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ADA4891-2ARMZ-R7 数据表(PDF) 16 Page - Analog Devices |
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ADA4891-2ARMZ-R7 数据表(HTML) 16 Page - Analog Devices |
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16 / 24 page ![]() ADA4891-1/ADA4891-2/ADA4891-3/ADA4891-4 Rev. B | Page 16 of 24 Table 6. Recommended Component Values and Effect of Gain on ADA4891-3/ADA4891-4 Performance (RL = 1 kΩ) Feedback Network Values −3 dB Small-Signal Bandwidth (MHz) Slew Rate (V/μs) Peaking (dB) Gain RF (Ω) RG (Ω) VOUT = 200 mV p-p tR tF −1 453 453 97 186 194 0.9 +1 0 Open 220 151 262 4.1 +2 453 453 97 181 223 0.9 +5 453 90.6 31 112 120 0 +10 453 45.3 13 68 67 0 EFFECT OF RF ON 0.1 dB GAIN FLATNESS Gain flatness is an important specification in video applications. It represents the maximum allowable deviation in the signal amplitude within the pass band. Tests have revealed that the human eye is unable to distinguish brightness variations of less than 1%, which translates into a 0.1 dB signal drop within the pass band or, put simply, 0.1 dB gain flatness. The PCB layout configuration and bond pads of the chip often contribute to stray capacitance. The stray capacitance at the inverting input forms a pole with the feedback and gain resistors. This additional pole adds phase shift and reduces phase margin in the closed-loop phase response, causing instability in the amplifier and peaking in the frequency response. Figure 52 and Figure 53 show the effect of using various values for Feedback Resistor RF on the 0.1 dB gain flatness of the parts. Figure 52 shows the effect for the ADA4891-1/ADA4891-2. Figure 53 show the effect for the ADA4891-3/ADA4891-4. Note that a larger RF value causes more peaking because the additional pole formed by RF and the input stray capacitance shifts down in frequency and interacts significantly with the internal poles of the amplifier. –0.4 –0.3 –0.2 –0.1 0 0.1 0.2 1 0.1 10 100 FREQUENCY (MHz) VS = 5V G = +2 VOUT = 2V p-p RL = 150Ω RG = RF = 604Ω RG = RF = 549Ω RG = RF = 649Ω RG = RF = 698Ω Figure 52. 0.1 dB Gain Flatness, Noninverting Gain Configuration, ADA4891-1/ADA4891-2 –0.4 –0.5 –0.3 –0.2 –0.1 0 0.1 0.2 0.3 1 0.1 10 100 FREQUENCY (MHz) VS = 5V G = +2 VOUT = 2V p-p RL = 150Ω RG = RF = 453Ω RG = RF = 402Ω RG = RF = 357Ω RG = RF = 301Ω Figure 53. 0.1 dB Gain Flatness, Noninverting Gain Configuration, ADA4891-3/ADA4891-4 To obtain the desired 0.1 dB bandwidth, adjust the feedback resistor, RF, as shown in Figure 52 and Figure 53. If RF cannot be adjusted, a small capacitor can be placed in parallel with RF to reduce peaking. The feedback capacitor, CF, forms a zero with the feedback resistor, which cancels out the pole formed by the input stray capacitance and the gain and feedback resistors. For a first pass in determining the CF value, use the following equation: RG × CS = RF × CF where: RG is the gain resistor. CS is the input stray capacitance. RF is the feedback resistor. CF is the feedback capacitor. Using this equation, the original closed-loop frequency response of the amplifier is restored, as if there is no stray input capacitance. Most often, however, the value of CF is determined empirically. Figure 54 shows the effect of using various values for the feedback capacitor to reduce peaking. In this case, the ADA4891-1/ ADA4891-2 are used for demonstration purposes and RF = RG = 604 Ω. The input stray capacitance, together with the board parasitics, is approximately 2 pF. |
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