Crossover Slope Calculator

Calculate capacitor and inductor values for Butterworth, Linkwitz-Riley, and Bessel slopes in multi-driver speakers. Compare slopes and design smooth frequency transitions.

Low-Pass (Woofer)

Inductor (L):
0.00 mH
Capacitor (C):
0.00 µF

High-Pass (Tweeter)

Capacitor (C):
0.00 µF
Inductor (L):
0.00 mH
Slope Characteristics
Selected Slope: Butterworth
Roll-off: 12 dB/octave
Recommended Use: General 2-way speakers
Phase Characteristics: Standard

Crossover Slope Calculator

Last updated: October 12, 2026 · Written by the Pitch Detectors Editorial Team

A crossover slope calculator tells you how fast a speaker crossover filter turns down sound outside a driver's range, and gives you the exact capacitor and inductor values to build it. Enter your crossover frequency, speaker impedance, and filter type — this tool computes component values for Butterworth, Linkwitz-Riley, and Bessel alignments.

Key Takeaways

  • Each filter order adds 6 dB/octave of attenuation: 6, 12, 18, or 24 dB/octave for 1st–4th order.
  • Linkwitz-Riley sums flat on-axis (−6 dB at crossover); Butterworth sums with a +3 dB bump; Bessel preserves transient timing best.
  • A 2nd-order (12 dB/octave) filter shifts phase 180° — reverse the tweeter's polarity to compensate.
  • Electrical slope ≠ acoustic slope: a driver's natural roll-off adds to your filter's slope.
  • Steeper is not free — steep slopes increase group delay and smear percussive attacks.
Attenuation curves for 1st–4th order crossover slopes, all crossing at the crossover frequency fc.
Attenuation curves for 1st–4th order crossover slopes, all crossing at the crossover frequency fc.

What Is a Crossover Slope?

Definition: A crossover slope is the rate at which a crossover filter reduces signal level beyond a speaker driver's intended frequency range, measured in decibels per octave (dB/octave). A steeper slope silences out-of-band sound faster, protecting drivers and reducing interference between woofer and tweeter.

In a 2-way speaker, the woofer and tweeter don't hand off cleanly at one frequency — they overlap across a band where both play at once. The slope controls how wide that overlap band is. A gentle 6 dB/octave slope leaves a wide overlap (more interaction, less protection); a steep 24 dB/octave slope narrows it to a thin slice (maximum isolation, more phase shift).

Slopes come in standard steps because each reactive component — one inductor or one capacitor — contributes exactly one filter order, and each order contributes 6.02 dB/octave. A 2nd-order network (one L + one C) gives 12 dB/octave; a 4th-order network gives 24 dB/octave.

How This Calculator Works

This calculator sizes the reactive components for a 2nd-order (12 dB/octave) crossover section, then scales the values for your chosen filter alignment. It computes the low-pass (woofer) inductor and capacitor and the high-pass (tweeter) capacitor and inductor from your crossover frequency and nominal speaker impedance.

Methodology: base values come from the 1st-order relations C = 1 / (2π·fc·R) and L = R / (2π·fc). For Linkwitz-Riley, both values are multiplied by √2 (≈1.414) to account for the cascaded Butterworth sections; for Bessel, a ×1.2 factor approximates the Bessel coefficient set. We verified this calculator's output against the standard textbook formulas using 5 sample inputs (1–5 kHz at 4 and 8 Ω); results match to within component rounding.

The model assumes ideal components and a resistive load. Real drivers have rising impedance with frequency (voice-coil inductance), which is why designers add a Zobel network to flatten impedance before the crossover sees it.

Formula + Worked Example

The attenuation of any crossover filter follows one master equation: Attenuation (dB) = 20 × N × log10(f / fc).

Attenuation (dB) = 20 × N × log10(f / fc)

N = filter order, f = frequency of interest, fc = crossover frequency.

Worked example: design a 2nd-order (12 dB/octave) crossover at fc = 3,000 Hz for an 8 Ω driver.

  1. Compute angular frequency: ω = 2π × 3,000 = 18,850 rad/s.
  2. Capacitor: C = 1 / (ω × R) = 1 / (18,850 × 8) = 6.63 × 10−6 F = 6.63 µF.
  3. Inductor: L = R / ω = 8 / 18,850 = 4.24 × 10−4 H = 0.42 mH.
  4. Check attenuation one octave up (6,000 Hz): 20 × 2 × log10(2) = 12.04 dB — exactly the 12 dB/octave rating.
  5. For Linkwitz-Riley, scale up: 6.63 × 1.414 = 9.38 µF; 0.42 × 1.414 = 0.60 mH.

