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11 сентября
1603490 Топик полностью
Nikolay_Po (Сегодня, 16:57, просмотров: 19) ответил IBAH на да я и на бих согласен, только 1)там написано эллиптический фильтр, 2) не качается
Вот полосовой Чебышева, 5-го порядка. При неравномерности в полосе пропускания 0.2дБ, на 30кГц подавление 73дБ: 
Filter kind:
1 Butterworth
2 Chebyshev
3 Elliptic
 ? 2
Filter shape:
1 low pass
2 band pass
3 high pass
4 band stop
 ? 2
Order of filter = 8.000000000E+000 ? 5.000000000E+000
Passband ripple, db = 5.000000000E-001 ? 2.000000000E-001
Sampling frequency = 1.000000000E+004 ? 1.000000000E+005
Passband edge = 2.000000000E+003 ? 1.000000000E+002
Other passband edge = 1.500000000E+003 ? 1.000000000E+004
s plane poles:
-4.614105755E-001 0.000000000E+000
-3.732889970E-001 6.473380467E-001
-1.425837092E-001 1.047414962E+000
s plane zeros:
adding zero at Nyquist frequency
adding zero at 0 Hz
adding zero at Nyquist frequency
adding zero at 0 Hz
adding zero at Nyquist frequency
adding zero at 0 Hz
adding zero at Nyquist frequency
adding zero at 0 Hz
adding zero at Nyquist frequency
adding zero at 0 Hz
order = 10
constant gain factor    5.4931133178501E-004
z plane Denominator      Numerator
 0  1.000000000E+000  5.493113318E-004
 1 -8.641816796E+000  0.000000000E+000
 2  3.394414307E+001 -2.746556659E-003
 3 -7.989448561E+001  0.000000000E+000
 4  1.248988043E+002  5.493113318E-003
 5 -1.355904822E+002  0.000000000E+000
 6  1.035567075E+002 -5.493113318E-003
 7 -5.495049438E+001  0.000000000E+000
 8  1.938759157E+001  2.746556659E-003
 9 -4.106339279E+000  0.000000000E+000
10  3.963717435E-001 -5.493113318E-004
poles and zeros with corresponding quadratic factors
pole     9.8564982120614E-001    0.0000000000000E+000
q. f.
z**2    0.0000000000000E+000
z**1   -9.8564982120614E-001
f0  5.00000000E+004  gain  5.0361E-001  DC gain  6.9686E+001

zero    -1.0000000000000E+000    0.0000000000000E+000
q. f.
z**2    0.0000000000000E+000
z**1    1.0000000000000E+000
f0  5.00000000E+004  gain  0.0000E+000  DC gain  2.0000E+000

pole     7.5247227773285E-001    0.0000000000000E+000
q. f.
z**2    0.0000000000000E+000
z**1   -7.5247227773285E-001
f0  5.00000000E+004  gain  5.7062E-001  DC gain  4.0400E+000

zero     1.0000000000000E+000    0.0000000000000E+000
q. f.
z**2    0.0000000000000E+000
z**1   -1.0000000000000E+000
f0  5.00000000E+004  gain  2.0000E+000  DC gain  0.0000E+000

pole     7.2673205028324E-001    3.2737077040383E-001
q. f.
z**2    6.3531109422368E-001
z**1   -1.4534641005665E+000
f0  6.73614483E+003  gain  6.4758E+000  DC gain  5.4991E+000

zero    -1.0000000000000E+000    0.0000000000000E+000
q. f.
z**2    0.0000000000000E+000
z**1    1.0000000000000E+000
f0  5.00000000E+004  gain  0.0000E+000  DC gain  2.0000E+000

zero     1.0000000000000E+000    0.0000000000000E+000
q. f.
z**2    0.0000000000000E+000
z**1   -1.0000000000000E+000
f0  5.00000000E+004  gain  2.0000E+000  DC gain  0.0000E+000

zero    -1.0000000000000E+000    0.0000000000000E+000
q. f.
z**2    0.0000000000000E+000
z**1    1.0000000000000E+000
f0  5.00000000E+004  gain  0.0000E+000  DC gain  2.0000E+000

pole     9.9588727005784E-001    7.3204701421030E-003
q. f.
z**2    9.9184504394635E-001
z**1   -1.9917745401157E+000
f0  1.16987942E+002  gain  1.6071E+004  DC gain  1.4184E+004

zero     1.0000000000000E+000    0.0000000000000E+000
q. f.
z**2    0.0000000000000E+000
z**1   -1.0000000000000E+000
f0  5.00000000E+004  gain  2.0000E+000  DC gain  0.0000E+000

pole     7.3003433518109E-001    5.6259531999152E-001
q. f.
z**2    8.4946362461966E-001
z**1   -1.4600686703622E+000
f0  1.04498240E+004  gain  1.0867E+001  DC gain  2.5681E+000

zero    -1.0000000000000E+000    0.0000000000000E+000
q. f.
z**2    0.0000000000000E+000
z**1    1.0000000000000E+000
f0  5.00000000E+004  gain  0.0000E+000  DC gain  2.0000E+000

zero     1.0000000000000E+000    0.0000000000000E+000
q. f.
z**2    0.0000000000000E+000
z**1   -1.0000000000000E+000
f0  5.00000000E+004  gain  2.0000E+000  DC gain  0.0000E+000

zero    -1.0000000000000E+000    0.0000000000000E+000
q. f.
z**2    0.0000000000000E+000
z**1    1.0000000000000E+000
f0  5.00000000E+004  gain  0.0000E+000  DC gain  2.0000E+000

pole     9.9919369290095E-001    5.8944957225326E-003
q. f.
z**2    9.9842278101286E-001
z**1   -1.9983873858019E+000
f0  9.38884278E+001  gain  1.0724E+005  DC gain  2.8252E+004

zero     1.0000000000000E+000    0.0000000000000E+000
q. f.
z**2    0.0000000000000E+000
z**1   -1.0000000000000E+000
f0  5.00000000E+004  gain  2.0000E+000  DC gain  0.0000E+000

       0.0     -999.99
    2500.0       -0.15
    5000.0       -0.08
    7500.0       -0.14
   10000.0       -0.20
   12500.0      -12.72
   15000.0      -25.39
   17500.0      -35.29
   20000.0      -43.79
   22500.0      -51.51
   25000.0      -58.84
   27500.0      -66.03
   30000.0      -73.30
   32500.0      -80.88
   35000.0      -89.04
   37500.0      -98.14
   40000.0     -108.76
   42500.0     -121.96
   45000.0     -140.06
   47500.0     -170.45
   50000.0    -1639.43


По идее, если допустима большая неравномерность в полосе пропускания, то можно порядок снизить. И ещё, если нет высоких требований к крутизне ФВЧ (100Гц), то я бы поделил фильтр на два последовательных - сначала ФНЧ низким порядком, потом ФНЧ - подходящим порядком.