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AD8307-EB Datasheet(PDF) 12 Page - Analog Devices |
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AD8307-EB Datasheet(HTML) 12 Page - Analog Devices |
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12 / 20 page ![]() AD8307 –12– REV. A In most applications, the signal will be single-sided, and may be applied to either Pin 1 or Pin 8, with the other pin ac-coupled to ground. Under these conditions, the largest input signal that can be handled by the AD8307 is +10 dBm (sine amplitude of ±1V) when operating from a 3 V supply; a +16 dBm may be handled using a 5 V supply. The full 16 dBm may be achieved for sup- plies down to 2.7 V, using a fully balanced drive. For frequencies above about 10 MHz, this is most easily achieved using a matching network (see below). Using such a network, having an inductor at the input, the input transient noted above is eliminated. Occa- sionally, it may be desirable to use the dc-coupled potential of the AD8307. The main challenge here is to present signals to the log amp at the elevated common-mode input level, requiring the use of low noise, low offset buffer amplifiers. Using dual supplies of ±3 V, the input pins may operate at ground potential. Offset Interface The input-referred dc offsets in the signal path are nulled via the interface associated with Pin 3, shown in Figure 28. Q1 and Q2 are the first stage input transistors, with their corresponding load resistors (125 Ω). Q3 and Q4 generate small currents, which can introduce a dc offset into the signal path. When the voltage on OFS is at about 1.5 V, these currents are equal, and nominally 16 µA. When OFS is taken to ground, Q4 is off and the effect of the current in Q3 is to generate an offset voltage of 16 µA × 125 Ω = 2 mV. Since the first stage gain is ×5, this is equivalent to a input offset (INP to INM) of 400 µV. When OFS is taken to its most positive value, the input-referred offset is reversed, to –400 µV. If true dc-coupling is needed, down to very small inputs, this automatic loop must be disabled, and the residual offset eliminated using a manual adjustment, as explained in the next section. In normal operation, however, using an ac-coupled input signal, the OFS pin should be left open. Any residual input-offset volt- age is then automatically nulled by the action of the feedback loop. The gm cell, which is gated off when the chip is disabled, converts any output offset (sensed at a point near the end of the cascade of amplifiers) to a current. This is integrated by the on- chip capacitor CHP, plus any added external capacitance COFS, so as to generate an error voltage, which is applied back to the input stage in the polarity needed to null the output offset. From a small-signal perspective, this feedback alters the response of the amplifier, which, rather than behaving as a fully dc-coupled system, now exhibits a zero in its ac transfer function, resulting in a closed-loop high-pass corner at about 700 kHz. 48k 125 MAIN GAIN STAGES Q2 Q1 Q3 16 A AT BALANCE Q4 gm S AVERAGE ERROR CURRENT OFS TO LAST DETECTOR COFS CHP COM VPS 36k INPUT STAGE BIAS, 1.2V Figure 28. Offset Interface and Offset-Nulling Path The offset feedback is limited to a range ±400 µV; signals larger than this override the offset control loop, which only impacts performance for very small inputs. An external capacitor re- duces the high pass corner to arbitrarily low frequencies; using 1 µF this corner is below 10 Hz. All ADI log amps use an offset- nulling loop; the AD8307 differs in using this single-sided form. Output Interface The outputs from the nine detectors are differential currents, having an average value that is dependent on the signal input level, plus a fluctuation at twice the input frequency. The cur- rents are summed at nodes LGP and LGN in Figure 29. Fur- ther currents are added at these nodes, to position the intercept, by slightly raising the output for zero input, and to provide temperature compensation. Since the AD8307 is not laser- trimmed, there is a small uncertainty in both the log slope and the log intercept. These scaling parameters may be adjusted (see below). For zero-signal conditions, all the detector output currents are equal. For a finite input, of either polarity, their difference is converted by the output interface to a single-sided unipolar current nominally scaled 2 µA/dB (40 µA/decade), at the output pin OUT. An on-chip 12.5 k Ω resistor, R1, converts this cur- rent to a voltage of 25 mV/dB. C1 and C2 are effectively in shunt with R1 and form a low-pass filter pole, with a corner frequency of about 5 MHz. The pulse response settles to within 1% of the final value within 300 ns. This integral low-pass filter provides adequate smoothing in many IF applications. At 10.7 MHz, the 2f ripple is 12.5 mV in amplitude, equivalent to ±0.5 dB, and only 0.5 mV (±0.02 dB) at f = 50 MHz. A filter capacitor CFLT added from OUT to ground will lower this cor- ner frequency. Using 1 µF, the ripple is maintained to less than ±0.5 dB down to input frequencies of 100 Hz. Note that C OFS (above) should also be increased in low frequency applications, and will typically be made equal to CFLT. It may be desirable to increase the speed of the output response, with the penalty of increased ripple. One way to do this is sim- ply by connecting a shunt load resistor from OUT to ground, which raises the low pass corner frequency. This also alters the logarithmic slope, for example to 7.5 mV/dB using a 5.36 k Ω resistor, while reducing the 10%-90% rise time to 25 ns. The ripple amplitude for 50 MHz input remains 0.5 mV, but this is now equivalent to ±0.07 dB. If a negative supply is available, the output pin may be connected directly to the summing node of an external op amp connected as an inverting-mode transresistance stage. 1.25k 25mV/dB OUT 2 A/dB 0-220 A INT FROM ALL DETECTORS CFLT C2 1pF VPS BIAS 1.25k 400mV 8.25k 60k 60 A COM R1 12.5k C1 2.5pF 3pF LGP LGM 1.25k 1.25k Figure 29. Simplified Output Interface |
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