Computed

400 Hz high-pass

Rejects everything below the corner at 12 dB/octave and passes what is above it. Solved at 8 sample rates, with the poles, the real −3 dB point and the word length it stops working at.

Open the interactive designer →All high-pass frequencies

Magnitude response at 48 kHz

Every vertex is 20·log₁₀|H(e^jω)| 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 (400 Hz)

−3.01 dB

exact at every sample rate — the bilinear transform maps this value, not just the frequency

Pole radius at 48 kHz

0.9636530

conjugate pair at ±2.12°, 0.0363 from the circle

−3 dB point

400.0 Hz

1.000× f0 at Q = 0.7071

16-bit fixed point

holds

largest pole 0.9636648 in Q1.14

Coefficients, at every sample rate

The cookbook computes w₀ = 2πf₀/F_s, so the same filter is a different set of numbers at every rate. Rates whose Nyquist limit is at or below 400 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	0.800592	-1.601185	0.800592	-1.561018	0.641352	0.800844	10.0%
16 kHz	0.894859	-1.789717	0.894859	-1.778632	0.800803	0.894876	5.0%
22.1 kHz	0.922561	-1.845123	0.922561	-1.839117	0.851128	0.922566	3.6%
32 kHz	0.945977	-1.891954	0.945977	-1.889033	0.894874	0.945978	2.5%
44.1 kHz	0.960503	-1.921005	0.960503	-1.919445	0.922566	0.960503	1.8%
48 kHz	0.963653	-1.927306	0.963653	-1.925984	0.928627	0.963653	1.7%
96 kHz	0.981658	-1.963317	0.981658	-1.962980	0.963653	0.981658	0.8%
192 kHz	0.990787	-1.981573	0.990787	-1.981489	0.981658	0.990787	0.4%

const float b0 = 0.96365276f, b1 = -1.92730553f, b2 = 0.96365276f;
const float a1 = -1.92598397f, a2 = 0.92862709f;   // a0 == 1

What 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	—	0.9636530	0.9636530	yes	reference
float32	—	0.9636530	0.9636530	yes	0.0002 dB
32-bit fixed	Q1.30	0.9636530	0.9636530	yes	0.0003 dB
24-bit fixed	Q1.22	0.9636530	0.9636530	yes	0.0765 dB
16-bit fixed	Q1.14	0.9636648	0.9636648	yes	10.0909 dB

What Q does at 400 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	−6.02 dB	0.00 dB @ 24.00 kHz	621.3 Hz	0.948965	0.398 ms
0.7071	−3.01 dB	0.00 dB @ 24.00 kHz	400.0 Hz	0.963653	0.563 ms
1	0.00 dB	+1.25 dB @ 567 Hz	342.3 Hz	0.974166	0.796 ms
2	+6.02 dB	+6.29 dB @ 423 Hz	640.2 Hz	0.987000	1.592 ms
4	+12.04 dB	+12.09 dB @ 410 Hz	471.4 Hz	0.993479	3.184 ms
10	+20.00 dB	+19.79 dB @ 396 Hz	424.0 Hz	0.997387	7.960 ms

Questions this filter answers

What are the biquad coefficients for a 400 Hz high-pass filter at 48 kHz?

b0 = 0.963653, b1 = -1.927306, b2 = 0.963653, a1 = -1.925984, a2 = 0.928627, with a0 normalised to 1 — the RBJ Audio EQ Cookbook form at Q = 0.7071. 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 400 Hz high-pass filter stable in 16-bit fixed point?

Yes. Rounding the five coefficients to a shared 1.14 scale leaves the largest pole at 0.9636648, against 0.9636530 exact, and the response drifts by at most 10.091 dB inside the band. 24-bit takes that to 0.0765 dB.

Where is the real −3 dB point of a 400 Hz high-pass filter?

400.0 Hz, which is 1.000× the 400 Hz 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 the Q sweep above shows the point moving from 621.3 Hz to 424.0 Hz across the sweep while f0 never moves.

How close to the unit circle are the poles of a 400 Hz high-pass filter?

0.9636530 at 48 kHz, as a conjugate pair at ±2.12°. Pole radius rises toward 1 as the corner frequency falls relative to the sample rate — the same filter at 192 kHz sits at 0.9907867 and at 8 kHz at 0.8008443. 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 400 Hz corner as every other filter type.

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 −3.01 dB at 400 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.