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AD604 数据表(PDF) 12 Page - Analog Devices |
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AD604 数据表(HTML) 12 Page - Analog Devices |
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12 / 20 page ![]() AD604 REV. 0 –12– Gain Control Interface The gain-control interface provides an input resistance of ap- proximately 2 M Ω at Pin VGN1 and gain scaling factors from 20 dB/V to 40 dB/V for VREF input voltages of 2.5 V to 1.25 V respectively. The gain scales linearly-in-dB for the center 40 dB of gain range, that is for VGN equal to 0.4 V to 2.4 V for the 20 dB/V scale, and 0.2 V to 1.2 V for the 40 dB/V scale. Figure 40 shows the ideal gain curves for a nominal preamplifier gain of 14 dB which are described by the following equations: G (20 dB/V) = 20 × VGN – 5, V REF = 2.500 V (4) G (30 dB/V) = 30 × VGN – 5, V REF = 1.666 V (5) G (40 dB/V) = 40 × VGN – 5, V REF = 1.250 V (6) GAIN CONTROL VOLTAGE – VGN 20 40 35 30 25 15 10 5 50 45 0 –5 LINEAR-IN-dB RANGE OF AD604 WITH PREAMPLIFIER SET TO 14dB 0.5 1.0 2.5 1.5 2.0 3.0 30dB/V 40dB/V 20dB/V Figure 40. Ideal Gain Curves vs. VREF. From these equations you can see that all gain curves intercept at the same –5 dB point; this intercept will be 6 dB higher (+1 dB) if the preamplifier gain is set to +20 dB or 14 dB, lower (–19 dB) if the preamplifier is not used at all. Outside of the central linear range, the gain starts to deviate from the ideal control law but still provides another 8.4 dB of range. For a given gain scaling you can calculate VREF as shown in Equation 7: V REF = 2.500 V × 20 dB / V Gain Scale (7) Usable gain control voltage ranges are 0.1 V to 2.9 V for 20 dB/V scale and 0.1 V to 1.45 V for the 40 dB/V scale. VGN voltages of less than 0.1 V are not used for gain control since below 50 mV the channel (preamp and DSX) is powered down. This can be used to conserve power and at the same time gate- off the signal. The supply current for a powered-down channel is 1.9 mA, the response time to power the device on-or-off, is less than 1 µs. Active Feedback Amplifier (Fixed Gain Amp) To achieve single supply operation and a fully differential input to the DSX, an active-feedback amplifier (AFA) is utilized. The AFA is basically an op amp with two gm stages; one of the active stages is used in the feedback path (therefore the name), while the other is used as a differential input. Note that the differential input is an open-loop gm stage that requires that it be highly linear over the expected input signal range. In this design, the gm stage that senses the voltages on the attenuator is a distrib- uted one; for example, there are as many gm stages as there are taps on the ladder network. Only a few of them are on at any one time, depending on the gain-control voltage. The AFA makes a differential input structure possible since one of its inputs (G1) is fully differential; this input is made up of a distributed gm stage. The second input (G2) is used for feed- back. The output of G1 will be some function of the voltages sensed on the attenuator taps which is applied to a high gain amplifier (A0). Because of negative feedback, the differential input to the high gain amplifier has to be zero; this in turn implies that the differential input voltage to G2 times gm2 (the transconductance of G2) has to be equal to the differential input voltage to G1 times gm1 (the transconductance of G1). There- fore the overall gain function of the AFA is: V OUT V ATTEN = gm1 gm2 × R1 + R2 R2 (8) where VOUT is the output voltage, VATTEN is the effective voltage sensed on the attenuator, (R1+R2)/R2 = 42, and gm1/gm2 = 1.25; the overall gain is thus 52.5 (34.4 dB). The AFA has additional features: (1) inverting the signal by switching the positive and negative input to the ladder network, (2) the possibility of using the DSX1 input as a second signal input, (3) fully differential high impedance inputs when both preamplifiers are used with one DSX (the other DSX could still be used alone), and (4) independent control of the DSX common- mode voltage. Under normal operating conditions it is best to connect a decoupling capacitor to pin VOCM in which case the common-mode voltage of the DSX is half the supply voltage; this allows for maximum signal swing. Nevertheless, the common-mode voltage can be shifted up or down by directly applying a voltage to VOCM. It can also be used as another signal input, the only limitation being the rather low slew-rate of the VOCM buffer. If the dc level of the output signal is not critical, another coupling capacitor is normally used at the output of the DSX; again this is done for level shifting and to eliminate any dc off- sets contributed by the DSX (see AC Coupling section). |
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