Say how the devices and environment measurements are made - #513
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B12, B13, B14 and B17: 215 findings closed, 22 open. Message to be rewritten before the PR.
Twenty-five Spanish pages brought level with the English of this branch: the acquisition sections, forty new plates and plots with their Spanish variants, and the corrected numbers. The terminology was settled before this ran, so it was applied rather than decided: apartado, hoja de características, desviación típica, incertidumbre expandida, método de control for the survey method, and the four terms that are recast rather than named. The checker reports no warnings. One error is corrected in both editions rather than mirrored. The English said the absorption area and the room constant "coincide for a dead room", where they differ by 10 lg[1/(1-alpha)]: that is zero when alpha tends to zero, which is a live room, and it grows with absorption. The page's own numbers, 0.5 dB at alpha = 0.1 and 3.0 dB at 0.5, say so two lines further down. The translation carried it over deliberately to keep parity and flagged it, which is how it was found.
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📝 WalkthroughWalkthroughThe pull request substantially expands acoustics documentation, diagrams, figure generators, registries, generated reference text, and Spanish translations. It covers noise control, electroacoustics, sound-power methods, environmental propagation, source models, assessment workflows, and measurement standards. ChangesDocumentation and visualization expansion
Estimated code review effort: 5 (Critical) | ~120 minutes Possibly related PRs
Suggested labels: Poem
🚥 Pre-merge checks | ✅ 5✅ Passed checks (5 passed)
✨ Finishing Touches📝 Generate docstrings
🧪 Generate unit tests (beta)
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Codecov Report✅ All modified and coverable lines are covered by tests. Additional details and impacted files@@ Coverage Diff @@
## main #513 +/- ##
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Files 295 295
Lines 39146 39146
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Hits 37992 37992
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Actionable comments posted: 49
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⚠️ Outside diff range comments (2)
site/src/content/docs/devices/emission/sound-power-intensity.mdx (1)
629-631: 📐 Maintainability & Code Quality | 🟡 Minor | ⚡ Quick winStale "five determination routes" in six "See also" lists. This PR raised the documented route count from five to six in the body text and coverage sections of every emission guide, but the "See also" bullets that link to the Sound Power chooser still state five. The shared root cause is one missed edit class.
site/src/content/docs/devices/emission/sound-power-intensity.mdx#L629-L631: change "choosing among the five determination routes" to six.site/src/content/docs/devices/emission/sound-power-pressure.mdx#L848-L850: change "choosing among the five determination routes" to six.site/src/content/docs/devices/emission/sound-power-reverberation.mdx#L477-L479: change "choosing among the five determination routes" to six.site/src/content/docs/es/devices/emission/sound-power-intensity.mdx#L662-L664: change "las cinco vías de determinación" to "las seis vías de determinación".site/src/content/docs/es/devices/emission/sound-power-pressure.mdx#L881-L883: change "las cinco vías de determinación" to "las seis vías de determinación".site/src/content/docs/es/devices/emission/sound-power-reverberation.mdx#L500-L502: change "las cinco vías de determinación" to "las seis vías de determinación".🤖 Prompt for AI Agents
Verify each finding against current code. Fix only still-valid issues, skip the rest with a brief reason, keep changes minimal, and validate. In `@site/src/content/docs/devices/emission/sound-power-intensity.mdx` around lines 629 - 631, Update the Sound Power chooser “See also” bullet to reflect six determination routes in all affected files: site/src/content/docs/devices/emission/sound-power-intensity.mdx (629-631), sound-power-pressure.mdx (848-850), and sound-power-reverberation.mdx (477-479); update the Spanish wording to “las seis vías de determinación” in site/src/content/docs/es/devices/emission/sound-power-intensity.mdx (662-664), sound-power-pressure.mdx (881-883), and sound-power-reverberation.mdx (500-502).site/public/llms/llms-devices-noise-control.txt (1)
758-758: 🗄️ Data Integrity & Integration | 🟠 Major | ⚡ Quick winRegenerate the generated LLMS shard for this change.
llms-devices-noise-control.txtstill contains stale text that the source MDX documents no longer have and can omit content that the MDX documents now include:
ReactiveSilencerResult now reportsin the shard;duct-path.mdxsaysEvery ReactiveSilencerResult reports.- Missing
## 3. How a silencer is measured (ISO 7235)and the nearby hardware limitation paragraph fromsilencers.mdx.Generate the artifact with
make llmsinstead.🤖 Prompt for AI Agents
Verify each finding against current code. Fix only still-valid issues, skip the rest with a brief reason, keep changes minimal, and validate. In `@site/public/llms/llms-devices-noise-control.txt` at line 758, Regenerate the generated LLMS artifact using make llms so llms-devices-noise-control.txt reflects the current duct-path.mdx and silencers.mdx content, including the updated “Every ReactiveSilencerResult reports” wording and the missing ISO 7235 section with its hardware limitation paragraph.
🤖 Prompt for all review comments with AI agents
Verify each finding against current code. Fix only still-valid issues, skip the
rest with a brief reason, keep changes minimal, and validate.
Inline comments:
In `@docs/devices/noise-control/noise-control.md`:
- Line 248: In the installation guidance near “Cooling openings,” hyphenate the
compound modifier by changing “short lined ducts” to “short-lined ducts.”
In `@docs/devices/noise-control/silencers.md`:
- Around line 308-310: Update the sentence around the modal filter requirements
so both the 3 dB fundamental attenuation and the 5 dB above-cut-on attenuation
limits apply to the fundamental mode, rather than assigning the 5 dB limit to
higher-order modes; preserve the existing loudspeaker and substitution-duct
requirements.
- Around line 283-286: Update the expansion_chamber example around freqs and
res.report to ensure every reported frequency is below the chamber’s computed
plane_wave_limit. Either restrict the frequency grid accordingly or adjust the
chamber geometry so the limit exceeds 4000 Hz, then regenerate the fiche output.
