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ADA4891-2ARMZ-R7 数据表(PDF) 13 Page - Analog Devices |
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ADA4891-2ARMZ-R7 数据表(HTML) 13 Page - Analog Devices |
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13 / 20 page ![]() ADA4891-1/ADA4891-2 Rev. A | Page 13 of 20 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 resistor. 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 43 shows the effect of using various values of Feedback Resistor RF on the 0.1 dB gain flatness. 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 43. Noninverting Configuration To get the desired 0.1 dB bandwidth, adjust the feedback resistor, RF, as shown in Figure 43. 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 resistor. For a first pass in determining the CF value, use the equation RG × CS = RF × CF, where RG is the gain resistor, CS is the input stray capacitance, RF is the feedback resistor, and CF is the feedback capacitor. This is the condition where 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 44 shows the effect of using various values for the feedback capacitors to reduce peaking. In this case, RF = RG = 604 Ω. The input stray capacitance, together with the board parasitics, is approximately 2 pF. 0.3 0.2 0.1 0 0.1 0.2 0.1 1 10 100 FREQUENCY (MHz) CF = 3.3pF CF = 0pF CF = 1pF VS = 5V G = 2 RF = 604Ω RL = 150Ω VOUT = 2V p-p Figure 44. 0.1 dB Gain Flatness vs. CF, VS = 5 V |
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