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ADL5511ACPZ-R7 数据表(PDF) 17 Page - Analog Devices |
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ADL5511ACPZ-R7 数据表(HTML) 17 Page - Analog Devices |
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17 / 29 page ![]() Data Sheet ADL5511 Rev. C | Page 17 of 29 CIRCUIT DESCRIPTION The ADL5511 employs a proprietary rectification technique to strip off the carrier of an input signal to reveal the true envelope. In this first detection stage, the carrier frequency is doubled and an on-chip two-pole passive low-pass filter accurately preserves the envelope and filters out the carrier. The poles of this filter, as defined by the on-chip RC filters (0.4 pF, 400 Ω, 0.8 pF, 250 Ω) values allow some carrier leakthrough for common RF frequencies. This is to ensure that maximum envelope bandwidth can be maintained. For more details, see the Basic Connections section. Figure 48. Block Diagram The extracted envelope is further processed in two parallel channels, one computing the rms value of the envelope and the other transferring the envelope with appropriate scaling to the envelope output. ENVELOPE PROPAGATION DELAY The delay specified in this data sheet is with no external capacitor at the FLT2 and FLT3 pins. The delay through the ADL5511, although very small, depends upon a number of factors, notable of which are internal filter component values and op amp compensation capacitors. The delay will vary from part to part by approximately ±15% due to process variations. In addition, the choice of external FLT2 and FLT3 values, as well as load on the VNEV pin will increase the delay. In this case, the delay variation will be dominated by the part-to-part tolerance of the external capacitors. RMS CIRCUIT DESCRIPTION The rms processing is done using a proprietary translinear technique. This method is a mathematically accurate rms computing approach and achieves unprecedented rms accuracies for complex modulation signals irrespective of the crest factor of the input signal. An integrating filter capacitor does the square-domain averaging. The VRMS output can be expressed as T1 T2 dt V A VRMS T2 T1 IN − × × = ∫ 2 (1) Note that A is a scaling parameter that is decided on by the on- chip resistor ratio, and there are no other scaling parameters involved in this computation, which means that the rms output is inherently free from any sources of error due to temperature, supply, and process variation. RMS FILTERING The on-chip rms filtering corner is internally set by a 400 Ω resistor and a 20 pF capacitor, yielding a corner frequency of approximately 20 MHz. Whereas this filters out all carrier frequencies, most of the modulation envelope is not filtered. For adequate rms filtering, connect an external filter capacitor between FLT4 (Pin 14) and VPOS (Pin 15). This capacitance acts on the internal 400 Ω resistor (see Figure 48) to yield a new corner frequency for the rms filter given by pF 20 ) 400 π 2 ( 1 − Ω × × = RMS FLT4 f C (2) For example, a supply-referenced 0.1 µF capacitor on FLT4 reduces the corner frequency of the rms averaging circuit to approximately 4 kHz. RMS filtering has a direct impact on rms accuracy. For most accurate detection, the rms filter corner should be low enough to filter out most of the modulation content. This will corre- spond to a corner frequency that is significantly lower than the bandwidth of the signal being measured. See the Choosing a Value for the RMS Averaging Capacitor (CFLT4) section for more details and filtering options. RFIN ENBL RMS 400Ω 20pF ENVELOPE VRMS VENV EREF VPOS VPOS VPOS 400Ω FLT1 FLT2 FLT3 COMM FLT4 0.8pF 0.4pF 10kΩ 5pF 250Ω 250Ω 100 Ω ADL5511 BIAS AND POWER- DOWN CONTROL G = 1.7 G = 1.5 NC 15 14 4 2 3 11 10 9 13 6 7 8 12 16 1 5 |
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