- Around line 302-307: Reverse the insertion-loss equation in the “What that
fiche is not” section so it computes substitution-duct level minus test-object
level, using the existing series II and series I labels respectively: D_i =
L_pII - L_pI.
In `@llms-full.txt`:
- Around line 17569-17580: Update render_reactive_silencer_report() so mean
transmission loss, peak transmission loss, and the PASS/FAIL verdict use only
frequencies at or below result.plane_wave_limit, or explicitly mark out-of-range
bands and exclude them from these aggregates. Regenerate the reactive-silencer
fiche with the corrected plane-wave-filtered results while preserving the
existing in-range reporting.
In `@scripts/diagrams/environment.py`:
- Around line 786-799: Update the two vertical source-height dimensions in the
diagram around ay, by, and their s.dim calls to include the same “out of scale”
annotation already used by the gauge dimension, while preserving their existing
labels, geometry, and styling.
- Line 819: Remove the s.circle call at the diagram-generation site so generated
SVGs no longer include the unused 0.1 px marker, leaving surrounding rendering
logic unchanged.
- Around line 711-723: Update the equivalent point-source position in the
diagram from rx0 + 5.5 * seg to rx0 + 6 * seg, including the hx assignment used
by the x = 60 m dimension and witness line. Keep the existing dL = 20 m segment
geometry and junction position unchanged so the dimension spans three segments
consistently.
In `@scripts/diagrams/i18n.py`:
- Around line 96-97: The Spanish translation for the key “1 — the day, split
into evaluation periods (Annex I A.1)” uses the inconsistent reference “Anexo I
A.2”; update that value to reference “Anexo I A.1” while preserving the rest of
the translation.
- Around line 16-119: Add Spanish entries for all six diagram title strings to
the translation map used by render(), _ES, so _ES.get(title, title) returns
Spanish titles instead of the English fallback. Keep the existing translation
style and place each title with its corresponding diagram section.
- Around line 2461-2463: Update the translations for the ⟨v_j²⟩ label and the
following “normal velocity, same bands” label so they preserve the
surface-averaged squared normal-velocity meaning, including “normal velocity” in
the second label and retaining the squared quantity in the first.
In `@scripts/figures/environment.py`:
- Around line 974-976: Update the docstring of
generate_iso9613_screening_anatomy to remove Kmet from its summary, so it
describes only the plotted caps and spent ground effect.
- Around line 1577-1578: Update the fixed-band marker in the plotting code near
the `left.plot` call so its geometry matches the “9.5.3: fixed 20-120 Hz band”
label: either extend the segment endpoint to 120 Hz or change it to a single
marker at the 70 Hz centre frequency, preserving the existing styling and label.
- Around line 1456-1463: Update the plotting loop around railway_source_power to
compute and retain each speed’s result once, then build each row’s plotted
values by indexing the cached results rather than invoking railway_source_power
separately for row 0 and row 1.
- Around line 1175-1198: Extend the `gradients` range in the plotting code so it
includes `grad_log` (approximately 0.4615), while preserving the existing curve
generation and marker placement. Ensure the second marker and annotation fall
within the swept curves and the plotted x-axis range matches the documented Rc
coverage.
In `@site/src/content/docs/devices/broadcast/program-loudness.mdx`:
- Around line 424-428: Correct the mathematically incorrect worst-case
explanation in site/src/content/docs/devices/broadcast/program-loudness.mdx
lines 424-428 by replacing the maximisation claim with the fact that a tone at
fs/4 can be phased so every sample lands at 1/√2. Apply the same translated
correction in site/src/content/docs/es/devices/broadcast/program-loudness.mdx
lines 436-441; no other changes are needed.
In `@site/src/content/docs/devices/electroacoustics/electroacoustics.mdx`:
- Line 33: Update the note near the Bendat & Piersol ISBN to cite chapter 6
instead of section/chapter 5, and revise any reused Bendat & Piersol references
in the swept-sine guide to use chapter 6 consistently.
- Around line 123-127: Update the electroacoustics documentation to use the
default n_harmonics order count and consistently describe the same ordered
harmonic list. Correct the 48 kHz, 7 kHz example to account for the plot loop
stopping at the first harmonic exceeding Nyquist, while preserving the
explanation that only below-Nyquist harmonics contribute to THD.
- Around line 410-415: Correct the electroacoustic reference explanation so the
combined-reference ratio is stated as d′ₘ = dₘ/5 when the denominator is a_f₁ +
a_f₂ = 5a_f₂. Update the corresponding dB comparison to say the
combined-reference datasheet value is 14 dB lower than the f₂-referenced value
returned by the function, and remove the incorrect multiplication and “five
times” wording.
In `@site/src/content/docs/devices/electroacoustics/loudspeakers.mdx`:
- Around line 732-736: Replace the dangling “Those two special cases” reference
with a direct introduction naming Long’s two special cases and Eqs. (18.21) and
(18.22) in
site/src/content/docs/devices/electroacoustics/loudspeakers.mdx:732-736. Apply
the equivalent Spanish wording, «Long da dos casos particulares (ecs. (18.21) y
(18.22))», in
site/src/content/docs/es/devices/electroacoustics/loudspeakers.mdx:762-766.
