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ADA4051-1ARJZ-R2 数据表(PDF) 17 Page - Analog Devices |
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ADA4051-1ARJZ-R2 数据表(HTML) 17 Page - Analog Devices |
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17 / 22 page ![]() Data Sheet ADA4051-1/ADA4051-2 Rev. C | Page 17 of 22 THEORY OF OPERATION The ADA4051-1/ADA4051-2 micropower chopper operational amplifiers feature a novel, patent-pending technique that sup- presses offset-related ripple in a chopper amplifier. Instead of filtering the ripple in the ac domain, this technique nulls the initial offset of the amplifier in the dc domain, thus preventing ripple at the overall output. Auto-zeroing and chopping are two techniques widely used in high precision CMOS amplifiers to achieve low offset, low offset drift, and no 1/f noise. Each of these techniques has pros and cons. Auto-zeroing results in more in-band noise due to aliasing introduced by sampling. On the other hand, chopping produces offset-related ripple because it modulates the initial offset associated with the amplifier up to its chopping frequency. To accomplish the best noise vs. power trade-off, the chopping technique is the better approach when designing a low offset amplifier because there is no increased in-band noise. It is preferable to suppress the offset-related ripple inside a chopper amplifier because the offset-related ripple would otherwise need to be eliminated by an extra off-chip postfilter. Figure 59 shows the block diagram design of the ADA4051-1/ ADA4051-2 chopper amplifiers employing a local feedback loop called autocorrection feedback (ACFB). The main signal path contains an input chopping switch network (CHOP1), a first transconductance amplifier (Gm1), an output chopping switch network (CHOP2), a second transconductance amplifier (Gm2), and a third transconductance amplifier (Gm3). CHOP1 and CHOP2 operate at 40 kHz of chopping frequency to modulate the initial offset and 1/f noise from Gm1 up to the chopping frequency. A fourth transconductance amplifier (Gm4) in the ACFB senses the modulated ripple at the output of CHOP2, caused by the initial offset voltage of Gm1. Then, the ripple is demodulated down to a dc domain through a third chopping switch network (CHOP3), operating with the same chopping clock as CHOP1 and CHOP2. Finally, a null transconductance amplifier (Gm5) tries to null any dc component at the output of Gm1 that would otherwise appear in the overall output as ripple. A switched-capacitor notch filter (NF) functions to selectively suppress the undesired offset-related ripple without disturbing the desired input signal from the overall input. The desired input dc signal appears as a dc signal at the output of CHOP2. Then, the initial offset is modulated up to the chopping frequency by CHOP3 and filtered out by the NF. Therefore, initial offset does not create any feedback and does not disturb the desired input signal. The NF is synchronized with the chopping clock to filter out the modulated component. In the same manner, the offset of Gm5 is filtered out by the combination of CHOP3 and the NF, enabling accurate ripple sensing at the output of CHOP2. In parallel with the high dc gain path, a feedforward transcon- ductance amplifier (Gm6) is added to bypass the phase shift introduced by the ACFB at the chopping frequency. Gm6 is designed to have the same transconductance as Gm1 to avoid pole-zero doublets. This design prevents any instability introduced by the ACFB in the overall feedback loop. Gm6 (= Gm1) C2 C1 Gm3 C3 NF Gm1 Gm2 CHOP1 CHOP2 Gm4 Gm5 CHOP3 OUT +IN –IN Figure 59. ADA4051-1/ADA4051-2 Chopper Amplifiers Block Diagram The voltage noise density, which is equal to the thermal noise floor dominated by the Gm1, is essentially flat from dc to the chopping frequency because CHOP1 and CHOP2 eliminate the 1/f noise generated in Gm1 and the ACFB does not contribute any additional noise. Although the ACFB suppresses the ripple related to the chopping, there is a remaining voltage ripple. To further suppress the remaining ripple down to a desired level, it is recommended to have a postfilter at the output of the amplifier. The remaining voltage ripple originates from two sources. The first type of ripple is due to the residual ripple associated with the initial offset of the Gm1. It is proportional to the magnitude of the initial offset and creates a spectrum at the chopping frequency (fCHOP). When the amplifier is configured as a unity- gain buffer, this ripple has a typical value of 4.9 μV rms and a maximum of 34.7 μV rms. The second type of ripple is due to the intermodulation between the high frequency input signal and the chopping frequency. This ripple depends on the input frequency (fIN) and creates a spectrum at frequencies equal to the difference between the chopping frequency and the input frequency (fCHOP − fIN), as well as at frequencies equal to the summation of the chopping frequency and the input frequency (fCHOP + fIN). The magnitude of the ripple for different input frequencies is shown in Figure 60. 0 100 200 300 400 500 0123456789 10 INPUT FREQUENCY (kHz) Figure 60. ADA4051-1/ADA4051-2 Modulated Output Ripple vs. Input Frequency |
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