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AD8597ACPZ-R2 数据表(PDF) 15 Page - Analog Devices |
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AD8597ACPZ-R2 数据表(HTML) 15 Page - Analog Devices |
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15 / 20 page ![]() Data Sheet AD8597/AD8599 Rev. E | Page 15 of 20 FUNCTIONAL OPERATION INPUT VOLTAGE RANGE The AD8597/AD8599 are not rail-to-rail input amplifiers; therefore, care is required to ensure that both inputs do not exceed the input voltage range. Under normal negative feedback operating conditions, the amplifier corrects its output to ensure that the two inputs are at the same voltage. However, if either input exceeds the input voltage range, the loop opens and large currents begin to flow through the ESD protection diodes in the amplifier. These diodes are connected between the inputs and each supply rail to protect the input transistors against an electrostatic discharge event and they are normally reverse-biased. However, if the input voltage exceeds the supply voltage, these ESD diodes can become forward-biased. Without current limiting, excessive amounts of current may flow through these diodes, causing permanent damage to the device. If inputs are subject to over- voltage, insert appropriate series resistors to limit the diode current to less than 5 mA maximum. The input stage has two diodes between the input pins to protect the differential pair. Under high slew rate conditions, when the op amp is connected as a voltage follower, the diodes may become forward-biased and the source may try to drive the output. Place a small resistor in the feedback loop and in the noninverting input. The noise of a 100 Ω resistor at room temperature is ~1.25 nV/√Hz, which is higher than the AD8597/AD8599. Thus, there is a tradeoff between noise performance and protection. If possible, place limiting earlier in the signal path. For further details, see the Amplifier Input Protection… Friend or Foe? article at http://www.analog.com/amplifier_input. Because of the large transistors used to achieve low noise, the input capacitance may seem rather high. To take advantage of the low noise performance, impedance around the op amp must be low, less than 500 Ω. Under these conditions, the pole from the input capacitance must be greater than 50 MHz, which does not affect the signal bandwidth. OUTPUT PHASE REVERSAL Output phase reversal occurs in some amplifiers when the input common-mode voltage range is exceeded. As the common-mode voltage is moved outside the input voltage range, the outputs of these amplifiers can suddenly jump in the opposite direction to the supply rail. This is the result of the differential input pair shutting down that causes a radical shifting of internal voltages that results in the erratic output behavior. The AD8597/AD8599 amplifiers are carefully designed to prevent any output phase reversal if both inputs are maintained within the specified input voltage range. If one or both inputs exceed the input voltage range but remain within the supply rails, the op amp specifications, such as CMRR, are not guaranteed, but the output remains close to the correct value. NOISE AND SOURCE IMPEDANCE CONSIDERATIONS The AD8597/AD8599 ultralow voltage noise of 1.1 nV/√Hz is achieved with special input transistors running at high collector current. Therefore, it is important to consider the total input- referred noise (eN total), which includes contributions from voltage noise (eN), current noise (iN), and resistor noise (√4 kTRS). eN total = [eN2 + 4 kTRS + (iN × RS)2]1/2 (1) where RS is the total input source resistance. This equation is plotted for the AD8597/AD8599 in Figure 58. Because optimum dc performance is obtained with matched source resistances, this case is considered even though it is clear from Equation 1 that eliminating the balancing source resistance lowers the total noise by reducing the total RS by a factor of 2. At a very low source resistance (RS < 50 Ω), the voltage noise of the amplifier dominates. As source resistance increases, the Johnson noise of RS dominates until a higher resistance of RS > 2 kΩ is achieved; the current noise component is larger than the resistor noise. 100 1 10 0.1 10 100 1k 10k SOURCE RESISTANCE (Ω) TOTAL NOISE RESISTOR NOISE ONLY Figure 58. Noise vs. Source Resistance |
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