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Speaker Crossover Calculator (Component Values)

Crossover frequency + driver impedances → the capacitor and inductor values for 1st and 2nd-order passive networks, with slope trade-offs explained.

0
Tweeter capacitor (µF)
0
Woofer inductor (mH)
0
Tweeter inductor (2nd order)
0
Woofer capacitor (2nd order)

Driver 'impedance' is a curve, not the nameplate number — an '8 Ω' woofer swings 6–40 Ω with frequency, which is why textbook crossovers need tweaking (or Zobel networks) in real cabinets. LR2 wires the tweeter inverted-polarity to sum flat; LR4 is the studio standard but needs twice the parts.

Formula

1st order: C = 1/(2πfZ), L = Z/(2πf); LR2: C = 1/(4πfZ), L = Z/(πf)·½ — series element + shunt element per driver
References: Linkwitz & Riley (1976), 'Active crossover networks' (JAES); Dickason, V., The Loudspeaker Design Cookbook

⚠️ Acoustic estimates from standard formulas — real rooms, drivers and ears vary. For hearing-safety decisions use a calibrated SPL meter and official occupational limits.

Crossover frequency + driver impedances → the capacitor and inductor values for 1st and 2nd-order passive networks, with slope trade-offs explained.

About Speaker Crossover Calculator (Component Values)

A two-way speaker is a treaty between drivers, and the crossover is its text: above this frequency the tweeter, below it the woofer, with the handoff's steepness set by filter order. This calculator computes the actual component values — capacitors in microfarads, inductors in millihenries — for first-order and Linkwitz-Riley second-order passive networks at any crossover point and impedance, with the engineering trade-offs (slope vs phase vs parts count) stated honestly.

How to use Speaker Crossover Calculator (Component Values)

  1. 1Enter — sensible defaults are pre-filled so you see a worked result immediately.
  2. 2Read the live results: .
  3. 3Check the "With your numbers" line to see the formula 1st order: C = 1/(2πfZ), L = Z/(2πf); LR2: C = 1/(4πfZ), L = Z/(πf)·½ — series element + shunt element per driver substituted step by step.
  4. 4Adjust inputs (or flip the unit toggle) until the scenario matches yours, then copy or share the result.

Why use Speaker Crossover Calculator (Component Values)?

  • Instant, free and private — every calculation runs in your browser, nothing is uploaded
  • Built on the published formula 1st order: C = 1/(2πfZ), L = Z/(2πf); LR2: C = 1/(4πfZ), L = Z/(πf)·½ — series element + shunt element per driver with sources cited on the page
  • Driver 'impedance' is a curve, not the nameplate number — an '8 Ω' woofer swings 6–40 Ω with frequency, which is why textbook crossovers need tweaking (or Zobel networks) in real cabinets. LR2 wires the tweeter inverted-polarity to sum flat; LR4 is the studio standard but needs twice the parts.
  • Switch units, tweak any input and watch every result update live

Frequently asked questions

How do I choose the crossover frequency itself?+

Bracket it from both drivers' limits: the tweeter sets the floor — cross at least an octave above its resonance (Fs 700 Hz → cross no lower than 1.4 kHz, higher with shallow slopes) or excursion and distortion soar; the woofer sets the ceiling — beaming begins where wavelength equals cone diameter (a 6.5-inch mid-woofer beams above ~2 kHz) and breakup follows. Typical sweet spots: 2–3 kHz for dome-tweeter two-ways, 80 Hz for sub/satellite splits (the THX convention — below where localization begins). The 2.5 kHz default is the industry's center of gravity for a reason.

What does filter order actually trade?+

Slope against phase and parts: 1st order (6 dB/oct) is one component per driver and the only type preserving a perfect transient waveform — but drivers must behave two octaves past the crossover, which real tweeters resent (distortion, power handling). 2nd order LR (12 dB/oct) protects drivers far better, sums flat with the tweeter inverted, two parts per driver. 4th order LR (the pro/studio standard) isolates drivers almost completely at the cost of four parts per leg and more group delay. Higher order = better driver protection, worse transient purity, more money in copper and film.

Why did my textbook crossover sound wrong in the actual cabinet?+

Three liars: impedance (the formula assumed 8 Ω; the driver's curve swings 6–40 Ω — a Zobel network flattens the woofer's rise, or the crossover point slides up and the slope warps), sensitivity mismatch (tweeters typically run 2–4 dB hotter than woofers and need an L-pad), and acoustic centers (the tweeter's voice coil sits ahead of the woofer's, so their outputs arrive misaligned at the crossover — the reason commercial designs measure, tilt baffles, or fix it in DSP). The values from this page are the correct STARTING point; speakers are finished with a measurement mic.

Passive components or active/DSP crossover — which way in 2026?+

Passive remains right for finished consumer speakers (one amp, no electronics per box) — but actives have quietly won everywhere else: studio monitors, PA, car audio DSP and DIY-with-plate-amps all filter BEFORE amplification, where a crossover is software (any slope, any delay, driver time-alignment for free) and each driver gets a dedicated amp channel. The economics crossed over too: a 2×100 W DSP plate amp costs less than the film caps and air-core inductors of a serious LR4 passive network. Learn the passive math — this page — and then check whether your project shouldn't simply skip it.

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