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.
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
⚠️ 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)
- 1Enter — sensible defaults are pre-filled so you see a worked result immediately.
- 2Read the live results: .
- 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.
- 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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