10 kHz high shelf
Lifts or drops everything above f0 by a fixed amount and leaves the bottom flat. Solved at 6 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. Shelves fix the slope at S = 1, so there is no Q family to draw; the faint traces are the gain sweep.
Gain at f0 (10 kHz)
+3.00 dB
exact at every sample rate — the bilinear transform maps this value, not just the frequency
Pole radius at 48 kHz
0.4166888
conjugate pair at ±82.56°, 0.583 from the circle
−3 dB point
9986.8 Hz
0.999× f0 at Q = 0.7071
16-bit fixed point
holds
largest pole 0.4167074 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 10 kHz are absent because the filter does not exist there — equivalently, the f₀/Nyquist column never reaches 100%. That is why this table is 6 rows and a 20 Hz page is 8.
| Sample rate | b0 | b1 | b2 | a1 | a2 | Pole r | f₀/Nyquist |
|---|---|---|---|---|---|---|---|
| 22.1 kHz | 1.073462 | 1.628856 | 0.658084 | 1.654468 | 0.705934 | 0.840199 | 90.7% |
| 32 kHz | 1.304371 | 0.349909 | 0.240426 | 0.647922 | 0.246784 | 0.496774 | 62.5% |
| 44.1 kHz | 1.454774 | -0.537243 | 0.284823 | 0.030616 | 0.171739 | 0.414414 | 45.4% |
| 48 kHz | 1.489305 | -0.745544 | 0.322025 | -0.107843 | 0.173630 | 0.416689 | 41.7% |
| 96 kHz | 1.709989 | -2.114437 | 0.780064 | -0.966048 | 0.341664 | 0.584520 | 20.8% |
| 192 kHz | 1.843266 | -2.973789 | 1.247554 | -1.461237 | 0.578268 | 0.760439 | 10.4% |
const float b0 = 1.48930475f, b1 = -0.74554363f, b2 = 0.32202547f;
const float a1 = -0.10784298f, a2 = 0.17362955f; // 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 | — | 0.4166888 | 0.4166888 | yes | reference |
| float32 | — | 0.4166888 | 0.4166888 | yes | 0.0000 dB |
| 32-bit fixed | Q1.30 | 0.4166888 | 0.4166888 | yes | 0.0000 dB |
| 24-bit fixed | Q1.22 | 0.4166888 | 0.4166888 | yes | 0.0000 dB |
| 16-bit fixed | Q1.14 | 0.4167074 | 0.4167074 | yes | 0.0003 dB |
What gain does at 10 kHz
A shelf reaches half its dB gain at f₀ — exactly half, at every sample rate — and its full gain on the far side.
| Gain | At f₀ | b0 | a1 | a2 | Pole r |
|---|---|---|---|---|---|
| -12 dB | −6.00 dB | 0.451364 | -0.683269 | 0.255343 | 0.505315 |
| -6 dB | −3.00 dB | 0.671454 | -0.500598 | 0.216225 | 0.465000 |
| -3 dB | −1.50 dB | 0.819364 | -0.405166 | 0.200743 | 0.448043 |
| +3 dB | +1.50 dB | 1.220459 | -0.208284 | 0.179252 | 0.423382 |
| +6 dB | +3.00 dB | 1.489305 | -0.107843 | 0.173630 | 0.416689 |
| +12 dB | +6.00 dB | 2.215506 | 0.094288 | 0.173145 | 0.416107 |
Questions this filter answers
What are the biquad coefficients for a 10 kHz high-shelf filter at 48 kHz?
b0 = 1.489305, b1 = -0.745544, b2 = 0.322025, a1 = -0.107843, a2 = 0.173630, with a0 normalised to 1 — the RBJ Audio EQ Cookbook form at Q = 0.7071 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 10 kHz high-shelf filter stable in 16-bit fixed point?
Yes. Rounding the five coefficients to a shared 1.14 scale leaves the largest pole at 0.4167074, against 0.4166888 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 10 kHz high-shelf filter?
9986.8 Hz, which is 0.999× the 10 kHz corner. f0 and the −3 dB point are the same frequency only at Q = 1/√2; this page is designed at Q = 0.7071, and a shelf does not read Q at all — its slope is fixed at S = 1, matching Web Audio's BiquadFilterNode, so the gain sweep above is the family that moves this filter rather than a Q sweep.
How close to the unit circle are the poles of a 10 kHz high-shelf filter?
0.4166888 at 48 kHz, as a conjugate pair at ±82.56°. Pole radius rises toward 1 as the corner frequency falls relative to the sample rate — the same filter at 192 kHz sits at 0.7604393 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 10 kHz corner as every other filter type.
- Low-pass10 kHz
- High-pass10 kHz
- Band-pass10 kHz
- Notch10 kHz
- All-pass10 kHz
- Peaking EQ10 kHz
- Low shelf10 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 +3.00 dB at 10 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.