In `@site/src/content/docs/devices/emission/sound-power-pressure.mdx`:
- Around line 315-320: Make every listed standalone figure block self-contained
by adding the requested imports:
site/src/content/docs/devices/emission/sound-power-pressure.mdx lines 315-320
add emission, lines 559-569 add emission and plot_microphone_positions;
intensity.mdx lines 625-653 add emission; sound-power-intensity.mdx lines
348-352 add emission; sound-power-reverberation.mdx lines 276-285 add numpy;
sound-power.mdx lines 264-274 add emission; vibration-sound-power.mdx lines
307-321 add numpy and vibration; and the corresponding Spanish blocks at
intensity.mdx lines 654-657, sound-power-intensity.mdx lines 366-370,
sound-power-pressure.mdx lines 325-330, sound-power-reverberation.mdx lines
286-296, and sound-power.mdx lines 278-282 add their specified imports. In the
Spanish sound-power-pressure.mdx block at lines 580-591, also pass language="es"
to both plot_microphone_positions calls; the Spanish vibration-sound-power.mdx
block at lines 318-328 requires numpy and vibration imports.
In `@site/src/content/docs/devices/emission/vibration-sound-power.mdx`:
- Around line 225-231: Update the extraneous-correction snippets in
site/src/content/docs/devices/emission/vibration-sound-power.mdx:225-231 and
site/src/content/docs/es/devices/emission/vibration-sound-power.mdx:231-237 so
their output comments match the shadowed six-band lv value, changing the English
comment to 78.2 dB after the correction and the Spanish comment to 78.2 dB tras
la corrección; no direct code change is required.
In `@site/src/content/docs/devices/noise-control/duct-path.mdx`:
- Around line 277-281: The claim about analysis bands applies only to models
returning HvacSpectrumResult; revise the English text to explicitly exclude the
scalar helpers split_loss, plenum_attenuation, and equivalent_diameter. Make the
same clarification in the Spanish sentence “Todos toman las bandas de análisis
como primer argumento” in
site/src/content/docs/es/devices/noise-control/duct-path.mdx at lines 288-292;
no other sections require changes.
- Around line 236-242: Correct the fan-efficiency caption so its 12 dB example
matches the figure’s 55% operating point: update
site/src/content/docs/devices/noise-control/duct-path.mdx lines 236-242 to
describe a fan running at 55% of peak static efficiency, and apply the
equivalent correction to
site/src/content/docs/es/devices/noise-control/duct-path.mdx lines 246-253. Do
not change the surrounding staircase or figure content.
In `@site/src/content/docs/devices/noise-control/noise-control.mdx`:
- Around line 226-231: The Wells outlet-angle value is incorrect in both
language editions. In
site/src/content/docs/devices/noise-control/noise-control.mdx lines 226-231,
replace 1.8 dB with the recomputed 1.59 dB (or explicitly state the baseline
angle that produces 1.8 dB); apply the same correction to “1,8 dB” in
site/src/content/docs/es/devices/noise-control/noise-control.mdx lines 236-239.
- Around line 339-341: The wording in both noise-control documents incorrectly
refers to “the figure”; explicitly identify the worked enclosure_insertion_loss
snippet as the source of the stated values. Update
site/src/content/docs/devices/noise-control/noise-control.mdx lines 339-341 and
site/src/content/docs/es/devices/noise-control/noise-control.mdx lines 354-356,
making the equivalent English and Spanish wording changes without altering the
calculations.
In `@site/src/content/docs/devices/noise-control/room-to-room.mdx`:
- Around line 286-290: Correct the warning in both editions: in
site/src/content/docs/devices/noise-control/room-to-room.mdx lines 286-290,
state that substituting A for R on the source side over-predicts both room
levels without changing NR, while substituting R for A2 on the receiving side
over-predicts noise reduction; apply the equivalent correction in
site/src/content/docs/es/devices/noise-control/room-to-room.mdx lines 294-297,
preserving the existing bilingual explanations.
In `@site/src/content/docs/devices/noise-control/silencers.mdx`:
- Around line 678-693: Update the selection-figure snippets in
site/src/content/docs/devices/noise-control/silencers.mdx:678-693 and
site/src/content/docs/es/devices/noise-control/silencers.mdx:710-725 to use a
wider frequency sweep, such as np.geomspace(40.0, 8000.0, 4000), and recompute
both the expansion chamber and Helmholtz branch results on that grid before
applying the plane-wave filter.
- Around line 129-135: The expansion-chamber area-ratio claim is incorrect in
both editions. In site/src/content/docs/devices/noise-control/silencers.mdx
lines 129-135, change the statement so doubling the chamber cross-section is
worth about 6 dB, or state that quadrupling is worth about 11 dB; apply the
equivalent correction to
site/src/content/docs/es/devices/noise-control/silencers.mdx lines 133-139,
preserving the surrounding explanation.
In `@site/src/content/docs/environment/assessment/environmental-levels.mdx`:
- Around line 286-289: Remove the redundant shorter ISO 1996-2:2007 Annex C.5
reference immediately after the explanatory provenance comment, preserving the
detailed comment and worked example unchanged.
In `@site/src/content/docs/environment/assessment/impulsive-sound.mdx`:
- Around line 227-236: Update the introductory sentence above the
keyword-argument table to account for all five documented arguments, and remove
or revise the claim that none is optional in practice so it does not apply to
situational options such as reference_pressure and onset_rate_method. Keep the
existing argument descriptions and defaults unchanged.
In `@site/src/content/docs/environment/assessment/spanish-noise-regulation.mdx`:
- Around line 199-219: Update the “Show the code for this figure” block so it no
longer claims to reproduce the two-panel bar comparison: rename the summary to
reflect that it only reports values, remove the unused matplotlib import and
plt.show() call, and preserve the existing printed comparison.
- Around line 188-197: Update the 250 Hz example in the paragraph to state that
the survey method raises no flag because the band does not exceed both
neighbours by 8 dB: it exceeds the 200 Hz neighbour by exactly 8 dB but the 315
Hz neighbour by only 7 dB. Preserve the surrounding comparison of the RD,
survey, and Annex C methods.
