
1
4
0.100 (2.54) BSC  
0.405 (10.29) MAX  
0.107 (2.72)  
0.413 (10.50)  
0.398 (10.10)  
0.320 (8.13)  
0.290 (7.37)  
0.089 (2.26)  
0.364 (9.246)  
0.344 (8.738)  
0.060 (1.52)  
0.015 (0.38)  
0.200.(5.08)  
MAX  
0.150  
(3.81)  
MIN  
0.045 (1.15)  
0.020 (0.50)  
0.200 (5.08)  
0.125 (3.18)  
0.010 (0.25)  
0.004 (0.10)  
0.050 (1.27)  
BSC  
0.018 (0.46)  
0.014 (0.36)  
0.015 (0.38)  
0.007 (1.18)  
0.015 (0.38)  
0.008 (0.20)  
SEATING  
PLANE  
15°  
0°  
0.023 (0.58) 0.070 (1.78)  
0.014 (0.36) 0.030 (0.76)  
20-Lead Wide Body SOIC (R-20) Package  
8-Lead SOIC (SO-8) Package  
0.512 (13.00)  
0.496 (12.60)  
0.1968 (5.00)  
0.1890 (4.80)  
20  
11  
8
1
5
4
0.2440 (6.20)  
0.2284 (5.80)  
0.1574 (4.00)  
0.1497 (3.80)  
0.300 (7.60)  
0.292 (7.40)  
0.419 (10.65)  
PIN 1  
0.394 (10.00)  
0.0196 (0.50)  
0.0099 (0.25)  
0.0500 (1.27)  
BSC  
10  
1
؋
 45؇  
0.0688 (1.75)  
0.0532 (1.35)  
0.0098 (0.25)  
0.0040 (0.10)  
SEATING  
PLANE  
0.50 (1.27)  
BSC  
0.019 (0.48)  
0.014 (0.36)  
8؇  
0؇  
0.0500 (1.27)  
0.0160 (0.41)  
0.0192 (0.49)  
0.0138 (0.35)  
0.0098 (0.25)  
0.0075 (0.19)  
0.104 (2.64)  
0.093 (2.36)  
0.011 (0.28)  
0.004 (0.10)  
0.015 (0.38)  
0.007 (0.18)  
0.050 (1.27)  
0.016 (0.40)  
REV. D  
–15–  

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