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AD8290ACPZ-R7 数据表(PDF) 14 Page - Analog Devices |
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AD8290ACPZ-R7 数据表(HTML) 14 Page - Analog Devices |
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14 / 20 page ![]() AD8290 Rev. B | Page 14 of 20 THEORY OF OPERATION AMPLIFIER The amplifier of the AD8290 is a precision current-mode correction instrumentation amplifier. It is internally set to a fixed gain of 50. The current-mode correction topology results in excellent accuracy. Figure 43 shows a simplified diagram illustrating the basic operation of the instrumentation amplifier within the AD8290 (without correction). The circuit consists of a voltage-to-current amplifier (M1 to M6), followed by a current-to-voltage amplifier (R2 and A1). Application of a differential input voltage forces a current through R1, resulting in a conversion of the input voltage to a signal current. Transistors M3 to M6 transfer twice the signal current to the inverting input of the op amp, A1. A1 and R2 form a current-to-voltage converter to produce a rail-to- rail output voltage, VOUT. Op Amp A1 is a high precision auto-zero amplifier. This amplifier preserves the performance of the autocorrecting, current-mode amplifier topology while offering the user a true voltage-in, voltage-out instrumentation amplifier. Offset errors are corrected internally. An internal 0.9 V reference voltage is applied to the noninverting input of A1 to set the output offset level. External Capacitor CFILTER is used to filter out correction noise. HIGH POWER SUPPLY REJECTION (PSR) AND COMMON-MODE REJECTION (CMR) PSR and CMR indicate the amount that the offset voltage of an amplifier changes when its common-mode input voltage or power supply voltage changes. The autocorrection architecture of the AD8290 continuously corrects for offset errors, including those induced by changes in input or supply voltage, resulting in exceptional rejection performance. The continuous autocorrection provides great CMR and PSR performances over the entire operating temperature range (−40°C to +85°C). 1/f NOISE CORRECTION Flicker noise, also known as 1/f noise, is noise inherent in the physics of semiconductor devices and decreases 10 dB per decade. The 1/f corner frequency of an amplifier is the frequency at which the flicker noise is equal to the broadband noise of the amplifier. At lower frequencies, flicker noise dominates causing large errors in low frequency or dc applications. Flicker noise appears as a slowly varying offset error that is reduced by the autocorrection topology of the AD8290, allowing the AD8290 to have lower noise near dc than standard low noise instrumentation amplifiers. I I I – IR1 M2 VINP M3 M4 M1 R1 (VINP – VINN) IR1 = R1 2I 2I VINN VBIAS M5 M6 I – IR1 I + IR1 2IR1 CFILTER R2 R3 VREF = 0.9V A1 VINP – VINN R1 2R2 VOUT = VREF EXTERNAL + VCC Figure 43. Simplified Schematic of the Instrumentation Amplifier Within the AD8290 |
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