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.
What Is a Crossover Slope?
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.
- Compute angular frequency: ω = 2π × 3,000 = 18,850 rad/s.
- Capacitor: C = 1 / (ω × R) = 1 / (18,850 × 8) = 6.63 × 10−6 F = 6.63 µF.
- Inductor: L = R / ω = 8 / 18,850 = 4.24 × 10−4 H = 0.42 mH.
- Check attenuation one octave up (6,000 Hz): 20 × 2 × log10(2) = 12.04 dB — exactly the 12 dB/octave rating.
- For Linkwitz-Riley, scale up: 6.63 × 1.414 = 9.38 µF; 0.42 × 1.414 = 0.60 mH.
How to Use This Calculator
- Enter the crossover frequencyType 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.
- Select speaker impedancePick the driver's nominal impedance (4, 6, 8, or 16 Ω) from the spec sheet.
- Choose the filter alignmentButterworth for general use, Linkwitz-Riley for the flattest summed response, Bessel for the cleanest transients.
- Read the component valuesThe 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:
| Slope | Overlap width | Tweeter protection | Phase at fc | Safe next step |
|---|---|---|---|---|
| 6 dB/oct (1st) | Wide (~3.3 octaves) | Poor — bass reaches the dome | 90° | Use only with rugged drivers; add a steeper high-pass for tweeter safety. |
| 12 dB/oct (2nd) | Moderate (~1.7 octaves) | Good for moderate levels | 180° — reverse tweeter polarity | This calculator's output: verify polarity with the speaker phase alignment calculator. |
| 18 dB/oct (3rd) | Narrow (~1.1 octaves) | High | 270° | Good compromise; mind the extra parts cost and group delay. |
| 24 dB/oct (4th) | Very narrow (~0.8 octaves) | Maximum | 360° — in phase | Best 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:
| Order | Slope | Phase shift | Tweeter wiring |
|---|---|---|---|
| 1st | 6 dB/oct | 90° | Normal polarity |
| 2nd | 12 dB/oct | 180° | Reversed polarity |
| 3rd | 18 dB/oct | 270° (≡ −90°) | Normal polarity (verify by measurement) |
| 4th | 24 dB/oct | 360° | 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.
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.