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AD830 数据表(PDF) 14 Page - Analog Devices |
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AD830 数据表(HTML) 14 Page - Analog Devices |
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14 / 16 page ![]() AD830 REV. A –14– Loop Through or Line Bridging Amplifier (Figure 37) The AD830 is ideally suited for use as a video line bridging am- plifier. The video signal is tapped from the conductor of the cable relative to its shield. The high input impedance of the AD830 provides negligible loading on the cable. More signifi- cantly, the benign loading is maintained while the AD830 is powered-down. Coupled with its good video load driving per- formance, the AD830 is well suited to video cable monitoring applications. 45 36 AD830 1 2 8 7 A=1 VP 0.1µF VOUT VN 0.1µF GM GM RG 75 Ω 75 Ω 499 Ω 499 Ω OPTIONAL CC 249 Ω C Figure 37. Cable Tap Amplifier Resistorless Summing Direct, two input, resistorless summing is easily realized from the general unity gain mode. By grounding VX2 and applying the two inputs to VX1 and VY1, the output is the exact sum of the applied voltages V1 and V3, relative to common; VOUT = V1 + V3. A diagram of this simple, but potent application is shown below in Figure 38. The AD830 summing circuit possesses sev- eral virtues not present in the classic op amp based summing circuits. It has high impedance inputs, no resistors, very precise summing, high reverse isolation and noninverting gain. Achiev- ing this function and performance with op amps requires signifi- cantly more components. 45 36 AD830 1 2 8 7 A=1 VOUT = V1 + V3 VP OUT VN GM GM V1 V3 C Figure 38. Resistorless Summing Amplifier 2 Gain Bandwidth Line Driver A gain of two, without the use of resistors, is possible with the AD830. This is accomplished by grounding VX2, tying the two inputs VX1 and VY1 together and applying the input, VIN, to this wired connection. The output is exactly twice the applied volt- age, VIN; VOUT = 2 VIN. Figure 39 below shows the connec- tions for this highly useful application. The most notable characteristic of this alternative gain of two is that there is no loss of bandwidth as in a voltage feedback op amp based gain of +2 where the bandwidth is halved, therefore, the gain band- width is doubled. Also, this circuit is accurate without the need for any precise valued resistors, as in the op amp equivalents, and it possess excellent differential gain and phase performance as shown in Figures 40 and 41. 45 36 AD830 1 2 8 7 A=1 VP 0.1µF VOUT VN 0.1µF GM GM 75 Ω 75 Ω VIN C Figure 39. Full Bandwidth Line Driver (G = +2) SUPPLY VOLTAGE – ±Volts .10 15 .03 .01 6 .02 5 .06 .04 .05 .07 .08 .09 14 13 12 11 10 9 8 7 .20 .06 .02 .04 .12 .08 .10 .14 .16 .18 PHASE GAIN GAIN = +2 R L = 150Ω FREQ = 3.58MHz 0 TO 0.7V Figure 40. Differential Gain and Phase for the Circuit of Figure 39 0.2 –0.3 –0.8 100k 100M 10M 1M 10k –0.2 –0.1 0 0.1 –0.7 –0.6 –0.5 –0.4 FREQUENCY – Hz V S = ±15V V S = ±10V V S = ±5V R L = 150Ω GAIN = +2 Figure 41. 0.1 dB Gain Flatness for the Circuit of Figure 39 |
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