In `@site/src/content/docs/environment/propagation/atmospheric-refraction.mdx`:
- Around line 450-453: Both editions refer to two validation figures, but only
the homogeneous-limit figure is present. In
site/src/content/docs/environment/propagation/atmospheric-refraction.mdx:450-453,
narrow the sentence to identify only the homogeneous-limit validation, and apply
the equivalent wording change to
site/src/content/docs/es/environment/propagation/atmospheric-refraction.mdx:472-473;
do not add a ray-geometry figure.
- Around line 151-156: Correct the wind-component convention in both
atmospheric-refraction passages so the displayed formula and worked values
agree: update the English text at
site/src/content/docs/environment/propagation/atmospheric-refraction.mdx:151-156
and the translated text at
site/src/content/docs/es/environment/propagation/atmospheric-refraction.mdx:160-165
to explicitly define the angle/sign convention or measure the angle from the
propagation direction, preserving the resulting +0.43 m/s downwind and -0.43 m/s
upwind values.
- Around line 148-149: Update the log_linear_sound_speed_profile example call to
explicitly pass ground_speed=340.0 while preserving the assertion that it
returns 344.0 m/s at 10 m.
In `@site/src/content/docs/environment/propagation/ground-barriers.mdx`:
- Line 179: The alt text at
site/src/content/docs/environment/propagation/ground-barriers.mdx:179 must
describe only output from generate_ground_reflection_coefficient, removing the
phase-curve and secondary |F(w)| axis claims. At
site/src/content/docs/environment/propagation/ground-barriers.mdx:374, update
the alt text for _d_barrier_four_paths to remove the side-panel path-length and
path-length-difference claims, while retaining its route legend and
thick-barrier inset. At
site/src/content/docs/es/environment/sources/cnossos-rail-emission.mdx:95,
update the _d_cnossos_rail alt text to remove claims that the diagram dimensions
the 25 m receiver distance or shades the lower half-space.
- Around line 516-519: Update the opening sentence in the barrier-model caveat
to refer to all three models, matching the three models named in the section and
the later “Both models” wording.
In `@site/src/content/docs/environment/sources/wind-turbine-noise.mdx`:
- Around line 67-74: Align the microphone-mounting geometry across both language
versions: in site/src/content/docs/environment/sources/wind-turbine-noise.mdx
lines 67-74, update the “Microphone diaphragm” row to match the figure alt
text’s diaphragm-in-board-plane geometry and re-check the split-board
requirement; in
site/src/content/docs/es/environment/sources/wind-turbine-noise.mdx lines 69-74,
apply the same correction to the alt text and “Diafragma del micrófono” row,
ensuring both split-board descriptions remain consistent.
- Around line 211-221: The audibility-criterion alt text reverses the frequency
dependence. Update the English alt text in
site/src/content/docs/environment/sources/wind-turbine-noise.mdx lines 211-221
and the Spanish alt text in
site/src/content/docs/es/environment/sources/wind-turbine-noise.mdx lines
222-233 so they state that the 1 kHz tone requires more emergence than the 100
Hz tone, by about 0.8 dB, while preserving the rest of the descriptions.
In `@site/src/content/docs/es/devices/electroacoustics/electroacoustics.mdx`:
- Around line 364-373: Corrige la explicación en el párrafo sobre 997 Hz:
elimina la afirmación de que es inconmensurable o que el tono nunca se repite, y
explica que la secuencia muestreada se repite tras 48 000 muestras a 48 kHz o 44
100 muestras a 44,1 kHz. Conserva la comparación con 1000 Hz indicando que la
ventaja de 997 Hz es su periodo discreto mucho más largo, y que n = fs contiene
exactamente un periodo completo.
- Around line 565-568: Corrige el texto alrededor de “transfer_function” para no
afirmar que un retardo fijo sin compensar reduce $\gamma^2$ ni que alargar el
segmento de Welch lo soluciona. Indica que el retardo fijo solo inclina la fase
de $H_1$ en una medición LTI ideal; atribuye una caída de coherencia a
desincronización de relojes, retardos variables entre segmentos, transitorios,
no linealidad o promediado insuficiente.
- Around line 241-245: Reemplaza la comparación de razones THD en el flujo que
calcula residual por una comparación entre tensiones RMS: calcula el residuo del
generador usando idle - signal, conservando el fundamental o la inyección del
generador según corresponda, y calcula el RMS de la distorsión en la misma banda
a partir de thd_f. Acepta el método solo cuando el RMS residual sea menor que un
tercio del RMS de distorsión; si no, conserva la bajada a harmonic_distortion.
In `@site/src/content/docs/es/devices/emission/intensity.mdx`:
- Line 408: En el encabezado “Medir el índice residual, y comprobar la sonda”,
añade un span vacío con el id ASCII
“medir-el-indice-residual-y-comprobar-la-sonda” para garantizar que el enlace
profundo funcione independientemente del slug generado por Astro.
In `@site/src/content/docs/es/environment/assessment/impulsive-sound.mdx`:
- Around line 230-239: Corrige el encabezado introductorio de esta sección para
que coincida con los cinco argumentos enumerados en la tabla (`dt`,
`calibration_offset`, `laeq`, `reference_pressure` y `onset_rate_method`), o
separa explícitamente los tres argumentos determinantes de los otros dos sin
alterar la tabla.
In
`@site/src/content/docs/es/environment/assessment/spanish-noise-regulation.mdx`:
- Around line 191-201: Reformula el párrafo alrededor del ejemplo de 250 Hz para
indicar que el indicador no se activa porque la banda supera a la vecina de 315
Hz en solo 7 dB; no atribuyas el resultado a superar a cada vecina en menos de 8
dB. Mantén explícita la condición del criterio de cribado para la diferencia
exacta de 8 dB respecto a la vecina de 200 Hz, usando la comparación definida
por el método.
