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OP275 датащи(PDF) 8 Page - Analog Devices |
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OP275 датащи(HTML) 8 Page - Analog Devices |
8 / 12 page OP275 REV. A –8– Noise Testing For audio applications the noise density is usually the most im- portant noise parameter. For characterization the OP275 is tested using an Audio Precision, System One. The input signal to the Audio Precision must be amplified enough to measure it accurately. For the OP275 the noise is gained by approximately 1020 using the circuit shown in Figure 7. Any readings on the Audio Precision must then be divided by the gain. In imple- menting this test fixture, good supply bypassing is essential. A B OP275 909 Ω 100 Ω OP37 909 Ω 100 Ω 909 Ω 100 Ω OP37 4.42k Ω 490 Ω OUTPUT Figure 7. Noise Test Fixture Input Overcurrent Protection The maximum input differential voltage that can be applied to the OP275 is determined by a pair of internal Zener diodes con- nected across its inputs. They limit the maximum differential in- put voltage to ±7.5 V. This is to prevent emitter-base junction breakdown from occurring in the input stage of the OP275 when very large differential voltages are applied. However, in or- der to preserve the OP275’s low input noise voltage, internal re- sistances in series with the inputs were not used to limit the current in the clamp diodes. In small signal applications, this is not an issue; however, in applications where large differential voltages can be inadvertently applied to the device, large tran- sient currents can flow through these diodes. Although these di- odes have been designed to carry a current of ±5 mA, external resistors as shown in Figure 8 should be used in the event that the OP275’s differential voltage were to exceed ±7.5 V. OP275 1.4k Ω 1.4k Ω – + 2 3 6 Figure 8. Input Overcurrent Protection Output Voltage Phase Reversal Since the OP275’s input stage combines bipolar transistors for low noise and p-channel JFETs for high speed performance, the output voltage of the OP275 may exhibit phase reversal if either of its inputs exceed its negative common-mode input voltage. This might occur in very severe industrial applications where a sensor, or system, fault might apply very large voltages on the inputs of the OP275. Even though the input voltage range of the OP275 is ±10.5 V, an input voltage of approximately –13.5 V will cause output voltage phase reversal. In inverting amplifier configurations, the OP275’s internal 7.5 V input clamping di- odes will prevent phase reversal; however, they will not prevent this effect from occurring in noninverting applications. For these applications, the fix is a simple one and is illustrated in Figure 9. A 3.92 k Ω resistor in series with the noninverting input of the OP275 cures the problem. RFB* VIN RS 3.92k Ω VOUT RL 2k Ω *RFB IS OPTIONAL Figure 9. Output Voltage Phase Reversal Fix Overload, or Overdrive, Recovery Overload, or overdrive, recovery time of an operational amplifier is the time required for the output voltage to recover to a rated output voltage from a saturated condition. This recovery time is important in applications where the amplifier must recover quickly after a large abnormal transient event. The circuit shown in Figure 10 was used to evaluate the OP275’s overload recovery time. The OP275 takes approximately 1.2 µs to recover to VOUT = +10 V and approximately 1.5 µs to recover to V OUT = –10 V. VIN RS 909 Ω VOUT RL 2.43k Ω A1 = 1/2 OP275 R2 10k Ω R1 1k Ω 4V p-p @100Hz 1 2 3 A1 Figure 10. Overload Recovery Time Test Circuit Measuring Settling Time The design of OP275 combines high slew rate and wide gain- bandwidth product to produce a fast-settling (tS < 1 µs) ampli- fier for 8- and 12-bit applications. The test circuit designed to measure the settling time of the OP275 is shown in Figure 11. This test method has advantages over false-sum node tech- niques in that the actual output of the amplifier is measured, in- stead of an error voltage at the sum node. Common-mode settling effects are exercised in this circuit in addition to the slew rate and bandwidth effects measured by the false-sum-node method. Of course, a reasonably flat-top pulse is required as the stimulus. The output waveform of the OP275 under test is clamped by Schottky diodes and buffered by the JFET source follower. The signal is amplified by a factor of ten by the OP260 and then Schottky-clamped at the output to prevent overloading the oscilloscope’s input amplifier. The OP41 is configured as a fast integrator which provides overall dc offset nulling. High Speed Operation As with most high speed amplifiers, care should be taken with supply decoupling, lead dress, and component placement. Rec- ommended circuit configurations for inverting and noninverting applications are shown in Figures 12 and Figure 13. |
Аналогичный номер детали - OP275 |
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Аналогичное описание - OP275 |
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