1.6 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 (1.6 kHz)
−∞ dB
exact at every sample rate — the bilinear transform maps this value, not just the frequency
Pole radius at 48 kHz
0.9009254
conjugate pair at ±10.43°, 0.0991 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 0.9009137 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 1.6 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 | 0.677723 | -0.418856 | 0.677723 | -0.418856 | 0.355447 | 0.596194 | 40.0% |
| 16 kHz | 0.772862 | -1.250516 | 0.772862 | -1.250516 | 0.545723 | 0.738731 | 20.0% |
| 22.1 kHz | 0.819574 | -1.471718 | 0.819574 | -1.471718 | 0.639149 | 0.799468 | 14.5% |
| 32 kHz | 0.866169 | -1.647552 | 0.866169 | -1.647552 | 0.732339 | 0.855768 | 10.0% |
| 44.1 kHz | 0.898476 | -1.750463 | 0.898476 | -1.750463 | 0.796952 | 0.892721 | 7.3% |
| 48 kHz | 0.905833 | -1.772077 | 0.905833 | -1.772077 | 0.811667 | 0.900925 | 6.7% |
| 96 kHz | 0.950332 | -1.890251 | 0.950332 | -1.890251 | 0.900663 | 0.949033 | 3.3% |
| 192 kHz | 0.974499 | -1.946328 | 0.974499 | -1.946328 | 0.948999 | 0.974166 | 1.7% |
const float b0 = 0.90583333f, b1 = -1.77207740f, b2 = 0.90583333f;
const float a1 = -1.77207740f, a2 = 0.81166666f; // 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 | — | 0.9009254 | 0.9009254 | yes | reference |
| float32 | — | 0.9009255 | 0.9009255 | yes | 0.0021 dB |
| 32-bit fixed | Q1.30 | 0.9009254 | 0.9009254 | yes | 0.0000 dB |
| 24-bit fixed | Q1.22 | 0.9009255 | 0.9009255 | yes | 0.0020 dB |
| 16-bit fixed | Q1.14 | 0.9009137 | 0.9009137 | yes | 0.7809 dB |
What Q does at 1.6 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 | 3797 Hz | 0.809784 | -156.150 ms |
| 0.7071 | −∞ dB | 0.00 dB @ 24.00 kHz | 3061 Hz | 0.862354 | -156.108 ms |
| 1 | −∞ dB | 0.00 dB @ 24.00 kHz | 2574 Hz | 0.900925 | -156.050 ms |
| 2 | −∞ dB | 0.00 dB @ 24.00 kHz | 2044 Hz | 0.949305 | -155.849 ms |
| 4 | −∞ dB | 0.00 dB @ 24.00 kHz | 1811 Hz | 0.974340 | -155.448 ms |
| 10 | −∞ dB | 0.00 dB @ 24.00 kHz | 1681 Hz | 0.989658 | -154.246 ms |
Questions this filter answers
What are the biquad coefficients for a 1.6 kHz notch filter at 48 kHz?
b0 = 0.905833, b1 = -1.772077, b2 = 0.905833, a1 = -1.772077, a2 = 0.811667, 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 1.6 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 0.9009137, against 0.9009254 exact, and the response drifts by at most 0.781 dB inside the band. 24-bit takes that to 0.0020 dB.
Where is the real −3 dB point of a 1.6 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 1.6 kHz notch filter?
0.9009254 at 48 kHz, as a conjugate pair at ±10.43°. Pole radius rises toward 1 as the corner frequency falls relative to the sample rate — the same filter at 192 kHz sits at 0.9741656 and at 8 kHz at 0.5961936. 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 1.6 kHz corner as every other filter type.
- Low-pass1.6 kHz
- High-pass1.6 kHz
- Band-pass1.6 kHz
- All-pass1.6 kHz
- Peaking EQ1.6 kHz
- Low shelf1.6 kHz
- High shelf1.6 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 1.6 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.