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AFE8221RFP Datasheet(PDF) 21 Page - Texas Instruments |
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AFE8221RFP Datasheet(HTML) 21 Page - Texas Instruments |
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21 / 48 page ![]() www.ti.com GAIN= å NCOEFF n=1 2h n 2 1 - 15 (9) GAIN= å NCOEFF n=1 h n 2 1 - 15 (10) SECOND FIR FILTERS ddc0_fir2a_ncoeff 4 ddc0_cic_dec_rate £ ´ (11) ddc0_fir2b_ncoeff 4 ddc0_cic_dec_rate £ ´ (12) AFE8221 SBAS394A – APRIL 2007 – REVISED MARCH 2008 For EVEN mode the, dc gain is shown by Equation 9: weights must add up to (215 – 1) to achieve unity gain through the filter. With longer filters (and therefore, smaller coefficients), frequency response errors may be introduced as a result of coefficient truncation. A Shift parameter has been added to the second FIR filter to alleviate this problem. The total of while for ARBITRARY mode the gain is shown by all filter tap weights must add up to (215+ddc0_fir2a_shift Equation 10: – 1) to achieve unity gain through FIR2A (similarly for ddc0_fir2b_shift and FIR2B). Note that shift values for FIR2A and FIR2B can be set separately. Extended-Length Filter Mode If FIR2A or FIR2B cannot provide enough filter taps to achieve the desired frequency response, setting The first FIR filter is followed by two parallel second control bit ddc0_interleave puts the two filters into an FIR filters, FIR2A and FIR2B. Duplicate filters allow interleaved mode that doubles the length of the filter the output of two I and Q output streams with that can be realized. However, there are several different bandwidths. For example, the bandwidth of limitations: FIR2A may be set wide to accommodate reception of 1. Only odd symmetrical filters may be realized; digital broadcasts, while FIR2B may be set narrower to receive an analog broadcast sharing the same 2. The filter length M must be such that (M + 1)/4 is band. Coefficients for FIR2A are stored in memory an integer; and bank 1 (MEM = 1) and coefficients for FIR2B are 3. Only one filter can be realized (in ddc_interleave stored in memory bank 2 (MEM = 2). mode the A and B outputs are identical: IB = IA and QB = QA). The operation of the second FIR filter is similar to the first FIR filter with several notable exceptions. First, In addition to setting the ddc0_interleave bit, FIR2A the depths of the coefficient and data memories are must be set to EVEN mode and FIR2A must be set to doubled to 128. This size increase allows for filters up ODD mode. ddc0_fir2a_ncoeff and ddc0_fir2b_ncoeff to 126 taps to be realized without running out of data are both set to (M + 1)/4. ddc0_fir2a_shift and memory. It also allows longer sets of filter coefficients ddc0_fir2b_shift should be identical. There are no to be stored in coefficient memory. restrictions on ddc0_fir2a_base_addr or ddc0_fir2b_base_addr. Second, because of the additional decimation by two from the first FIR filter, twice as many MCLK cycles The M-tap filter has (M + 1)/2 unique coefficients. The are available to process coefficients, increasing the first, third, fifth, etc. coefficients are loaded into the maximum allowable value of NCOEFF, as shown in FIR2A coefficient memory; the second, fourth, sixth, Equation 11 and Equation 12. etc. coefficients are loaded into the FIR2B memory. The center coefficients of the filter end up as the last coefficient loaded into FIR2B. Third, in the first FIR filter the total of all the filter tap Copyright © 2007–2008, Texas Instruments Incorporated Submit Documentation Feedback 21 Product Folder Link(s): AFE8221 |
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