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ADA4851-1YRJZ-R2 数据表(PDF) 13 Page - Analog Devices |
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ADA4851-1YRJZ-R2 数据表(HTML) 13 Page - Analog Devices |
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13 / 20 page ![]() ADA4851-1/ADA4851-2/ADA4851-4 Rev. E | Page 13 of 20 CIRCUIT DESCRIPTION The ADA4851-1/ADA4851-2/ADA4851-4 feature a high slew rate input stage that is a true single-supply topology, capable of sensing signals at or below the minus supply rail. The rail-to-rail output stage can pull within 60 mV of either supply rail when driving light loads and within 0.17 V when driving 150 Ω. High speed performance is maintained at supply voltages as low as 2.7 V. HEADROOM CONSIDERATIONS These amplifiers are designed for use in low voltage systems. To obtain optimum performance, it is useful to understand the behavior of the amplifiers as input and output signals approach the headroom limits of the amplifiers. The input common-mode voltage range of the amplifiers extends from the negative supply voltage (actually 200 mV below this), or from ground for single- supply operation, to within 2.2 V of the positive supply voltage. Therefore, at a gain of 3, the amplifiers can provide full rail-to- rail output swing for supply voltages as low as 3.3 V and down to 3 V for a gain of 4. Exceeding the headroom limit is not a concern for any inverting gain on any supply voltage, as long as the reference voltage at the positive input of the amplifier lies within the input common- mode range of the amplifier. The input stage is the headroom limit for signals approaching the positive rail. Figure 40 shows a typical offset voltage vs. the input common-mode voltage for the ADA4851-1/ADA4851-2/ ADA4851-4 amplifiers on a ±5 V supply. Accurate dc performance is maintained from approximately 200 mV below the negative supply to within 2.2 V of the positive supply. For high speed signals, however, there are other considerations. Figure 41 shows −3 dB bandwidth vs. input common-mode voltage for a unity-gain follower. As the common-mode voltage gets within 2 V of positive supply, the amplifier responds well but the bandwidth begins to drop as the common-mode voltage approaches the positive supply. This can manifest itself in increased distortion or settling time. Higher frequency signals require more headroom than the lower frequencies to maintain distortion performance. 600 580 560 540 520 500 480 460 440 –6 –5 –4 –3 –2 –1 0 1 2 3 4 VCM (V) Figure 40. VOS vs. Common-Mode Voltage, VS = ±5 V –6 –5 –4 –3 –2 –1 0 1 0.1 10 1 100 FREQUENCY (MHz) 2 1000 G = +1 RL = 1kΩ VS = 5V VCM = 3.0V VCM = 3.1V VCM = 3.2V VCM = 3.3V Figure 41. Unity-Gain Follower Bandwidth vs. Input Common-Mode |
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