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ADA4941-1YRZ-R7 データシート(PDF) 15 Page - Analog Devices |
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ADA4941-1YRZ-R7 データシート(HTML) 15 Page - Analog Devices |
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15 / 24 page ![]() ADA4941-1 Rev. C | Page 15 of 24 THEORY OF OPERATION The ADA4941-1 is a low power, single-ended input, differential output amplifier optimized for driving high resolution ADCs. Figure 47 illustrates how the ADA4941-1 is typically connected. The amplifier is composed of an uncommitted amplifier, A1, driving a precision inverter, A2. The negative input of A1 is brought out to Pin 1 (FB), allowing for user-programmable gain. The inverting op amp, A2, provides accurate inversion of the output of A1, VOP, producing the output signal VON. 1k Ω 1k Ω RG RF RF || RG 500 Ω A2 A1 REF IN VREF 2 8 4 5 FB OUT+ + – VOP 1 OUT– + – VON VIN VG Figure 47. Basic Connections (Power Supplies Not Shown) The voltage applied to the REF pin appears as the output common-mode voltage. Note that the voltage applied to the REF pin does not affect the voltage at the OUT+ pin. Because of this, a differential offset can exist between the outputs, while the desired output common-mode voltage is present. For example, when VOP = 3.5 V and VON = 1.5 V, the output common- mode voltage is equal to 2.5 V, just as it is when both outputs are at 2.5 V. In the first case, the differential voltage (or offset) is 2.0 V, and in the latter case, the differential voltage is 0 V. When calculating output voltages, both differential and common-mode voltages must be considered at the same time to avoid undesired differential offsets. BASIC OPERATION In Figure 47, RG and RF form the external gain-setting network. VG and VREF are externally applied voltages. VO, cm is defined as the output common-mode voltage and VO, dm is defined as the differential-mode output voltage. The following equations can be derived from Figure 47: − + = G F G F R R VG R R VIN VOP 1 (1) ) ( 2 1 VREF R R VG R R VIN VON G F G F + + + − = (2) ) ( 2 2 1 ) ( 2 , VREF R R VG R R VIN VON VOP dm V G F G F O − − + = − = (3) VREF VON VOP cm VO = + = 2 , (4) When RF = 0 and RG is removed, Equation 3 simplifies to the following: VO, dm = 2(VIN) − 2(VREF) (5) 1k Ω 1k Ω 4.99k Ω 1k Ω 825 Ω 500 Ω A2 A1 REF IN 2 8 4 5 FB +5V –5V VS+ VS– OUT+ + – VOP 1 3 6 OUT– + – VON VIN Figure 48. Dual Supply, G = 2.4, Single-Ended-to-Differential Amplifier Figure 48 shows an example of a dual-supply connection. In this example, VG and VREF are set to 0 V, and the external RF and RG network provides a noninverting gain of 1.2 in A1. This example takes full advantage of the rail-to-rail output stage. The gain equation is VOP − VON = 2.4(VIN) (6) The in-series, 825 Ω resistor combined with Pin 8 compensates for the voltage error generated by the input offset current of A1. The linear output range of both A1 and A2 extends to within 200 mV of each supply rail, which allows a peak-to-peak differential output voltage of 19.2 V on ±5 V supplies. 1k Ω 1k Ω 500 Ω A2 A1 REF IN 2 8 4 5 FB +5V VS+ VS– OUT+ + – VOP 1 3 6 OUT– + – VON +2.5V VIN Figure 49. Single +5V Supply, G=2 Single-Ended-to-Differential Amplifier Figure 49 shows a single 5 V supply connection with A1 used as a unity gain follower. The 2.5 V at the REF pin sets the output common-mode voltage to 2.5 V. The transfer function is then VOP − VON = 2(VIN) − 5 V (7) |
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