In `@site/src/content/docs/es/environment/propagation/ground-barriers.mdx`:
- Around line 532-536: Corrige el recuento en el párrafo que comienza con “Los
cuatro modelos” para indicar que son tres modelos, manteniendo sin cambios la
explicación sobre pantallas bidimensionales infinitas y los efectos no
representados.
In `@site/src/content/docs/es/environment/propagation/outdoor-propagation.mdx`:
- Around line 774-781: Update the output comment following the loop to use
periods as decimal separators, matching Python’s print output and the file’s
other documented examples; change only the four documented values.
In `@site/src/content/docs/reference/bibliography.md`:
- Around line 978-983: Merge the duplicate Attenborough and Van Renterghem
citation into the existing English entry at
site/src/content/docs/reference/bibliography.md lines 904-909, incorporating its
chapter coverage, ISBNs, and guide links, then remove the duplicate at lines
978-983. Apply the same merge to the existing Spanish entry at
site/src/content/docs/es/reference/bibliography.md lines 946-952, incorporating
the duplicate content and removing the duplicate at lines 1023-1030; retain one
entry per language.
---
Outside diff comments:
In `@site/public/llms/llms-devices-noise-control.txt`:
- Line 758: Regenerate the generated LLMS artifact using make llms so
llms-devices-noise-control.txt reflects the current duct-path.mdx and
silencers.mdx content, including the updated “Every ReactiveSilencerResult
reports” wording and the missing ISO 7235 section with its hardware limitation
paragraph.
In `@site/src/content/docs/devices/emission/sound-power-intensity.mdx`:
- Around line 629-631: Update the Sound Power chooser “See also” bullet to
reflect six determination routes in all affected files:
site/src/content/docs/devices/emission/sound-power-intensity.mdx (629-631),
sound-power-pressure.mdx (848-850), and sound-power-reverberation.mdx (477-479);
update the Spanish wording to “las seis vías de determinación” in
site/src/content/docs/es/devices/emission/sound-power-intensity.mdx (662-664),
sound-power-pressure.mdx (881-883), and sound-power-reverberation.mdx (500-502).
🪄 Autofix
Fix all unresolved CodeRabbit comments on this PR:
- Push a commit to this branch (recommended)
- Create a new PR with the fixes
ℹ️ Review info
⚙️ Run configuration
Configuration used: Organization UI
Review profile: ASSERTIVE
Plan: Pro Plus
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📒 Files selected for processing (61)
docs/devices/noise-control/noise-control.mddocs/devices/noise-control/silencers.mdllms-full.txtscripts/diagrams/devices.pyscripts/diagrams/environment.pyscripts/diagrams/i18n.pyscripts/diagrams/registry.pyscripts/figures/devices.pyscripts/figures/environment.pyscripts/figures/registry.pysite/public/llms/llms-devices-noise-control.txtsite/src/content/docs/devices/broadcast/program-loudness.mdxsite/src/content/docs/devices/electroacoustics/electroacoustics.mdxsite/src/content/docs/devices/electroacoustics/loudspeakers.mdxsite/src/content/docs/devices/electroacoustics/microphones.mdxsite/src/content/docs/devices/electroacoustics/swept-sine-distortion.mdxsite/src/content/docs/devices/emission/intensity.mdxsite/src/content/docs/devices/emission/sound-power-intensity.mdxsite/src/content/docs/devices/emission/sound-power-pressure.mdxsite/src/content/docs/devices/emission/sound-power-reverberation.mdxsite/src/content/docs/devices/emission/sound-power.mdxsite/src/content/docs/devices/emission/vibration-sound-power.mdxsite/src/content/docs/devices/noise-control/duct-path.mdxsite/src/content/docs/devices/noise-control/noise-control.mdxsite/src/content/docs/devices/noise-control/room-to-room.mdxsite/src/content/docs/devices/noise-control/silencers.mdxsite/src/content/docs/environment/assessment/environmental-levels.mdxsite/src/content/docs/environment/assessment/impulsive-sound.mdxsite/src/content/docs/environment/assessment/spanish-noise-regulation.mdxsite/src/content/docs/environment/propagation/atmospheric-refraction.mdxsite/src/content/docs/environment/propagation/ground-barriers.mdxsite/src/content/docs/environment/propagation/outdoor-propagation.mdxsite/src/content/docs/environment/sources/cnossos-rail-emission.mdxsite/src/content/docs/environment/sources/cnossos-road-emission.mdxsite/src/content/docs/environment/sources/wind-turbine-noise.mdxsite/src/content/docs/es/devices/broadcast/program-loudness.mdxsite/src/content/docs/es/devices/electroacoustics/electroacoustics.mdxsite/src/content/docs/es/devices/electroacoustics/loudspeakers.mdxsite/src/content/docs/es/devices/electroacoustics/microphones.mdxsite/src/content/docs/es/devices/electroacoustics/swept-sine-distortion.mdxsite/src/content/docs/es/devices/emission/intensity.mdxsite/src/content/docs/es/devices/emission/sound-power-intensity.mdxsite/src/content/docs/es/devices/emission/sound-power-pressure.mdxsite/src/content/docs/es/devices/emission/sound-power-reverberation.mdxsite/src/content/docs/es/devices/emission/sound-power.mdxsite/src/content/docs/es/devices/emission/vibration-sound-power.mdxsite/src/content/docs/es/devices/noise-control/duct-path.mdxsite/src/content/docs/es/devices/noise-control/noise-control.mdxsite/src/content/docs/es/devices/noise-control/room-to-room.mdxsite/src/content/docs/es/devices/noise-control/silencers.mdxsite/src/content/docs/es/environment/assessment/environmental-levels.mdxsite/src/content/docs/es/environment/assessment/impulsive-sound.mdxsite/src/content/docs/es/environment/assessment/spanish-noise-regulation.mdxsite/src/content/docs/es/environment/propagation/atmospheric-refraction.mdxsite/src/content/docs/es/environment/propagation/ground-barriers.mdxsite/src/content/docs/es/environment/propagation/outdoor-propagation.mdxsite/src/content/docs/es/environment/sources/cnossos-rail-emission.mdxsite/src/content/docs/es/environment/sources/cnossos-road-emission.mdxsite/src/content/docs/es/environment/sources/wind-turbine-noise.mdxsite/src/content/docs/es/reference/bibliography.mdsite/src/content/docs/reference/bibliography.md
| the mean insertion loss from 28.9 dB to 21.4 dB, and adding a 0.24 m² gap at the | ||
| door foot takes it to 15.1 dB. `composite_transmission_loss(areas, | ||
| reduction_indices)` builds that composite and `enclosure_insertion_loss` takes | ||
| its result directly as the panel $R$. Cooling openings become short lined ducts |
There was a problem hiding this comment.
