6.3 kHz band-pass
Passes a band centred on f0 at unity gain and rejects everything either side. 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)
0.00 dB
exact at every sample rate — the bilinear transform maps this value, not just the frequency
Pole radius at 48 kHz
0.6803567
conjugate pair at ±43.13°, 0.320 from the circle
−3 dB point
9410.4 Hz
1.494× f0 at Q = 1.0000
16-bit fixed point
holds
largest pole 0.6803607 in Q0.15
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 | 0.236377 | 0.000000 | -0.236377 | 1.199372 | 0.527246 | 0.726117 | 78.8% |
| 22.1 kHz | 0.327715 | 0.000000 | -0.327715 | 0.299195 | 0.344570 | 0.587001 | 57.1% |
| 32 kHz | 0.320838 | 0.000000 | -0.320838 | -0.445028 | 0.358324 | 0.598601 | 39.4% |
| 44.1 kHz | 0.281049 | 0.000000 | -0.281049 | -0.896517 | 0.437902 | 0.661741 | 28.6% |
| 48 kHz | 0.268557 | 0.000000 | -0.268557 | -0.993008 | 0.462885 | 0.680357 | 26.3% |
| 96 kHz | 0.166927 | 0.000000 | -0.166927 | -1.526504 | 0.666147 | 0.816178 | 13.1% |
| 192 kHz | 0.092851 | 0.000000 | -0.092851 | -1.775876 | 0.814298 | 0.902385 | 6.6% |
const float b0 = 0.26855739f, b1 = 0.00000000f, b2 = -0.26855739f;
const float a1 = -0.99300758f, a2 = 0.46288523f; // 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 | — | 0.6803567 | 0.6803567 | yes | reference |
| float32 | — | 0.6803567 | 0.6803567 | yes | 0.0000 dB |
| 32-bit fixed | Q0.31 | 0.6803567 | 0.6803567 | yes | 0.0000 dB |
| 24-bit fixed | Q0.23 | 0.6803567 | 0.6803567 | yes | 0.0000 dB |
| 16-bit fixed | Q0.15 | 0.6803607 | 0.6803607 | yes | 0.0001 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 | 0.00 dB | 0.00 dB @ 6.31 kHz | 12416 Hz | 0.391392 | 0.028 ms |
| 0.7071 | 0.00 dB | 0.00 dB @ 6.31 kHz | 10720 Hz | 0.562533 | 0.040 ms |
| 1 | 0.00 dB | 0.00 dB @ 6.31 kHz | 9410 Hz | 0.680357 | 0.057 ms |
| 2 | 0.00 dB | 0.00 dB @ 6.31 kHz | 7802 Hz | 0.830535 | 0.113 ms |
| 4 | 0.00 dB | 0.00 dB @ 6.31 kHz | 7029 Hz | 0.912060 | 0.227 ms |
| 10 | 0.00 dB | −0.01 dB @ 6.31 kHz | 6586 Hz | 0.963934 | 0.567 ms |
Questions this filter answers
What are the biquad coefficients for a 6.3 kHz band-pass filter at 48 kHz?
b0 = 0.268557, b1 = 0.000000, b2 = -0.268557, a1 = -0.993008, a2 = 0.462885, with a0 normalised to 1 — the RBJ Audio EQ Cookbook form at Q = 1.0000. 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 band-pass filter stable in 16-bit fixed point?
Yes. Rounding the five coefficients to a shared 0.15 scale leaves the largest pole at 0.6803607, against 0.6803567 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 band-pass filter?
9410.4 Hz, which is 1.494× 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 12416.1 Hz to 6585.9 Hz across the sweep while f0 never moves.
How close to the unit circle are the poles of a 6.3 kHz band-pass filter?
0.6803567 at 48 kHz, as a conjugate pair at ±43.13°. Pole radius rises toward 1 as the corner frequency falls relative to the sample rate — the same filter at 192 kHz sits at 0.9023846 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
- Notch6.3 kHz
- All-pass6.3 kHz
- Peaking EQ6.3 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 0.00 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.