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OP176GS датащи(PDF) 15 Page - Analog Devices |
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OP176GS датащи(HTML) 15 Page - Analog Devices |
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15 / 21 page ![]() OP176 REV. 0 –15– High Pass Sections Figure 44a illustrates the high-pass form of a 2-pole SK filter using an OP176. For simplicity and practicality, capacitors C1 and C2 are set equal (“C”), and resistors R2 and R1 are adjusted to a ratio, N, which provides the filter damping coefficient, α, as per the design expressions. This high pass design is begun with selection of standard capacitor values for C1 and C2 and a calculation of N. The values for R1 and R2 are then determined from the following expressions: R1 = 1 2 π× FREQ × C × N and R2 = N × R1 Figures 44a. Two-Pole Unity Gain HP/LP Active Filters In this examples, circuit α (or 1/Q) is set equal to √2, providing a Butterworth (maximally flat) characteristic. The filter corner frequency is normalized to 1 kHz, with resistor values shown in both rounded and (exact) form. Various other 2-pole response shapes are possible with appropriate selection of α, and fre- quency can be easily scaled, using inversely proportional R or C values for a given α. The 22 V/µs slew rate of the OP176 will support 20 V p-p outputs above 100 kHz with low distortion. The frequency response resulting with this filter is shown as the dotted HP portion of Figure 45. +VS R1 11k (11.254k) C1 0.01µF 7 4 6 3 2 OUT IN OP176 C2 0.01µF –VS R2 22k (22.508k) GIVEN: α, FREQ SET C1 = C2 = C α = = 2 N 1 Q N = = 4 α2 R2 R1 R1 = 1 R2 = N x R1 ZCOMP ZCOMP (HIGH PASS) IN (–) R2 OUTPUT C1 C2 R1 1 kHz BW SHOWN 2 π FREQ x C x N Low Pass Sections In the LP SK arrangement of Figure 44b, the R and C elements are interchanged where the resistors are made equal. Here, the ratio of C2/C1 (“M”) is used to set the filter α, as noted. Otherwise, this filter is similar to the HP section, and the resulting 1 kHz LP response is shown in Figure 45. The design begins with a choice of a standard capacitor value for C1 and a calculation of M. This then forces a value of “M × C1” for C2. Then, the value for R1 and R2 (“R”) is calculated according to the following equation: R = 1 2 π× FREQ × C1× M Figures 44b. Two-Pole Unity Gain HP/LP Active Filters Figure 45. Relative Frequency Response of 2-Pole, 1 kHz Butterworth LP (Left) and HP (Right) Active Filters +VS R1 11k (11.254k) C1 0.02µF 7 4 6 3 2 OUT IN OP176 C2 0.01µF –VS R2 11k (11.254k) GIVEN: α, FREQ α = = 2 M 1 Q M = = 4 α2 C2 C1 C2 = M x C1 ZCOMP IN (–) R2 OUTPUT C1 C2 R1 1 kHz BW SHOWN CHOOSE C1 R = 1 2 π FREQ x C1 x M ZCOMP (LOW PASS) 100 50k 10k 1k 20 10.000 –30.00 –70.00 –50.00 –10.00 –20.00 –40.00 –60.00 0.0 LP HP FREQUENCY – Hz |
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