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OP484FSZ Datasheet(PDF) 15 Page - Analog Devices |
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OP484FSZ Datasheet(HTML) 15 Page - Analog Devices |
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15 / 24 page ![]() OP184/OP284/OP484 Rev. D | Page 15 of 24 5 4 –5 –4 –3 –2 –1 0 1 2 3 –5 –4 –3 –2 –1 0 12345 INPUT VOLTAGE (V) OUTPUT PHASE REVERSAL Some operational amplifiers designed for single-supply operation exhibit an output voltage phase reversal when their inputs are driven beyond their useful common-mode range. Typically, for single-supply bipolar op amps, the negative supply determines the lower limit of their common-mode range. With these devices, external clamping diodes, with the anode connected to ground and the cathode to the inputs, prevent input signal excursions from exceeding the device’s negative supply (that is, GND), preventing a condition that causes the output voltage to change phase. JFET-input amplifiers can also exhibit phase reversal, and, if so, a series input resistor is usually required to prevent it. The OP284 is free from reasonable input voltage range restrictions, provided that input voltages no greater than the supply voltages are applied. Although device output does not change phase, large currents can flow through the input protection diodes as shown in Figure 46. Input Overvoltage I-V Characteristics of the OP284 As shown in Figure 46, internal p-n junctions to the OP284 energize and permit current flow from the inputs to the supplies when the input is 1.8 V more positive and 0.6 V more negative than the respective supply rails. As illustrated in the simplified equivalent circuit shown in Figure 46. Therefore, the technique recommended in the Input Overvoltage Protection section should be applied to those applications where the likelihood of input voltages exceeding the supply voltages is high. Figure 44, the OP284 does not have any internal current limiting resistors; thus, fault currents can quickly rise to damaging levels. DESIGNING LOW NOISE CIRCUITS IN SINGLE- SUPPLY APPLICATIONS This input current is not inherently damaging to the device, provided that it is limited to 5 mA or less. For the OP284, once the input exceeds the negative supply by 0.6 V, the input current quickly exceeds 5 mA. If this condition continues to exist, an external series resistor should be added at the expense of additional thermal noise. In single-supply applications, devices like the OP284 extend the dynamic range of the application through the use of rail-to-rail operation. In fact, the OPx84 family is the first of its kind to combine single-supply, rail-to-rail operation and low noise in one device. It is the first device in the industry to exhibit an input noise voltage spectral density of less than 4 nV/√Hz at 1 kHz. It was also designed specifically for low-noise, single- supply applications, and as such, some discussion on circuit noise concepts in single-supply applications is appropriate. Figure 47 illustrates a typical noninverting configuration for an overvoltage-protected amplifier where the series resistance, R , is chosen such that S () mA 5 SUPPLY MAX IN S V V R − = Referring to the op amp noise model circuit configuration illustrated in For example, a 1 kΩ resistor protects the OP284 against input signals up to 5 V above and below the supplies. For other configurations where both inputs are used, then each input should be protected against abuse with a series resistor. Again, to ensure optimum dc and ac performance, it is recommended to balance source impedance levels. Figure 48, the expression for an amplifier’s total equivalent input noise voltage for a source resistance level, RS, is given by ( ) ( ) [ ] ()2 2 2 2 nOA nOA nR nT e R i e e + × + = Hz V , units in where: R1 R2 VIN VOUT 1/2 OP284 Figure 47. Resistance in Series with Input Limits Overvoltage Currents to Safe Values RS = 2R is the effective, or equivalent, circuit source resistance. (enOA)2 is the op amp equivalent input noise voltage spectral power (1 Hz BW). (inOA)2 is the op amp equivalent input noise current spectral power (1 Hz BW). (enR)2 is the source resistance thermal noise voltage power (4 kTR). k = Boltzmann’s constant = 1.38 × 10–23 J/K. T is the ambient temperature in Kelvins of the circuit = 273.15 + T (°C). A |
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