📐 Maintainability & Code Quality | 🟡 Minor | ⚡ Quick win
Hyphenate the compound modifier.
Change short lined ducts to short-lined ducts so the installation guidance is parsed consistently.
🧰 Tools
🪛 LanguageTool
[grammar] ~248-~248: Use a hyphen to join words.
Context: ...panel
(QB_NEW_EN_HYPHEN)
🤖 Prompt for AI Agents
Verify each finding against current code. Fix only still-valid issues, skip the
rest with a brief reason, keep changes minimal, and validate.
In `@docs/devices/noise-control/noise-control.md` at line 248, In the installation
guidance near “Cooling openings,” hyphenate the compound modifier by changing
“short lined ducts” to “short-lined ducts.”
Source: Linters/SAST tools
Comment on lines
+283
to
+286
| # A 0.5 m chamber of area ratio m = 8, at the octave-band centres. | ||
| freqs = np.array([63.0, 125.0, 250.0, 500.0, 1000.0, 2000.0, 4000.0]) | ||
| res = expansion_chamber(freqs, length=0.5, chamber_area=0.08, pipe_area=0.01) | ||
| res.report( |
There was a problem hiding this comment.
🎯 Functional Correctness | 🟠 Major | ⚡ Quick win
Keep the report frequencies below plane_wave_limit.
The preceding text states that frequencies above the first higher-order cut-on are invalid. This example analyzes the 0.08 m² chamber through 4000.0 Hz, so it likely reports above-cut-on peaks and troughs. The larger chamber area also lowers the cut-on frequency relative to the earlier 0.04 m² example. Use a frequency grid below the computed limit, or choose geometry with a limit above 4 kHz, then regenerate the fiche. (iteh.eu)
Suggested correction
- freqs = np.array([63.0, 125.0, 250.0, 500.0, 1000.0, 2000.0, 4000.0])
+ freqs = np.array([63.0, 125.0, 250.0, 500.0]) # verify against plane_wave_limit📝 Committable suggestion
‼️ IMPORTANT
Carefully review the code before committing. Ensure that it accurately replaces the highlighted code, contains no missing lines, and has no issues with indentation. Thoroughly test & benchmark the code to ensure it meets the requirements.
Suggested change
| # A 0.5 m chamber of area ratio m = 8, at the octave-band centres. | |
| freqs = np.array([63.0, 125.0, 250.0, 500.0, 1000.0, 2000.0, 4000.0]) | |
| res = expansion_chamber(freqs, length=0.5, chamber_area=0.08, pipe_area=0.01) | |
| res.report( | |
| # A 0.5 m chamber of area ratio m = 8, at the octave-band centres. | |
| freqs = np.array([63.0, 125.0, 250.0, 500.0]) # verify against plane_wave_limit | |
| res = expansion_chamber(freqs, length=0.5, chamber_area=0.08, pipe_area=0.01) | |
| res.report( |
🤖 Prompt for AI Agents
Verify each finding against current code. Fix only still-valid issues, skip the
rest with a brief reason, keep changes minimal, and validate.
In `@docs/devices/noise-control/silencers.md` around lines 283 - 286, Update the
expansion_chamber example around freqs and res.report to ensure every reported
frequency is below the chamber’s computed plane_wave_limit. Either restrict the
frequency grid accordingly or adjust the chamber geometry so the limit exceeds
4000 Hz, then regenerate the fiche output.
Source: MCP tools
Comment on lines
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+307
| **What that fiche is not.** The number in the box is a plane-wave prediction | ||
| from the declared geometry. The figure a supplier publishes is an **insertion | ||
| loss measured by substitution** to ISO 7235:2003: two series with everything | ||
| else unchanged, one with the test object installed and one with a substitution | ||
| duct in its place, differenced third octave by third octave as | ||
| `D_i = L_pI - L_pII`. The rig carries its own requirements — a sealed, lined |
There was a problem hiding this comment.
🎯 Functional Correctness | 🟠 Major | ⚡ Quick win
Reverse the insertion-loss subtraction.
The text defines series I as the test object and series II as the substitution duct. Insertion loss must therefore be the substitution level minus the test-object level. The current D_i = L_pI - L_pII produces a negative value for an attenuating silencer. (cdn.standards.iteh.ai)
Suggested correction
- D_i = L_pI - L_pII
+ D_i = L_pII - L_pI📝 Committable suggestion
‼️ IMPORTANT
Carefully review the code before committing. Ensure that it accurately replaces the highlighted code, contains no missing lines, and has no issues with indentation. Thoroughly test & benchmark the code to ensure it meets the requirements.
