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AD620 Arkusz danych(PDF) 16 Page - Analog Devices |
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AD620 Arkusz danych(HTML) 16 Page - Analog Devices |
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16 / 20 page ![]() AD620 Rev. G | Page 16 of 20 Precision V-I Converter The AD620, along with another op amp and two resistors, makes a precision current source (Figure 42). The op amp buffers the reference terminal to maintain good CMR. The output voltage, VX, of the AD620 appears across R1, which converts it to a current. This current, less only the input bias current of the op amp, then flows out to the load. AD620 RG –VS VIN+ V IN– LOAD R1 I L Vx I = L R1 = IN+ [(V ) – (V )] G IN– R1 6 5 + V – X 4 2 1 8 3 7 +VS AD705 Figure 42. Precision Voltage-to-Current Converter (Operates on 1.8 mA, ±3 V) GAIN SELECTION The AD620’s gain is resistor-programmed by RG, or more precisely, by whatever impedance appears between Pins 1 and 8. The AD620 is designed to offer accurate gains using 0.1% to 1% resistors. Table 4 shows required values of RG for various gains. Note that for G = 1, the RG pins are unconnected (RG = ∞). For any arbitrary gain, RG can be calculated by using the formula: 1 4 . 49 − Ω = G k R G To minimize gain error, avoid high parasitic resistance in series with RG; to minimize gain drift, RG should have a low TC—less than 10 ppm/°C—for the best performance. Table 4. Required Values of Gain Resistors 1% Std Table Value of RG(Ω) Calculated Gain 0.1% Std Table Value of RG(Ω ) Calculated Gain 49.9 k 1.990 49.3 k 2.002 12.4 k 4.984 12.4 k 4.984 5.49 k 9.998 5.49 k 9.998 2.61 k 19.93 2.61 k 19.93 1.00 k 50.40 1.01 k 49.91 499 100.0 499 100.0 249 199.4 249 199.4 100 495.0 98.8 501.0 49.9 991.0 49.3 1,003.0 INPUT AND OUTPUT OFFSET VOLTAGE The low errors of the AD620 are attributed to two sources, input and output errors. The output error is divided by G when referred to the input. In practice, the input errors dominate at high gains, and the output errors dominate at low gains. The total VOS for a given gain is calculated as Total Error RTI = input error + (output error/G) Total Error RTO = (input error × G) + output error REFERENCE TERMINAL The reference terminal potential defines the zero output voltage and is especially useful when the load does not share a precise ground with the rest of the system. It provides a direct means of injecting a precise offset to the output, with an allowable range of 2 V within the supply voltages. Parasitic resistance should be kept to a minimum for optimum CMR. INPUT PROTECTION The AD620 features 400 Ω of series thin film resistance at its inputs and will safely withstand input overloads of up to ±15 V or ±60 mA for several hours. This is true for all gains and power on and off, which is particularly important since the signal source and amplifier may be powered separately. For longer time periods, the current should not exceed 6 mA (IIN ≤ VIN/400 Ω). For input overloads beyond the supplies, clamping the inputs to the supplies (using a low leakage diode such as an FD333) will reduce the required resistance, yielding lower noise. RF INTERFERENCE All instrumentation amplifiers rectify small out of band signals. The disturbance may appear as a small dc voltage offset. High frequency signals can be filtered with a low pass R-C network placed at the input of the instrumentation amplifier. Figure 43 demonstrates such a configuration. The filter limits the input signal according to the following relationship: ) 2 ( 2 1 C D DIFF C C R FilterFreq + π = C CM RC FilterFreq π = 2 1 where CD ≥10CC. CD affects the difference signal. CC affects the common-mode signal. Any mismatch in R × CC will degrade the AD620’s CMRR. To avoid inadvertently reducing CMRR-bandwidth performance, make sure that CC is at least one magnitude smaller than CD. The effect of mismatched CCs is reduced with a larger CD:CC ratio. |
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