OP285 thereby reducing phase error dramatically. This is shown in A Low Noise, High Speed Instrumentation Amplifier Figure 13 where the 10x composite amplifier’s phase response A high speed, low noise instrumentation amplifier, constructed exhibits less than 1.5° phase shift through 500 kHz. On the other with a single OP285, is illustrated in Figure 15. The circuit exhibits hand, the single gain stage amplifier exhibits 25° of phase shift less than 1.2 µV p-p noise (RTI) in the 0.1 Hz to 10 Hz band over the same frequency range. An additional benefit of the low and an input noise voltage spectral density of 9 nV/√Hz (1 kHz) phase error configuration is constant group delay, by virtue of at a gain of 1000. The gain of the amplifier is easily set by RG constant phase shift at all frequencies below 500 kHz. Although according to the formula: this technique is valid for minimum circuit gains of 10, actual closed-loop magnitude response must be optimized for the VOUT 9 9 . 8 kΩ = + 2 amplifier chosen. VIN RG The advantages of a two op amp instrumentation amplifier based on a dual op amp is that the errors in the individual am- LOW PHASE ERROR0AMPLIFIER RESPONSE plifiers tend to cancel one another. For example, the circuit’s input offset voltage is determined by the input offset voltage –5 matching of the OP285, which is typically less than 250 µV. –10–15+SINGLE STAGE5AMPLIFIER RESPONSEVIN3Degrees7–20––1A2V6OUT2 A1–25AC CMRR TRIMR34.99kPHASE –30R4R2C14.99k4.99–355pF–40pFRGA1, A2 = 1/2 OP285R1–409.98k4.99kGAIN =+2DC CMRR TRIMRQ–45GAINR10k100k1M10MG()P1START 10,000.000HzSTOP 10,000,000.000Hz2OPEN500101.24k100102 Figure 13. Phase Error Comparison 100010 For a more detailed treatment on the design of low phase error Figure 15. A High-Speed Instrumentation Amplifier amplifiers, see Application Note AN-107. Common-mode rejection of the circuit is limited by the matching Fast Current Pump of resistors R1 to R4. For good common-mode rejection, these A fast, 30 mA current source, illustrated in Figure 14, takes resistors ought to be matched to better than 1%. The circuit was advantage of the OP285’s speed and high output current drive. constructed with 1% resistors and included potentiometer P1 This is a variation of the Howland current source where a sec- for trimming the CMRR and a capacitor C1 for trimming the ond amplifier, A2, is used to increase load current accuracy and CMRR. With these two trims, the circuit’s common-mode output voltage compliance. With supply voltages of ± 15 V, the rejection was better than 95 dB at 60 Hz and better than 65 dB output voltage compliance of the current pump is ± 8 V. To at 10 kHz. For the best common-mode rejection performance, keep the output resistance in the MΩ range requires that 0.1% use a matched (better than 0.1%) thin-film resistor network for or better resistors be used in the circuit. The gain of the current R1 through R4 and use the variable capacitor to optimize the pump can be easily changed according to the equations shown circuit’s CMR. in the diagram. The instrumentation amplifier exhibits very wide small- and R1R2 large-signal bandwidths regardless of the gain setting, as shown 2k2kVIN1 in the table. Because of its low noise, wide gain-bandwidth 2R5 product, and high slew rate, the OP285 is ideally suited for high R3150A12k3 speed signal conditioning applications. VIN2R45VIN2 – V IN1VIN=2kIOUT =7R5R5A2Circuit RGCircuit Bandwidth6IOUT = (MAX) =30mAA1, A2 = 1/2 OP285Gain ()VOUT = 100 mV p-p VOUT = 20 V p-pR2GAIN = , R4 = R2, R3 = R1R1 2 Open 5 MHz 780 kHz Figure 14. A Fast Current Pump 10 1.24 k 1 MHz 460 kHz 100 102 90 kHz 85 kHz 1000 10 10 kHz 10 kHz –10– REV. C