Suggested change
| **What that fiche is not.** The number in the box is a plane-wave prediction | |
| from the declared geometry. The figure a supplier publishes is an **insertion | |
| loss measured by substitution** to ISO 7235:2003: two series with everything | |
| else unchanged, one with the test object installed and one with a substitution | |
| duct in its place, differenced third octave by third octave as | |
| `D_i = L_pI - L_pII`. The rig carries its own requirements — a sealed, lined | |
| **What that fiche is not.** The number in the box is a plane-wave prediction | |
| from the declared geometry. The figure a supplier publishes is an **insertion | |
| loss measured by substitution** to ISO 7235:2003: two series with everything | |
| else unchanged, one with the test object installed and one with a substitution | |
| duct in its place, differenced third octave by third octave as | |
| `D_i = L_pII - L_pI`. The rig carries its own requirements — a sealed, lined |
🤖 Prompt for AI Agents
Verify each finding against current code. Fix only still-valid issues, skip the
rest with a brief reason, keep changes minimal, and validate.
In `@docs/devices/noise-control/silencers.md` around lines 302 - 307, Reverse the
insertion-loss equation in the “What that fiche is not” section so it computes
substitution-duct level minus test-object level, using the existing series II
and series I labels respectively: D_i = L_pII - L_pI.
Source: MCP tools
Comment on lines
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| loudspeaker box driving at least 6 dB and preferably 10 dB above the background, | ||
| a modal filter attenuating the fundamental by at least 3 dB and higher-order | ||
| modes by at least 5 dB above cut-on, a substitution duct matched within 5 % in |
There was a problem hiding this comment.
🎯 Functional Correctness | 🟠 Major | ⚡ Quick win
Apply the 3 dB and 5 dB limits to the fundamental mode.
The sentence currently assigns the 5 dB limit to higher-order modes. ISO 7235 describes small attenuation of the fundamental mode and substantial attenuation of higher-order modes. Its numeric longitudinal-attenuation limits apply to the fundamental mode: 3 dB at the low-frequency end and 5 dB above higher-order-mode cut-on. (iteh.eu)
🤖 Prompt for AI Agents
Verify each finding against current code. Fix only still-valid issues, skip the
rest with a brief reason, keep changes minimal, and validate.
In `@docs/devices/noise-control/silencers.md` around lines 308 - 310, Update the
sentence around the modal filter requirements so both the 3 dB fundamental
attenuation and the 5 dB above-cut-on attenuation limits apply to the
fundamental mode, rather than assigning the 5 dB limit to higher-order modes;
preserve the existing loudspeaker and substitution-duct requirements.
Source: MCP tools
Comment on lines
+17569
to
+17580
| # A 0.5 m chamber of area ratio m = 8, at the octave-band centres. | ||
| freqs = np.array([63.0, 125.0, 250.0, 500.0, 1000.0, 2000.0, 4000.0]) | ||
| res = expansion_chamber(freqs, length=0.5, chamber_area=0.08, pipe_area=0.01) | ||
| res.report( | ||
| "silencer_fiche.pdf", | ||
| metadata=ReportMetadata( | ||
| specimen="Simple expansion-chamber muffler (m = 8, design case)", | ||
| measurement_standard="Munjal Eq. (3.27) four-pole model", | ||
| laboratory="Phonometry Reference Laboratory", | ||
| requirement=6.0, # minimum acceptable mean transmission loss | ||
| ), | ||
| ) # mean and peak transmission loss (dB) |
There was a problem hiding this comment.
🎯 Functional Correctness | 🟠 Major | ⚡ Quick win
🧩 Analysis chain
🏁 Script executed:
#!/bin/bash
set -euo pipefail
echo "Files:"
git ls-files | sed -n '1,120p' | rg -n 'llms-full|\.py$' | sed -n '1,120p'
echo
echo "Search for expansion_chamber / ReactiveSilencerResult / plane_wave_limit:"
rg -n "def expansion_chamber|class ReactiveSilencerResult|def report\(|plane_wave_limit|expansion_chamber" -S .Repository: jmrplens/phonometry
Length of output: 164
🏁 Script executed:
#!/bin/bash
set -euo pipefail
echo "Working directory:"
pwd
echo
echo "Tracked files (first 200):"
git ls-files | sed -n '1,200p'
echo
echo "All files named llms-full.txt:"
git ls-files | rg '(^|/)llms-full\.txt$' || true
echo
echo "Search symbols in tracked Python/text files:"
rg -n "def expansion_chamber|class ReactiveSilencerResult|def report\(|plane_wave_limit|ReactiveSilencer|expansion_chamber|silencer_fiche|Phonometry Reference Laboratory|Munjal Eq" -S --glob '*.py' --glob '*.txt' --glob '*.md' . || trueRepository: jmrplens/phonometry
Length of output: 50375
🏁 Script executed:
#!/bin/bash
set -euo pipefail
echo "Source outline for silencers.py and plot/noise_control.py:"
ast-grep outline src/phonometry/noise_control/silencers.py --view compact || true
ast-grep outline src/phonometry/_plot/noise_control.py --view compact || true
echo
echo "ReactiveSilencerResult class section:"
sed -n '378,480p' src/phonometry/noise_control/silencers.py
echo
echo "Report Metadata validation and report rendering sources:"
sed -n '390,460p' src/phonometry/noise_control/silencers.py
sed -n '324,405p' src/phonometry/_plot/noise_control.py
echo
echo "Test silencer report relevant cases:"
sed -n '1,260p' tests/noise_control/test_silencer_report.py
echo
echo "Plane wave limit docs from reference:"
sed -n '670,680p' docs/reference/api/index.md
sed -n '262,280p' docs/devices/noise-control/silencers.md
echo
echo "Compute plane_wave_limit for example dimensions:"
python3 - <<'PY'
import math
def plane_wave_limit_area(area, c=343.0):
dia = (4*area/math.pi)**0.5
return 0.586*c/dia
for area in (0.01, 0.02, 0.04, 0.08):
print(area, plane_wave_limit_area(area))
print("example frequencies:", [63,125,250,500,1000,2000,4000])
PYRepository: jmrplens/phonometry
Length of output: 24635
🏁 Script executed:
#!/bin/bash
set -euo pipefail
echo "Silencer report implementation:"
sed -n '420,512p' src/phonometry/noise_control/silencers.py
echo
echo "Expansion chamber constructor report/limit section:"
sed -n '550,595p' src/phonometry/noise_control/silencers.py
echo
echo "Behavioral probe: model reported validity for current implementation's visible slices:"
python3 - <<'PY'
import ast
from pathlib import Path
source = Path("src/phonometry/noise_control/silencers.py").read_text()
tree = ast.parse(source)
