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Omnikalc

Passive two-way crossover calculator

Get the inductor and capacitor values of a passive two-way speaker crossover for a chosen frequency, driver impedance and filter type: first order, second-order Linkwitz-Riley or Butterworth.

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Hz

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Ω

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Ω

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Filter type

Results

Woofer low-pass inductor (in series)

1.019 mH

Tweeter high-pass capacitor (in series)

3.98 µF

Woofer low-pass capacitor (in parallel, 2nd order only)
3.98 µF
Tweeter high-pass inductor (in parallel, 2nd order only)
1.019 mH
Tweeter polarity
2
2nd order: reverse the tweeter's polarity so both outputs add in phase at the crossover

What a crossover does

A two-way loudspeaker splits the music between a woofer, which handles the bass and midrange, and a tweeter, which handles the treble. The passive crossover is the small network of inductors and capacitors between the amplifier and the drivers that makes the split. An inductor in series passes low frequencies and blocks high ones; a capacitor in series does the opposite.

The formulas

For a crossover frequency f in hertz and a driver impedance R in ohms, the component values are a constant times R ÷ f for inductors, or a constant ÷ (R × f) for capacitors:

Filter type Series inductor (woofer) Series capacitor (tweeter) Parallel parts
1st order, 6 dB/octave 0.1592 × R ÷ f 0.1592 ÷ (R × f) none
2nd order Linkwitz-Riley 0.3183 × R ÷ f 0.0796 ÷ (R × f) same constants, swapped
2nd order Butterworth 0.2251 × R ÷ f 0.1125 ÷ (R × f) same constants, swapped

The calculator converts the results to millihenries and microfarads. In a second-order filter, the woofer also gets a capacitor across it and the tweeter an inductor across it.

Example

At 2,500 Hz with two 8 Ω drivers and a Linkwitz-Riley filter, the woofer needs a 1.02 mH series inductor and a 3.98 µF parallel capacitor; the tweeter gets a 3.98 µF series capacitor and a 1.02 mH parallel inductor. A Linkwitz-Riley filter is −6 dB at the crossover on each side, so the two outputs add up to a flat response, provided the tweeter is wired in reverse polarity.

Choosing parts

  • Use the nearest standard value; a few percent off moves the crossover point only slightly.
  • Prefer air-core inductors for the woofer side if the budget allows, and film capacitors rather than electrolytics on the tweeter.
  • A tweeter should be crossed at least an octave above its resonance frequency (Fs) to protect it.

Limits of the textbook formulas

Real drivers are not resistors: their impedance rises with frequency because of the voice-coil inductance, and peaks at resonance. Builders often add a Zobel network across the woofer to flatten its impedance, and an L-pad to lower a tweeter that is more sensitive than the woofer. The values from this calculator are an excellent starting point, but a measured response with a microphone is what tells you whether the crossover sums correctly in your cabinet.

Frequently asked questions

What crossover frequency should I choose for a two-way speaker?

Most two-way designs cross between 1,800 and 3,500 Hz. Stay at least an octave above the tweeter's resonance frequency and below the frequency where the woofer starts to beam or break up.

Why must the tweeter be wired in reverse polarity?

A second-order filter shifts the woofer and tweeter outputs by 180° relative to each other at the crossover. Reversing the tweeter brings them back in phase, so they add up instead of creating a dip.

What is the difference between Linkwitz-Riley and Butterworth?

Both slope at 12 dB per octave. Linkwitz-Riley sections are −6 dB at the crossover and sum flat in amplitude; Butterworth sections are −3 dB and produce a 3 dB bump when summed.

Can I use the nominal impedance printed on the driver?

It is a reasonable start, but real impedance varies with frequency. For accurate results use the impedance measured at the crossover frequency, or add a Zobel network to flatten the woofer's impedance.

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Results are estimates provided for information purposes. They do not replace professional advice.