800 Hz band-pass
Passes a band centred on f0 at unity gain and rejects everything either side. Solved at 8 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 (800 Hz)
0.00 dB
exact at every sample rate — the bilinear transform maps this value, not just the frequency
Pole radius at 48 kHz
0.9490328
conjugate pair at ±5.20°, 0.0510 from the circle
−3 dB point
1293.0 Hz
1.616× f0 at Q = 1.0000
16-bit fixed point
holds
largest pole 0.9490178 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 800 Hz are absent because the filter does not exist there — equivalently, the f₀/Nyquist column never reaches 100%. That is why this table is 8 rows and a 20 Hz page is 8.
| Sample rate | b0 | b1 | b2 | a1 | a2 | Pole r | f₀/Nyquist |
|---|---|---|---|---|---|---|---|
| 8 kHz | 0.227138 | 0.000000 | -0.227138 | -1.250516 | 0.545723 | 0.738731 | 20.0% |
| 16 kHz | 0.133831 | 0.000000 | -0.133831 | -1.647552 | 0.732339 | 0.855768 | 10.0% |
| 22.1 kHz | 0.101524 | 0.000000 | -0.101524 | -1.750463 | 0.796952 | 0.892721 | 7.3% |
| 32 kHz | 0.072543 | 0.000000 | -0.072543 | -1.832077 | 0.854914 | 0.924615 | 5.0% |
| 44.1 kHz | 0.053807 | 0.000000 | -0.053807 | -1.880106 | 0.892386 | 0.944662 | 3.6% |
| 48 kHz | 0.049668 | 0.000000 | -0.049668 | -1.890251 | 0.900663 | 0.949033 | 3.3% |
| 96 kHz | 0.025501 | 0.000000 | -0.025501 | -1.946328 | 0.948999 | 0.974166 | 1.7% |
| 192 kHz | 0.012919 | 0.000000 | -0.012919 | -1.973485 | 0.974161 | 0.986996 | 0.8% |
const float b0 = 0.04966835f, b1 = 0.00000000f, b2 = -0.04966835f;
const float a1 = -1.89025126f, a2 = 0.90066329f; // 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 | — | 0.9490328 | 0.9490328 | yes | reference |
| float32 | — | 0.9490328 | 0.9490328 | yes | 0.0000 dB |
| 32-bit fixed | Q1.30 | 0.9490328 | 0.9490328 | yes | 0.0000 dB |
| 24-bit fixed | Q1.22 | 0.9490329 | 0.9490329 | yes | 0.0002 dB |
| 16-bit fixed | Q1.14 | 0.9490178 | 0.9490178 | yes | 0.0326 dB |
What Q does at 800 Hz
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 @ 812 Hz | 1923 Hz | 0.900404 | 0.199 ms |
| 0.7071 | 0.00 dB | 0.00 dB @ 812 Hz | 1542 Hz | 0.928627 | 0.282 ms |
| 1 | 0.00 dB | 0.00 dB @ 812 Hz | 1293 Hz | 0.949033 | 0.399 ms |
| 2 | 0.00 dB | −0.01 dB @ 812 Hz | 1025 Hz | 0.974201 | 0.797 ms |
| 4 | 0.00 dB | −0.06 dB @ 812 Hz | 907.5 Hz | 0.987018 | 1.594 ms |
| 10 | 0.00 dB | −0.35 dB @ 812 Hz | 844.3 Hz | 0.994787 | 3.986 ms |
Questions this filter answers
What are the biquad coefficients for a 800 Hz band-pass filter at 48 kHz?
b0 = 0.049668, b1 = 0.000000, b2 = -0.049668, a1 = -1.890251, a2 = 0.900663, 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 800 Hz band-pass filter stable in 16-bit fixed point?
Yes. Rounding the five coefficients to a shared 1.14 scale leaves the largest pole at 0.9490178, against 0.9490328 exact, and the response drifts by at most 0.033 dB inside the band. 24-bit takes that to 0.0002 dB.
Where is the real −3 dB point of a 800 Hz band-pass filter?
1293.0 Hz, which is 1.616× the 800 Hz 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 1923.2 Hz to 844.3 Hz across the sweep while f0 never moves.
How close to the unit circle are the poles of a 800 Hz band-pass filter?
0.9490328 at 48 kHz, as a conjugate pair at ±5.20°. Pole radius rises toward 1 as the corner frequency falls relative to the sample rate — the same filter at 192 kHz sits at 0.9869961 and at 8 kHz at 0.7387309. 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 800 Hz corner as every other filter type.
- Low-pass800 Hz
- High-pass800 Hz
- Notch800 Hz
- All-pass800 Hz
- Peaking EQ800 Hz
- Low shelf800 Hz
- High shelf800 Hz
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 800 Hz 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.