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AD830 датащи(PDF) 12 Page - Analog Devices |
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AD830 датащи(HTML) 12 Page - Analog Devices |
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12 / 20 page ![]() AD830 Data Sheet Rev. D | Page 12 of 20 VX1 VOUT IY IX CC A = 1 GM AOLS= GMRP VX2 GM VY1 VY2 RP IZ IX = (VX1 – VX2) GM IY = (VY1 – VY2) GM IZ = IX + IY 1 + S (CCRP) Figure 26. Topology Diagram VX1 VOUT IY IX CC A = 1 GM 1 VX2 GM VY1 VY2 VX1 – VX2 = VY2 – VY1 FOR VY2 = VOUT VOUT = (VX1 – VX2 + VY1) 1 + S(C C/GM) Figure 27. Closed-Loop Connection Precise amplification is accomplished through closed-loop operation of this topology. Voltage feedback is implemented via the Y GM stage where the output is connected to the −Y input for negative feedback, as shown in Figure 27. An input signal is applied across the X GM stage, either fully differential or single- ended referred to common. It produces a current signal that is summed at the high impedance node with the output current from the Y GM stage. Negative feedback nulls this sum to a small error current necessary to develop the output voltage at the high impedance node. The error current is usually negligible, so the null condition essentially forces the Y GM output stage current to equal the exact X GM output current. Because the two transconductances are identical, the differential voltage across the Y inputs equals the negative of the differential voltage across the X input; VY = −VX or, more precisely, VY2 − VY1 = VX1 − VX2. This simple relation provides the basis to easily analyze any function possible to synthesize with the AD830, including any feedback situation. The bandwidth of the circuit is defined by the GM and the capacitor, CC. The highly linear GM stages give the amplifier a single-pole response, excluding the output amplifier and loading effects. It is important to note that the bandwidth and general dynamic behavior is symmetrical (identical) for the noninverting and the inverting connections of the AD830. In addition, the input impedance and CMRR are the same for either connection. This is very advantageous and unlike in a voltage or current feedback amplifier where there is a distinct difference in performance between the inverting and noninverting gain. The practical importance of this cannot be overemphasized and is a key feature offered by the AD830 amplifier topology. INTERFACING THE INPUT Common-Mode Voltage Range The common-mode range of the AD830 is defined by the amplitude of the differential input signal and the supply voltage. The general definition of common-mode voltage, VCM, is usually applied to a symmetrical differential signal centered around a particular voltage, as illustrated in Figure 28. This is the meaning implied here for common-mode voltage. The internal circuitry establishes the maximum allowable voltage on the input or feedback pins for a given supply voltage. This constraint and the differential input voltage sets the common- mode voltage limit. Figure 29 shows a curve of the common- mode voltage range versus the differential voltage for three supply voltage settings. VMAX VCM VPEAK Figure 28. Common-Mode Definition DIFFERENTIAL INPUTVOLTAGE (VPEAK) 15 0 0 2.0 0.4 0.8 1.2 1.6 6 3 12 9 ±5V = VS ±15V = VS –VCM –VCM +VCM +VCM +VCM ±10V = VS –VCM Figure 29. Input Common-Mode Voltage Range vs. Differential Input Voltage Differential Voltage Range The maximum applied differential voltage is limited by the clipping range of the input stages. This is nominally set at a 2.4 V magnitude and depicted in the cross plot (X-Y) in Figure 30. The useful linear range of the input stages is set at 2 V but is actually a function of the distortion required for a particular application. The distortion increases for larger differential input voltages. A plot of relative distortion versus the input differential voltage is shown in Figure 13 and Figure 16. The distortion characteristics impose a secondary limit to the differential input voltage for high accuracy applications. |
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