2.5 kHz notch
Removes one frequency and leaves the rest of the spectrum untouched. 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 (2.5 kHz)
−∞ dB
exact at every sample rate — the bilinear transform maps this value, not just the frequency
Pole radius at 48 kHz
0.8503345
conjugate pair at ±16.38°, 0.150 from the circle
−3 dB point
none
the magnitude never falls 3 dB below its own peak inside the band
16-bit fixed point
holds
largest pole 0.8503432 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 2.5 kHz 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 | 0.684023 | 0.523528 | 0.684023 | 0.523528 | 0.368045 | 0.606667 | 62.5% |
| 16 kHz | 0.706347 | -0.784851 | 0.706347 | -0.784851 | 0.412694 | 0.642413 | 31.3% |
| 22.1 kHz | 0.753683 | -1.140788 | 0.753683 | -1.140788 | 0.507366 | 0.712296 | 22.7% |
| 32 kHz | 0.809259 | -1.427405 | 0.809259 | -1.427405 | 0.618518 | 0.786459 | 15.6% |
| 44.1 kHz | 0.851533 | -1.596168 | 0.851533 | -1.596168 | 0.703066 | 0.838490 | 11.3% |
| 48 kHz | 0.861534 | -1.631626 | 0.861534 | -1.631626 | 0.723069 | 0.850335 | 10.4% |
| 96 kHz | 0.924686 | -1.824671 | 0.924686 | -1.824671 | 0.849373 | 0.921614 | 5.2% |
| 192 kHz | 0.960744 | -1.915060 | 0.960744 | -1.915060 | 0.921487 | 0.959941 | 2.6% |
const float b0 = 0.86153442f, b1 = -1.63162580f, b2 = 0.86153442f;
const float a1 = -1.63162580f, a2 = 0.72306884f; // 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 | — | 0.8503345 | 0.8503345 | yes | reference |
| float32 | — | 0.8503345 | 0.8503345 | yes | 0.0001 dB |
| 32-bit fixed | Q1.30 | 0.8503345 | 0.8503345 | yes | 0.0000 dB |
| 24-bit fixed | Q1.22 | 0.8503346 | 0.8503346 | yes | 0.0007 dB |
| 16-bit fixed | Q1.14 | 0.8503432 | 0.8503432 | yes | 0.2249 dB |
What Q does at 2.5 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 | −∞ dB | 0.00 dB @ 24.00 kHz | 5795 Hz | 0.716590 | -99.935 ms |
| 0.7071 | −∞ dB | 0.00 dB @ 24.00 kHz | 4717 Hz | 0.793476 | -99.908 ms |
| 1 | −∞ dB | 0.00 dB @ 24.00 kHz | 3988 Hz | 0.850335 | -99.870 ms |
| 2 | −∞ dB | 0.00 dB @ 24.00 kHz | — | 0.922624 | -99.741 ms |
| 4 | −∞ dB | 0.00 dB @ 24.00 kHz | 2825 Hz | 0.960596 | -99.482 ms |
| 10 | −∞ dB | 0.00 dB @ 24.00 kHz | 2626 Hz | 0.984055 | -98.704 ms |
Questions this filter answers
What are the biquad coefficients for a 2.5 kHz notch filter at 48 kHz?
b0 = 0.861534, b1 = -1.631626, b2 = 0.861534, a1 = -1.631626, a2 = 0.723069, 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 2.5 kHz notch filter stable in 16-bit fixed point?
Yes. Rounding the five coefficients to a shared 1.14 scale leaves the largest pole at 0.8503432, against 0.8503345 exact, and the response drifts by at most 0.225 dB inside the band. 24-bit takes that to 0.0007 dB.
Where is the real −3 dB point of a 2.5 kHz notch filter?
This type has no −3 dB edge to find: its magnitude response sits at 0.00 dB at its peak and never falls 3 dB below it inside the band. At f0 the response measures −∞ dB.
How close to the unit circle are the poles of a 2.5 kHz notch filter?
0.8503345 at 48 kHz, as a conjugate pair at ±16.38°. Pole radius rises toward 1 as the corner frequency falls relative to the sample rate — the same filter at 192 kHz sits at 0.9599411 and at 8 kHz at 0.6066675. 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 2.5 kHz corner as every other filter type.
- Low-pass2.5 kHz
- High-pass2.5 kHz
- Band-pass2.5 kHz
- All-pass2.5 kHz
- Peaking EQ2.5 kHz
- Low shelf2.5 kHz
- High shelf2.5 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 −∞ dB at 2.5 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.