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LTC1060CSW Datasheet(PDF) 16 Page - Linear Technology |
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LTC1060CSW Datasheet(HTML) 16 Page - Linear Technology |
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16 / 20 page ![]() 16 LTC1060 1060fb Modes 2, 2a, and 2b have a notch output which frequency, fn, can be tuned independently from the center frequency, f0. For all cases, however, fn<f0. These modes are useful when cascading second order functions to create an overall elliptic highpass, bandpass or notch response. The input amplifier and its feedback resistors (R2/R4) are now part of the resonant loop. Because of this, mode 2 and its derivatives are slower than mode 1’s. In mode 3 (Figure 11), a single resistor ratio (R2/R4) can tune the center frequency below or above the fCLK/100 (or fCLK/50) ratio. Mode 3 is a state variable configuration since it provides a highpass, bandpass, lowpass output through progressive integration; notches are obtained by summing the highpass and lowpass outputs (mode 3a, Figure 12). The notch frequency can be tuned below or above the center frequency through the resistor ratio (Rh/Ri). Because of this, modes 3 and 3a are the most versatile and useful modes for cascading second order sections to obtain high order elliptic filters. Figure 20 shows the two sections of an LTC1060 connected in mode 3a to obtain a clock tunable 4th order sharp elliptic bandpass filter. The first notch is created by summing directly the HP and LP outputs of the first section into the inverting input of the second section op amp. The indi- vidual Q’s are 29.6 and the filter maintains its shape and performance up to 20kHz center frequency (Figure 21). For this circuit an external op amp is required to obtain the 2nd notch. The dynamics of Figure 20 are excellent be- cause the amplitude response at each output pin does not exceed 0dB. The gain in the passband depends on the ratio of (Rg/Rh2) • (R22/Rh1)• (R21/R11). Any gain value can be obtained by acting on the (Rg/Rh2) ratio of the external op amp, meanwhile the remaining ratios are adjusted for optimum dynamics of the LTC1060 output nodes. The external op amp of Figure 20 is not always required. In Figure 22, one section of the LTC1060 in mode 3a is cascaded with the other section in mode 2b to obtain a 4th order, 1dB ripple, elliptic bandreject filter. This configura- tion is interesting because a 4th order function with two different notches is realized without requiring an external op amp. The clock-to-center frequency ratio is adjusted to 200:1; this is done in order to better approximate a linear R,C notch filter. The amplitude response of the filter is shown in Figure 23 with up to 1MHz clock frequency. The 0dB bandwidth to the stop bandwidth ratio is 9/1. When the filter is centered at 1kHz, it should theoretically have a 44dB rejection with a 50Hz stop bandwidth. For a more narrow filter than the above, the unused BP output of the Figure 19. Cascading the Two Sections of the LTC1060 Connected in Mode 1c to Obtain a Clock Tunable 4th Order 1dB Ripple Bandpass Chebyshev Filter with (Center Frequency)/(Ripple Bw) = 20/1. 0.9kHz –15dB –10dB –5dB 0dB 1.1kHz –25dB –20dB 1kHz 50Hz fCLK = 40kHz 18kHz –15dB –10dB –5dB 0dB 22kHz TLC1060 • CMO01b –25dB –20dB 20kHz 19kHz 21kHz 1kHz fCLK = 800kHz LTC1060 • CM01 VIN R31 R21 R52 R32 1 2 3 4 5 6 7 8 9 10 20 19 18 17 16 15 14 13 12 11 V+ = 5V VOUT T2L OR CMOS CLK IN R51 R22 R62 R12 LPA BPA NA INVA S1A SA/B VA + VD + LSh CLKA LPB BPB NB INVB S1B AGND VA – VD – 50/100 CLKB LTC1060 R61 R11 5V PRECISE RESISTOR VALUES R11 = 149.21k R21 = 4.99k R31 = 149.12k R51 = 2.55k R61 = 2.49k R12 = 45.14k R22 = 5.00k R32 = 142.64k R5 = 2.49k R62 = 4.29k V– = –5V COMM E TS ON THE M ODES OF OPERATIO |
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