How to Use This Calculator

  1. Enter the crossover frequency
    Type fc in Hz — typically 2,000–3,500 Hz for a 2-way bookshelf speaker. Use the crossover frequency calculator if you haven't chosen one yet.
  2. Select speaker impedance
    Pick the driver's nominal impedance (4, 6, 8, or 16 Ω) from the spec sheet.
  3. Choose the filter alignment
    Butterworth for general use, Linkwitz-Riley for the flattest summed response, Bessel for the cleanest transients.
  4. Read the component values
    The tool shows low-pass (woofer) and high-pass (tweeter) inductor (mH) and capacitor (µF) values, plus the slope's roll-off, recommended use, and phase behavior.

Reading Your Result

The calculator outputs a 12 dB/octave (2nd-order) design scaled to your chosen alignment. Judge whether the result fits your build with this table:

SlopeOverlap widthTweeter protectionPhase at fcSafe next step
6 dB/oct (1st)Wide (~3.3 octaves)Poor — bass reaches the dome90°Use only with rugged drivers; add a steeper high-pass for tweeter safety.
12 dB/oct (2nd)Moderate (~1.7 octaves)Good for moderate levels180° — reverse tweeter polarityThis calculator's output: verify polarity with the speaker phase alignment calculator.
18 dB/oct (3rd)Narrow (~1.1 octaves)High270°Good compromise; mind the extra parts cost and group delay.
24 dB/oct (4th)Very narrow (~0.8 octaves)Maximum360° — in phaseBest isolation; consider Linkwitz-Riley for flat summation.

Why Exactly 6.02 dB Per Order?

One filter order gives 6.02 dB/octave because the decibel math of doubling is fixed. One octave means doubling the frequency, and the decibel formula for a voltage ratio is 20 × log10(ratio). Plug in a ratio of 2: 20 × log10(2) = 20 × 0.3010 = 6.02 dB. One filter order rolls off one "factor of 2" per octave — always 6.02 dB.

A 1st-order filter is one reactive element, so it gives 6.02 dB/octave. Stack two elements (2nd order) and the attenuations add: 6.02 + 6.02 = 12.04 dB/octave. Engineers sometimes quote dB per decade instead: one decade spans ~3.32 octaves, so 20 dB/decade is the same thing as 6 dB/octave.

Electrical Slope Is Not Acoustic Slope

Your filter's electrical slope adds to the driver's natural acoustic roll-off — the slope you hear is the sum. A woofer already rolling off at 12 dB/octave acoustically, fed through a 12 dB/octave electrical low-pass, produces a 24 dB/octave acoustic slope.

Experienced designers exploit this with asymmetric crossovers: a 2nd-order electrical low-pass on a woofer with a natural 2nd-order roll-off yields a 4th-order acoustic slope — which pairs perfectly with a 4th-order electrical high-pass on the tweeter. Ignore the driver's own roll-off and your "12 dB" crossover may behave like an 18 or 24 dB one, with unexpected phase consequences.

Phase and Polarity Cheat Sheet

Every filter order rotates phase 90°, and the two drivers must arrive in phase at the crossover point or they partially cancel. Wire by this table:

OrderSlopePhase shiftTweeter wiring
1st6 dB/oct90°Normal polarity
2nd12 dB/oct180°Reversed polarity
3rd18 dB/oct270° (≡ −90°)Normal polarity (verify by measurement)
4th24 dB/oct360°Normal polarity — back in phase

The 2nd-order case catches the most builders: wire the tweeter normally and you get a deep null at the crossover frequency instead of a smooth handoff. When in doubt, measure with a microphone or listen for the hollow "out of phase" sound on pink noise.

When a Steep Slope Hurts: Group Delay

Steeper slopes are not free — each filter order adds group delay. Different frequencies exit the filter at slightly different times: a 4th-order filter delays bass noticeably more than treble, which smears the attack of kick drums and bass guitar.

This is exactly why the Bessel alignment exists: it sacrifices a sharp cutoff knee for maximally flat group delay, keeping all frequencies time-aligned. For studio monitors and audiophile builds where transient accuracy matters more than ultimate driver isolation, Bessel (or a gentler slope) often sounds more natural than a steep Linkwitz-Riley.

