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AD607 数据表(PDF) 14 Page - Analog Devices |
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AD607 数据表(HTML) 14 Page - Analog Devices |
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14 / 24 page ![]() REV. 0 –14– AD607 Table I. AD607 Filter Termination Resistor Values for Common IFs Filter Filter Termination Resistor IF Impedance Values 1 for 24 dB of Mixer Gain R1 R2 R3 450 kHz 1500 Ω 174 Ω 1330 Ω 1500 Ω 455 kHz 1500 Ω 174 Ω 1330 Ω 1500 Ω 6.5 MHz 1000 Ω 215 Ω 787 Ω 1000 Ω 10.7 MHz 330 Ω 330 Ω 0 Ω 330 Ω NOTES 1Resistor values were calculated such that R1+ R2 = Z FILTER and R1 (R2 + ZFILTER) = 165 Ω. The maximum permissible signal level at MXOP is determined by both voltage and current limitations. Using a 3 V supply and VMID at 1.5 V, the maximum swing is about ±1.3 V. To attain a voltage swing of ±1 V in the standard IF filter load of 165 Ω load requires a peak drive current of about ±6 mA, which is well within the linear capability of the mixer. However, these upper limits for voltage and current should not be confused with issues related to the mixer gain, already discussed. In an operational system, the AGC voltage will determine the mixer gain, and hence the signal level at the IF input pin IFHI; it will always be less than ±56 mV (–15 dBm into 50 Ω), which is the limit of the IF amplifier’s linear range. IF Amplifier Most of the gain in the AD607 arises in the IF amplifier strip, which comprises four stages. The first three are fully differential and each has a gain span of 25 dB for the nominal AGC voltage range. Thus, in conjunction with the mixer’s variable gain, the total gain exceeds 90 dB. The final IF stage has a fixed gain of 20 dB, and it also provides differential to single-ended conversion. The IF input is differential, at IFHI (noninverting relative to the output IFOP) and IFLO (inverting). Figure 36 shows a simpli- fied schematic of the IF interface. The offset voltage of this stage would cause a large dc output error at high gain, so it is nulled by a low-pass feedback path from the IF output, also shown in Figure 25. Unlike the mixer output, the signal at IFOP is a low-impedance single-sided voltage, centered at VP/2 by the DC feedback loop. It may be loaded by a resistance as low as 50 Ω which will normally be connected to VMID. 10k Ω 10k Ω VMID AD607 IFHI IFLO OFFSET FEEDBACK LOOP IFOP Figure 36. Simplified Schematic of the IF Interface The mixer’s RF input port is differential, that is, pin RFLO is functionally identical to RFHI, and these nodes are internally biased; we will generally assume that RFLO is decoupled to ac ground. The RF port can be modeled as a parallel RC circuit as shown in Figure 34. RIN CIN C2 C1 C3 L1 RFHI RFLO AD607 C1, C2, L1: OPTIONAL MATCHING CIRCUIT C3: COUPLES RFLO TO AC GROUND Figure 34. Mixer Port Modeled as a Parallel RC Network; an Optional Matching Network Is also Shown The local oscillator (LO) input is internally biased at VP/2 via a nominal 1000 Ω resistor internally connected from pin LOIP to VMID. The LO interface includes a preamplifier which mini- mizes the drive requirements, thus simplifying the oscillator de- sign and reducing LO leakage from the RF port. Internally, this single-sided input is actually differential; the noninverting input is referenced to pin VMID. The LO requires a single-sided drive of ±50 mV, or –16 dBm in a 50 Ω system. The mixer’s output passes through both a low-pass filter and a buffer, which provides an internal differential to single-ended signal conversion with a bandwidth of approximately 45 MHz. Its output at pin MXOP is in the form of a single-ended current. This approach eliminates the 6 dB voltage loss of the usual se- ries termination by replacing it with shunt terminations at the both the input and the output of the filter. The nominal conver- sion gain is specified for operation into a total IF bandpass filter (BPF) load of 165 Ω, that is, a 330 Ω filter, doubly-terminated as shown in Figure 33. Note that these loads are connected to bias point VMID, which is always at the midpoint of the supply (that is, VP/2). The conversion gain is measured between the mixer input and the input of this filter, and varies between 1.5 dB and 26.5 dB for a 165 Ω load impedance. Using filters of higher impedance, the conversion gain can always be maintained at its specified value or made even higher; for filters of lower impedance, of say ZO, the conversion gain will be lowered by 10 log10(165/ZO). Thus, the use of a 50 Ω filter will result in a conversion gain that is 5.2 dB lower. Figure 35 shows filter matching networks and Table I lists resistor values. IFLO BPF MXOP VMID IFHI 10 11 8 9 1nF 100nF R3 100nF R1 R2 Figure 35. Suggested IF Filter Matching Network. The Values of R1 and R2 Are Selected to Keep the Impedance at Pin MXOP at 165 Ω |
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