Download e-book for kindle: KTeV beam systems design report by Coleman, R.; Childress, S.; Bocean, V.; Fermi National

By Coleman, R.; Childress, S.; Bocean, V.; Fermi National Accelerator Laboratory.; United States. Dept. of Energy. Office of Energy Research.; United States. Dept. of Energy. Office of Scientific and Technical Information

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11 Design an HP Chebyshev 3-dB “equal component” filter at a cutoff frequency of 200 Hz. 5 dB, f2 = 100 Hz, K = 1; (b) its frequency response. 19b. 19 (a) HP Chebyshev 3-dB, “equal component,” f2 = 200 Hz; (b) its frequency response. 8 HIGHER-ORDER FILTERS In the preceding sections of this chapter we have considered the realization of secondorder filters using Sallen–Key circuits. Many filtering applications, however, require filters of higher than second order, either to provide greater stopband attenuation and sharper cutoff at the edge of the passband in the low-pass or high-pass case, or to provide a broad passband with some special transmission characteristic in the bandpass case.

39). 9, are omitted from the transformation. After the normalized low-pass configuration is transformed into a high-pass filter, the circuit is frequency- and impedance-scaled in the same manner as in the design of low-pass filters. 9 Design a 100-Hz HP Butterworth with gain 10. 17b. 17 (a) HP Butterworth filter, with f2 = 100 Hz, K = 10; (b) frequency response. 5-dB filter must be designed with a gain of 1 at a cutoff frequency of 100 Hz. 18 b. 11 Design an HP Chebyshev 3-dB “equal component” filter at a cutoff frequency of 200 Hz.

2 shows the frequency response of the filter. 1 A first-order LP Butterworth filter must be designed with gain of 5 at a cutoff frequency of 1 kHz. 2 Frequency response of first-order LPF. 3 LP Butterworth filter, where f1 = 1 kHz and K = 5 (14 dB). 3 shows the designed filter with its frequency response. 4 shows the first-order high-pass filter with noninverting gain K. 4 First-order HPF with gain K. 10), we have: From this transfer function, we have: 1. For s << 1 ω2 ∴ ⎛ ω⎞ H ( jω ) = K ⎜ j ⎟ ⎝ ω2 ⎠ ∴ ⎛ ω⎞ A = 20 log H ( jω ) = 20 log K + 20 log ⎜ ⎟ dB ⎝ ω2 ⎠ Sallen–Key Filters 27 ω = 10 ω2 ω For =2 ω2 For ∴ slope = 20 dB / dec.

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KTeV beam systems design report by Coleman, R.; Childress, S.; Bocean, V.; Fermi National Accelerator Laboratory.; United States. Dept. of Energy. Office of Energy Research.; United States. Dept. of Energy. Office of Scientific and Technical Information


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