6.3 kHz peaking eq
Boosts or cuts a band around f0 and leaves both ends of the spectrum at unity. Solved at 7 sample rates, with the poles, the real −3 dB point and the word length it stops working at.
Magnitude response at 48 kHz
Every vertex is 20·log₁₀|H(ejω)| evaluated on the unit circle — not a sketch of the filter's shape. The faint traces behind it are the same corner at every Q in the sweep below.
Gain at f0 (6.3 kHz)
+6.00 dB
exact at every sample rate — the bilinear transform maps this value, not just the frequency
Pole radius at 48 kHz
0.7664134
conjugate pair at ±45.33°, 0.234 from the circle
−3 dB point
4027.7 Hz
0.639× f0 at Q = 1.0000
16-bit fixed point
holds
largest pole 0.7664218 in Q1.14
Coefficients, at every sample rate
The cookbook computes w₀ = 2πf₀/Fs, so the same filter is a different set of numbers at every rate. Rates whose Nyquist limit is at or below 6.3 kHz are absent because the filter does not exist there — equivalently, the f₀/Nyquist column never reaches 100%. That is why this table is 7 rows and a 20 Hz page is 8.
| Sample rate | b0 | b1 | b2 | a1 | a2 | Pole r | f₀/Nyquist |
|---|---|---|---|---|---|---|---|
| 16 kHz | 1.178900 | 1.288310 | 0.461598 | 1.288310 | 0.640497 | 0.800311 | 78.8% |
| 22.1 kHz | 1.255344 | 0.330862 | 0.231536 | 0.330862 | 0.486880 | 0.697768 | 57.1% |
| 32 kHz | 1.249432 | -0.491039 | 0.249329 | -0.491039 | 0.498761 | 0.706230 | 39.4% |
| 44.1 kHz | 1.215733 | -0.976685 | 0.350748 | -0.976685 | 0.566481 | 0.752649 | 28.6% |
| 48 kHz | 1.205328 | -1.077521 | 0.382062 | -1.077521 | 0.587389 | 0.766413 | 26.3% |
| 96 kHz | 1.123643 | -1.604737 | 0.627894 | -1.604737 | 0.751537 | 0.866912 | 13.1% |
| 192 kHz | 1.067246 | -1.825376 | 0.797623 | -1.825376 | 0.864869 | 0.929983 | 6.6% |
const float b0 = 1.20532787f, b1 = -1.07752114f, b2 = 0.38206158f;
const float a1 = -1.07752114f, a2 = 0.58738944f; // a0 == 1What word length this filter survives
The fixed-point rows round all five coefficients to one shared scale, which is what a q15/q31 biquad section does with its post-shift.Pole radius is solved from the quadratic, not taken as √|a₂| — once rounding pushes the poles onto the real axis those two disagree, and the convenient one reports a comfortable margin on a filter that has already left the unit circle. Error is the worst deviation from float64 across frequencies where the response is within 40 dB of its own peak; below that it is measuring the −200 dB floor.
| Word format | Q format | Largest pole | √|a₂| says | Stable | Worst error in band |
|---|---|---|---|---|---|
| float64 | — | 0.7664134 | 0.7664134 | yes | reference |
| float32 | — | 0.7664134 | 0.7664134 | yes | 0.0000 dB |
| 32-bit fixed | Q1.30 | 0.7664134 | 0.7664134 | yes | 0.0000 dB |
| 24-bit fixed | Q1.22 | 0.7664134 | 0.7664134 | yes | 0.0000 dB |
| 16-bit fixed | Q1.14 | 0.7664218 | 0.7664218 | yes | 0.0003 dB |
What Q does at 6.3 kHz
f₀ does not move with Q — the −3 dB point does. They are the same frequency only at Q = 1/√2, which is why a Butterworth corner is the one people quote and why every other Q surprises somebody.
