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ADA4927-2YCPZ-R2 数据表(PDF) 21 Page - Analog Devices |
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ADA4927-2YCPZ-R2 数据表(HTML) 21 Page - Analog Devices |
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21 / 25 page ![]() Data Sheet ADA4927-1/ADA4927-2 Rev. B | Page 21 of 25 RTS = RTH = RS||RT = 26.5 Ω. Note that VTH is greater than 1 V p-p, which was obtained with RT = 50 Ω. The modified circuit with the Thevenin equivalent (closest 1% value used for RTH) of the terminated source and RTS in the lower feedback loop is shown in Figure 53. ADA4927 RL VOUT, dm +VS –VS RTH 26.7Ω RG 348Ω RG 348Ω RF 348Ω RF 348Ω VOCM VTH 1.06V p-p RTS 26.7Ω Figure 53. Thevenin Equivalent and Matched Gain Resistors Figure 53 presents a tractable circuit with matched feedback loops that can be easily evaluated. It is useful to point out two effects that occur with a terminated input. The first is that the value of RG is increased in both loops, lowering the overall closed-loop gain. The second is that VTH is a little larger than 1 V p-p, as it is when RT = 50 Ω. These two effects have opposite impacts on the output voltage, and for large resistor values in the feedback loops (~1 kΩ), the effects essentially cancel each other out. For small RF and RG, or high gains, however, the diminished closed-loop gain is not canceled completely by the increased VTH. This can be seen by evaluating Figure 53. The desired differential output in this example is 1 V p-p because the terminated input signal is 1 V p-p and the closed- loop gain = 1. The actual differential output voltage, however, is equal to (1.06 V p-p)(348/374.7) = 0.984 V p-p. To obtain the desired output voltage of 1 V p-p, a final gain adjustment can be made by increasing RF without modifying any of the input circuitry. This is discussed in Step 4. 4. The feedback resistor value is modified as a final gain adjustment to obtain the desired output voltage. To make the output voltage VOUT = 1 V p-p, RF must be calculated using the following formula: 35 06 . 1 Ω 374.7 1 , p p V p p V V R R V Desired R TH TS G dm OUT F The closest standard 1% values to 353 Ω are 348 Ω and 357 Ω. Choosing 357 Ω for RF gives a differential output voltage of 1.01 V p-p. The closed-loop bandwidth is diminished by a factor of approximately 348/357 from what it would be with RF = 348 Ω due to the inversely proportional relationship between RF and closed-loop gain that is characteristic of current feedback amplifiers. The final circuit is shown in Figure 54. ADA4927 RL VOUT, dm 1.01V p-p +VS –VS RS 50Ω RG 348Ω RG 348Ω RF 357Ω RF 357Ω VOCM VS 2V p-p 1V p-p RT 56.2Ω RTS 26.7Ω Figure 54. Terminated Single-Ended-to-Differential System with G = 1 INPUT COMMON-MODE VOLTAGE RANGE The ADA4927 input common-mode range is centered between the two supply rails, in contrast to other ADC drivers with level-shifted input ranges, such as the ADA4937. The centered input common- mode range is best suited to ac-coupled, differential-to-differential, and dual supply applications. For operation with ±5 V supplies, the input common-mode range at the summing nodes of the amplifier is specified as −3.5 V to +3.5 V and is specified as +1.3 V to +3.7 V with a single +5 V supply. To avoid nonlinearities, the voltage swing at the +IN and −IN terminals must be confined to these ranges. INPUT AND OUTPUT CAPACITIVE AC COUPLING Input ac coupling capacitors can be inserted between the source and RG. This ac coupling blocks the flow of the dc common- mode feedback current and causes the ADA4927 dc input common-mode voltage to equal the dc output common-mode voltage. These ac coupling capacitors must be placed in both loops to keep the feedback factors matched. Output ac coupling capacitors can be placed in series between each output and respective load. See Figure 58 for an example that uses input and output capacitive ac coupling. SETTING THE OUTPUT COMMON-MODE VOLTAGE The VOCM pin of the ADA4927 is internally biased with a voltage divider comprising two 10 kΩ resistors at a voltage approximately equal to the midsupply point, [(+VS) + (−VS)]/2. Because of this internal divider, the VOCM pin sources and sinks current, depending on the externally applied voltage and associated source resistance. Relying on the internal bias results in an output common-mode voltage that is within about 100 mV of the expected value. In cases where accurate control of the output common-mode level is required, it is recommended that an external source or resistor divider be used with source resistance less than 100 Ω. The output common-mode offset listed in the Specifications section presumes that the VOCM input is driven by a low impedance voltage source. It is also possible to connect the VOCM input to a common-mode level (CML) output of an ADC; however, care must be taken to ensure that the output has sufficient drive capability. The input impedance of the VOCM pin is approximately 10 kΩ. If multiple ADA4927 devices share one ADC reference output, a buffer may be necessary to drive the parallel inputs. |
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