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AD8138ARZ-R7 Datasheet(PDF) 17 Page - Analog Devices |
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AD8138ARZ-R7 Datasheet(HTML) 17 Page - Analog Devices |
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17 / 24 page ![]() AD8138 Rev. F | Page 17 of 24 THEORY OF OPERATION The AD8138 differs from conventional op amps in that it has two outputs whose voltages move in opposite directions. Like an op amp, it relies on high open-loop gain and negative feedback to force these outputs to the desired voltages. The AD8138 behaves much like a standard voltage feedback op amp and makes it easy to perform single-ended-to-differential conversion, common-mode level-shifting, and amplification of differential signals. Also like an op amp, the AD8138 has high input impedance and low output impedance. Previous differential drivers, both discrete and integrated designs, have been based on using two independent amplifiers and two independent feedback loops, one to control each of the outputs. When these circuits are driven from a single-ended source, the resulting outputs are typically not well balanced. Achieving a balanced output has typically required exceptional matching of the amplifiers and feedback networks. DC common-mode level-shifting has also been difficult with previous differential drivers. Level-shifting has required the use of a third amplifier and feedback loop to control the output common-mode level. Sometimes the third amplifier has also been used to attempt to correct an inherently unbalanced circuit. Excellent performance over a wide frequency range has proven difficult with this approach. The AD8138 uses two feedback loops to separately control the differential and common-mode output voltages. The differential feedback, set with external resistors, controls only the differential output voltage. The common-mode feedback controls only the common-mode output voltage. This architecture makes it easy to arbitrarily set the output common-mode level. It is forced, by internal common-mode feedback, to be equal to the voltage applied to the VOCM input, without affecting the differential output voltage. The AD8138 architecture results in outputs that are very highly balanced over a wide frequency range without requiring tightly matched external components. The common-mode feedback loop forces the signal component of the output common-mode voltage to be zeroed. The result is nearly perfectly balanced differential outputs of identical amplitude and exactly 180° apart in phase. ANALYZING AN APPLICATION CIRCUIT The AD8138 uses high open-loop gain and negative feedback to force its differential and common-mode output voltages in such a way as to minimize the differential and common-mode error voltages. The differential error voltage is defined as the voltage between the differential inputs labeled +IN and −IN in Figure 42. For most purposes, this voltage can be assumed to be zero. Similarly, the difference between the actual output common- mode voltage and the voltage applied to VOCM can also be assumed to be zero. Starting from these two assumptions, any application circuit can be analyzed. SETTING THE CLOSED-LOOP GAIN Neglecting the capacitors CF, the differential-mode gain of the circuit in Figure 42 can be determined to be described by S G S F dm OUT dm OUT R R V V = , , This assumes the input resistors, RGS, and feedback resistors, RFS, on each side are equal. ESTIMATING THE OUTPUT NOISE VOLTAGE Similar to the case of a conventional op amp, the differential output errors (noise and offset voltages) can be estimated by multiplying the input referred terms, at +IN and −IN, by the circuit noise gain. The noise gain is defined as ⎟⎟ ⎠ ⎞ ⎜⎜ ⎝ ⎛ + = G F N R R G 1 To compute the total output referred noise for the circuit of Figure 42, consideration must also be given to the contribution of the Resistors RF and RG. Refer to Table 8 for the estimated output noise voltage densities at various closed-loop gains. Table 8. Gain RG (Ω) RF (Ω) Bandwidth −3 dB Output Noise AD8138 Only Output Noise AD8138 + RG, RF 1 499 499 320 MHz 10 nV/√Hz 11.6 nV/√Hz 2 499 1.0 k 180 MHz 15 nV/√Hz 18.2 nV/√Hz 5 499 2.49 k 70 MHz 30 nV/√Hz 37.9 nV/√Hz 10 499 4.99 k 30 MHz 55 nV/√Hz 70.8 nV/√Hz |
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