| Q | At f₀ | Peak | −3 dB | Pole r | Group delay at f₀ |
|---|---|---|---|---|---|
| 0.5 | +6.00 dB | +6.00 dB @ 6.31 kHz | 12435 Hz | 0.562059 | 0.020 ms |
| 0.7071 | +6.00 dB | +6.00 dB @ 6.31 kHz | 10735 Hz | 0.680014 | 0.028 ms |
| 1 | +6.00 dB | +6.00 dB @ 6.31 kHz | 9422 Hz | 0.766413 | 0.040 ms |
| 2 | +6.00 dB | +6.00 dB @ 6.31 kHz | 7808 Hz | 0.877477 | 0.080 ms |
| 4 | +6.00 dB | +6.00 dB @ 6.31 kHz | 7032 Hz | 0.936998 | 0.160 ms |
| 10 | +6.00 dB | +5.98 dB @ 6.31 kHz | 6588 Hz | 0.974336 | 0.400 ms |
What gain does at 6.3 kHz
A peaking filter puts its full gain at f₀ and returns to unity at both ends of the spectrum.
| Gain | At f₀ | b0 | a1 | a2 | Pole r |
|---|---|---|---|---|---|
| -12 dB | −12.00 dB | 0.683382 | -0.783571 | 0.154346 | 0.392869 |
| -6 dB | −6.00 dB | 0.829650 | -0.893965 | 0.316977 | 0.563007 |
| -3 dB | −3.00 dB | 0.911273 | -0.945160 | 0.392397 | 0.626416 |
| +3 dB | +3.00 dB | 1.097365 | -1.037186 | 0.527968 | 0.726614 |
| +6 dB | +6.00 dB | 1.205328 | -1.077521 | 0.587389 | 0.766413 |
| +12 dB | +12.00 dB | 1.463310 | -1.146607 | 0.689166 | 0.830160 |
Questions this filter answers
What are the biquad coefficients for a 6.3 kHz peaking EQ filter at 48 kHz?
b0 = 1.205328, b1 = -1.077521, b2 = 0.382062, a1 = -1.077521, a2 = 0.587389, with a0 normalised to 1 — the RBJ Audio EQ Cookbook form at Q = 1.0000 and +6 dB of gain. Every other sample rate in the table above gives different numbers for the same filter, because w0 = 2πf0/Fs and every cosine and sine downstream of it moves.
Is a 6.3 kHz peaking EQ filter stable in 16-bit fixed point?
Yes. Rounding the five coefficients to a shared 1.14 scale leaves the largest pole at 0.7664218, against 0.7664134 exact, and the response drifts by at most 0.000 dB inside the band. 24-bit takes that to 0.0000 dB.
Where is the real −3 dB point of a 6.3 kHz peaking EQ filter?
4027.7 Hz, which is 0.639× the 6.3 kHz corner. f0 and the −3 dB point are the same frequency only at Q = 1/√2; this page is designed at Q = 1.0000, and the Q sweep above shows the point moving from 12435.4 Hz to 6587.9 Hz across the sweep while f0 never moves.
How close to the unit circle are the poles of a 6.3 kHz peaking EQ filter?
0.7664134 at 48 kHz, as a conjugate pair at ±45.33°. Pole radius rises toward 1 as the corner frequency falls relative to the sample rate — the same filter at 192 kHz sits at 0.9299831 and at 8 kHz it is above Nyquist. That distance is the whole story of the fixed-point table: a pole a few parts in 10⁵ from the circle has nowhere to be rounded to.
The neighbouring corners
One third-octave either side, and the same 6.3 kHz corner as every other filter type.
- Low-pass6.3 kHz
- High-pass6.3 kHz
- Band-pass6.3 kHz
- Notch6.3 kHz
- All-pass6.3 kHz
- Low shelf6.3 kHz
- High shelf6.3 kHz
Method and limits. Coefficients follow the RBJ Audio EQ Cookbook, the bilinear transform of the analog prototype prewarped so the corner lands exactly on f0 — which is why +6.00 dB at 6.3 kHz holds at every sample rate in the table rather than only at low f0/Fs. Shelves fix the slope at S = 1, matching Web Audio's BiquadFilterNode, so Q is not read for those two types. Pole and zero radii are the roots of the quadratic, not sqrt(|a2|). The fixed-point rows model a single shared coefficient scale and no other quantisation: they say nothing about signal-path headroom, limit cycles or the accumulator width your implementation uses, all of which can make a filter that passes this table still misbehave. Nothing on this page is fetched or estimated — it is solved from the type and the frequency in the URL.