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ADA4500-2ACPZ-R7 数据表(PDF) 19 Page - Analog Devices |
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ADA4500-2ACPZ-R7 数据表(HTML) 19 Page - Analog Devices |
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19 / 24 page ![]() Data Sheet ADA4500-2 Rev. A | Page 19 of 24 THEORY OF OPERATION RAIL-TO-RAIL OUTPUT When processing a signal through an op amp to a load, it is often desirable to have the output of the op amp swing as close to the voltage supply rails as possible. For example, when an op amp is driving an ADC and both the op amp and ADC are using the same supply rail voltages, the op amp must drive as close to the V+ and V− rails as possible so that all codes in the ADC are usable. A non-rail-to-rail output can require as much as 1.5 V or more between the output and the rails, thus limiting the input dynamic range to the ADC, resulting in less precision (number of codes) in the converted signal. The ADA4500-2 can drive its output to within a few millivolts of the supply rails (see the output voltage high and output voltage low specifications in Table 1 and Table 2). The rail-to-rail output maximizes the dynamic range of the output, increasing the range and precision, and often saving the cost, board space, and added error of the additional gain stages. RAIL-TO-RAIL INPUT (RRI) Using a CMOS nonrail-to-rail input stage (that is, a single differential pair) limits the input voltage to approximately one gate- source voltage (VGS) away from one of the supply lines. Because VGS for normal operation is commonly more than 1 V, a single differential pair, input stage op amp greatly restricts the allowable input voltage. This can be quite limiting with low supply voltages supplies. To solve this problem, RRI stages are designed to allow the input signal to range to the supply voltages (see the input voltage range specifications in Table 1 and Table 2). In the case of the ADA4500-2, the inputs continue to operate 200 mV beyond the supply rails (see Figure 7 and Figure 10). ZERO CROSS-OVER DISTORTION A typical rail-to-rail input stage uses two differential pairs (see Figure 59). One differential pair amplifies the input signal when the common-mode voltage is on the high end, and the other pair amplifies the input signal when the common-mode voltage is on the low end. This classic dual-differential pair topology does have a potential drawback. If the signal level moves through the range where one input stage turns off and the other input stage turns on, noticeable distortion occurs. Figure 60 shows the distortion in a typical plot of VOS (voltage difference between the inverting and the noninverting input) vs. VCM (input voltage). VDD M10 M9 M12 M11 M8 M7 M6 M5 VSS BIAS5 BIAS4 BIAS3 –AV OUT VSS BIAS2 M3 M4 VDD BIAS1 M1 M2 VIN+ VIN– Figure 59. Typical PMOS-NMOS Rail-to-Rail Input Structure VCM (V) 0 –300 –100 100 300 1.5 3.5 5.0 1.0 0.5 2.5 4.5 4.0 3.0 2.0 –200 –150 –250 –50 0 50 150 200 250 VSY = 5V TA = 25°C Figure 60. Typical Input Offset Voltage (VOS) vs. Common-Mode Voltage (VCM) Response in a Dual Differential Pair Input Stage Op Amp (Powered by a 5 V Supply; Results of Approximately 100 Units per Graph Are Displayed) This distortion in the offset error forces the designer to live with the bump in the common-mode error or devise impractical ways to avoid the crossover distortion areas, thereby narrowing the common-mode dynamic range of the op amp. |
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