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AD605ARZ-R7 数据表(PDF) 15 Page - Analog Devices |
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AD605ARZ-R7 数据表(HTML) 15 Page - Analog Devices |
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15 / 20 page ![]() AD605 Rev. E | Page 15 of 20 35 30 25 20 15 10 5 0 –5 –10 –15 –20 40dB/V 30dB/V 20dB/V LINEAR-IN-dB RANGE OF AD605 1.0 0.5 1.5 2.0 2.5 3.0 GAIN CONTROL VOLTAGE Figure 37. Ideal Gain Curves vs. VREF Usable gain control voltage ranges are 0.1 V to 2.9 V for the 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 because below 50 mV the channel 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, and the response time to power the device on or off is less than 1 μs. FIXED GAIN AMPLIFIER AND INTERPOLATOR CIRCUITS—APPLYING AN ACTIVE FEEDBACK AMPLIFIER A typical X-amp architecture is powered by a dual polarity power supply. Because the AD605 operates from a single- supply, a supply-common equal to half the value of the supply voltage is required. An active feedback amplifier (AFA) is used to provide a differential input and to implement the feedback loop. The AFA in the AD605 is an op amp with two gm stages, one is used in the feedback path and the other is used as a highly linear differential input. A multisection distributed gm stage senses the voltages on the ladder network, one stage for each of the ladder nodes. Only a few of the stages are active at any time and are dependent on the gain control voltage. The AFA makes a differential input structure possible because 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 feedback. The output of G1 is some function of the voltages sensed on the attenuator taps that is applied to a high-gain amplifier (A0). Because of negative feedback, the differential input to the high gain amplifier is zero; this in turn implies that the differential input voltage to G2 times gm2 (the transconductance of G2) is equal to the differential input voltage to G1 times gm1 (the transconductance of G1). Therefore, the overall gain function of the AFA is R2 R2 R1 g g V V m m ATTEN OUT × × = 2 1 (7) where: VOUT is the output voltage. VATTEN is the effective voltage sensed on the attenuator. ( R1 + R2)/R2 = 42. gm1/gm2 = 1.25; the overall gain is therefore 52.5 (34.4 dB). The AFA has additional features: inverting the output signal by switching the positive and negative input to the ladder network; the possibility of using the −IN input as a second signal input; and 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 of 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 offsets contributed by the DSX (see the AC Coupling section). The gain range of the DSX is programmable by a resistor connected between Pin FBK and Pin OUT. The possible ranges are −14 dB to +34.4 dB when the pins are shorted together or 0 dB to +48.4 dB when FBK is left open. Note that for the higher gain range, the bandwidth of the amplifier is reduced by a factor of five to about 8 MHz because the gain increased by 14 dB. This is the case for any constant gain bandwidth product amplifier that includes the active feedback amplifier. |
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