RACK/FILTERS & ENCLOSURES
H(f)H(f)

Crossover filters

Shape the handoff. See exactly what your filter does.

Inputs

YOUR SYSTEM
Hz
2020000
Filter order
Filter type

Result

METER
Asymptotic roll-off
12.0dB/oct
2-order low-pass Butterworth response
Response at cutoff
-3.01dB
Slope per decade
40dB/dec
Cutoff frequency
1,000Hz
0-12-24-36-48201126323.56k20kdBFREQUENCY / Hz1,000 Hz CUTOFF
Butterworth magnitude response: Ideal Butterworth filter

How it works

The slope is only part of the story.

A Butterworth filter has a flat passband and is down about 3 dB at its cutoff. Increasing the order makes the transition steeper and adds more phase shift.

The formula

L(f)=−10log⁡10(1+(ffc)2n)(low-pass)L(f) = -10 \log_{10}\left(1 + \left(\frac{f}{f_c}\right)^{2n}\right) \quad \text{(low-pass)}
  • fcf_c — cutoff frequency in Hz\text{Hz}
  • nn — filter order
  • High-pass: replace f/fcf / f_c with fc/ff_c / f

Worth knowing

Two Butterworth sections do not automatically make a flat-summing crossover. Linkwitz-Riley filters have different crossover behavior and are not modeled here.

Assumptions

An ideal electrical magnitude response, not the acoustic sum of real drivers. Driver response, phase, polarity, latency and other filter families are not included.

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