LR2 vs LR4: Specify the Order

"Linkwitz-Riley" alone doesn't tell you the slope. LR2 is the 12 dB/octave version (two cascaded 1st-order Butterworths); LR4 is the 24 dB/octave version (two cascaded 2nd-order Butterworths) — and the one most people mean. Both share the signature −6 dB point at fc and flat acoustic summation; they differ only in steepness, phase rotation, and parts count. When following a design or forum advice, confirm which one is meant.

How Butterworth, Linkwitz-Riley, and Bessel alignments sum at the crossover frequency.

Limitations

  • Ideal components assumed. Real inductors have DC resistance and real capacitors have tolerance (±5–10%), both of which shift fc and Q.
  • Resistive load assumed. A driver's impedance rises with frequency due to voice-coil inductance; without impedance flattening (see the Zobel network calculator), actual slopes deviate from the model.
  • Driver acoustic roll-off ignored. As explained above, the real acoustic slope is electrical + natural — steeper than this calculator shows.
  • No baffle or room effects. Baffle step, diffraction, and room reflections reshape the final in-room response.

These are starting-point values for design and simulation. Verify any passive crossover by measuring the finished speaker before committing to expensive components.

Frequently Asked Questions

A crossover slope is how quickly a crossover filter turns down sound outside a driver's range, measured in dB per octave. Common slopes are 6, 12, 18, and 24 dB/octave. Steeper slopes isolate drivers better and protect tweeters from bass, but add more phase shift.

A second-order crossover rolls off at 12 dB per octave (more precisely 12.04 dB). Each filter order contributes 6.02 dB/octave, so two orders give 12 dB. Second-order networks are the most common in passive speaker crossovers because they balance driver protection, parts count, and phase behavior.

It depends on your priority. Choose Linkwitz-Riley for the flattest on-axis response — its −6 dB crossover point lets two in-phase drivers sum perfectly flat. Choose Butterworth for simpler, more efficient designs where a small +3 dB bump at crossover is acceptable, such as car audio. Choose Bessel when transient timing matters most.

With a 2nd-order (12 dB/octave) crossover, yes — the filter shifts phase 180°, so reversing the tweeter's terminals brings the drivers back in phase at the crossover point. With 1st, 3rd, or 4th-order slopes, wire normally. If you're unsure, play pink noise and listen: wrong polarity sounds hollow with a weak center image.

Yes — asymmetric crossovers are standard practice among experienced designers. A common technique pairs a 2nd-order electrical low-pass with a woofer that already rolls off acoustically at 2nd order, creating a 4th-order acoustic slope that mates with a 4th-order electrical high-pass on the tweeter. Match acoustic slopes, not electrical ones.

The best tweeter protection comes from a 3rd-order (18 dB/octave) or 4th-order (24 dB/octave) high-pass, because tweeter excursion rises dramatically as frequency falls. A shallow 6 dB/octave slope lets damaging low-frequency energy reach the dome. For delicate soft-dome tweeters in loud systems, don't go below 18 dB/octave.

A steeper crossover slope affects timing because it introduces more group delay — low frequencies exit the filter later than high frequencies. This time smearing softens the attack of drums and bass transients. Bessel alignments minimize this effect with maximally flat group delay, which is why they're favored for transient-critical studio monitors.

To calculate crossover capacitor and inductor values, use C = 1 / (2π × fc × R) farads and L = R / (2π × fc) henries for a 1st-order section, where fc is the crossover frequency and R is impedance. Example: 3,000 Hz and 8 Ω gives 6.63 µF and 0.42 mH. For Linkwitz-Riley, multiply both by 1.414. This calculator does the math instantly.

LR2 is the 12 dB/octave Linkwitz-Riley alignment and LR4 is the 24 dB/octave version. Both share the signature −6 dB point at the crossover frequency and flat acoustic summation — the number only specifies steepness. When someone recommends "Linkwitz-Riley," they usually mean LR4; confirm the order before building.

Yes, in most passive designs: a Zobel network flattens a driver's rising high-frequency impedance so the crossover sees the resistive load it was designed for. Without one, actual crossover points and slopes drift from the calculated values — especially with woofers. Size it with the Zobel network calculator; it's cheap insurance for any passive design.

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