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ADA4922-1ACPZ-R2 数据表(PDF) 17 Page - Analog Devices |
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ADA4922-1ACPZ-R2 数据表(HTML) 17 Page - Analog Devices |
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17 / 20 page ![]() ADA4922-1 Rev. 0 | Page 17 of 20 Defining VIN as the voltage applied to the input pin, the equations that govern the two signal paths are given in Equation 12 and Equation 13. VOUT+ = +VIN (12) VOUT− = −VIN + 2(REF) (13) When the REF voltage is set to the midswing level of the input signal, the two output signals fall directly on top of each other with minimal offset. Setting the REF voltage elsewhere results in an offset between the two outputs. This effect is illustrated in the Theory of Operation section. The best use of the REF pin can be further illustrated by considering a single-supply example that uses a 10 V dc power supply and has an input signal that varies between 2 V and 7 V. This is a case where the midswing level of the input signal is not at midsupply but is at 4.5 V. By setting the REF input to 4.5 V and neglecting offsets, Equation 12 and Equation 13 are used to calculate the results. When the input signal is at its midpoint of 4.5 V, VOUT+ is at 4.5 V, as is VOUT−. This can be considered as a type of baseline state where the differential output voltage is zero. When the input increases to 7 V, VOUT+ tracks the input to 7 V and VOUT− decreases to 2 V. This can be viewed as a positive peak signal where the differential output voltage equals 5 V. When the input signal decreases to 2 V, VOUT+ again tracks to 2 V, and VOUT− increases to 7 V. This can be viewed as a negative peak signal where the differential output voltage equals −5 V. The resulting differential output voltage is 10 V p-p. The previous discussion exposes how the single-ended-to- differential gain of 2 is achieved. INTERNAL FEEDBACK NETWORK POWER DISSIPATION While traditional op amps do not have on-chip feedback elements, the ADA4922-1 contains two on-chip 600 Ω resistors that comprise an internal feedback loop. The power dissipated in these resistors must be included in the overall power dissipation calculations for the device. Under certain circumstances, the power dissipated in these resistors could be considerably more than the device’s quiescent current. For example, on ±12 V supplies with the REF pin tied to ground and OUT− at 9 V dc, each 600 Ω resistor carries 15 mA and dissipates 135 mW. This is a significant amount of power and must therefore be included in the overall device power dissipation calculations. For ac signals, rms analysis is required. DISABLE FEATURE The ADA4922-1 includes a disable feature that can be asserted to minimize power consumption in a device that is not needed at a particular time. When asserted, the disable feature does not place the device output in a high impedance or three-state condition. The disable feature is asserted by applying a control voltage to the DIS pin and is active low. See the Specifications section for the high and low level voltage specifications. DRIVING A DIFFERENTIAL INPUT ADC The ADA4922-1 provides the single-ended-to-differential conversion that is required to drive most high resolution ADCs. Figure 50 shows how the ADA4922-1 simplifies ADC driving. VIN ±10V 0.1 μF –12V HIGH VOLTAGE HIGH RESOLUTION ADC VS– VS+ DIS R R IN 8 OUT+ ADA4922-1 OUT– 4 5 6 73 REF 2 0.1 μF –12V 0.1 μF +12V 0.1 μF +12V R R C C Figure 50. Driving a Differential Input ADC For example, consider the case where the input signal bandwidth is 100 KHz and R = 41.2 Ω and C = 3.9 nF, as is shown in Figure 50, to form a single-pole filter with −3 dB bandwidth of approximately 1 MHz. The ADA4922-1 output noise (with zero source resistance) integrated over this bandwidth appears at the ADC input and is calculated as () () rms μV 15 MHz 1 2 π Hz nV/ 12 ) ( , = ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ = rms V dm ADC n, (14) The rms value of a 20 V p-p signal at the ADC input is 7 V rms, yielding a SNR of 113 dB at the ADC input. |
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