# Locate ReactiveSilencerResult.report method.
for node in ast.walk(tree):
if isinstance(node, ast.FunctionDef) and node.name == "report" and any(
isinstance(base, ast.Name) and base.id == "ReactiveSilencerResult"
for base in ast.walk(node)
):
method_src = ast.get_source_segment(source, node)
print(f"ReactiveSilencerResult.report span: {node.lineno}-{node.end_lineno}")
print("contains plane_wave_limit? ", "plane_wave_limit" in method_src)
print("contains warn_above? ", "warn_above" in method_src or "PlaneWaveWarning" in method_src)
print("contains filtering? ", any(s in method_src for s in ("<", ">", ">=b", "<=b", "idx", "mask", "where", "keep", "exclude")))
print("contains verdict calculation? ", any(s in method_src for s in ("PASS", "FAIL", "requirement", "mean", "TL")))
break
limit_node = None
for node in tree.body:
if isinstance(node, ast.FunctionDef) and node.name == "expansion_chamber":
limit_node = node
break
print("\nexpansion_chamber uses warn_above_plane_wave_limit?", bool(limit_node and "warn_above_plane_wave_limit" in ast.get_source_segment(source, limit_node) if limit_node else False))
PYRepository: jmrplens/phonometry
Length of output: 6182
🏁 Script executed:
#!/bin/bash
set -euo pipefail
echo "Find render_reactive_silencer_report source and relevant report functions:"
rg -n "def render_reactive_silencer_report|render_reactive_silencer_report|Mean transmission loss|Peak transmission|PASS|FAIL|requirement|invalid|plane_wave_limit" src/phonometry/tests/scripts -S
echo
echo "Silencer report renderer candidates:"
fd -i 'silencer|report' src/phonometry tests/scripts | sed -n '1,120p'
echo
echo "Read report renderer source sections:"
for f in $( rg -l "def render_reactive_silencer_report|render_reactive_silencer_report" src; do
echo "--- $f"
rg -n "def render_reactive_silencer_report|Mean transmission loss|Peak transmission|PASS|FAIL|requirement|plane_wave|invalid|warnings|not marked|mark|exclude" "$f" -C 8
doneRepository: jmrplens/phonometry
Length of output: 361
🏁 Script executed:
#!/bin/bash
set -euo pipefail
echo "Find render_reactive_silencer_report source:"
rg -n "def render_reactive_silencer_report|render_reactive_silencer_report" -S .
echo
echo "Read renderer source:"
f="$(rg -l "def render_reactive_silencer_report|render_reactive_silencer_report" -S . | head -n 1)"
echo "FILE=$f"
wc -l "$f"
sed -n '1,180p' "$f"Repository: jmrplens/phonometry
Length of output: 7646
🏁 Script executed:
#!/bin/bash
set -euo pipefail
echo "Reactive silencer report renderer source:"
sed -n '1,260p' src/phonometry/_report/silencer.py
echo
echo "Static implementation facts:"
python3 - <<'PY'
from pathlib import Path
import ast
src = Path("src/phonometry/_report/silencer.py").read_text()
tree = ast.parse(src)
for node in tree.body:
if isinstance(node, ast.FunctionDef) and node.name == "render_reactive_silencer_report":
print(f"span {node.lineno}-{node.end_lineno}")
code = ast.get_source_segment(src, node)
for term in ["plane_wave_limit", "warnings", "PASS", "FAIL", "requirement", "transmission_loss", "mean", "peak", "invalid"]:
print(f"{term}:", term in code)
PYRepository: jmrplens/phonometry
Length of output: 9629
Keep the reactive-silencer fiche inside the plane-wave range.
This fiche is described as a plane-wave four-pole prediction, but render_reactive_silencer_report() builds mean/peak/verdict from all requested bands and does not exclude or mark frequencies above result.plane_wave_limit. Bands above that limit can change the displayed mean, peak, and PASS/FAIL verdict; exclude or mark them and regenerate the fiche.
🤖 Prompt for AI Agents
Verify each finding against current code. Fix only still-valid issues, skip the
rest with a brief reason, keep changes minimal, and validate.
In `@llms-full.txt` around lines 17569 - 17580, Update
render_reactive_silencer_report() so mean transmission loss, peak transmission
loss, and the PASS/FAIL verdict use only frequencies at or below
result.plane_wave_limit, or explicitly mark out-of-range bands and exclude them
from these aggregates. Regenerate the reactive-silencer fiche with the corrected
plane-wave-filtered results while preserving the existing in-range reporting.
Comment on lines
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| ```python | ||
| # `electroacoustics` importado arriba. Captura `idle` con la misma longitud que | ||
| # `signal`, con el generador silenciado, y ejecuta sobre ella la misma llamada. | ||
| residual = electroacoustics.thd(idle, fs, 1000.0, kind="F") | ||
| print(residual < thd_f / 3.0) # False -> descartar, y bajar a harmonic_distortion |
There was a problem hiding this comment.
🎯 Functional Correctness | 🟠 Major | ⚡ Quick win
🧩 Analysis chain
🏁 Script executed:
#!/usr/bin/env bash
set -euo pipefail
rg -n -C 6 \
'electroacoustics\.thd\(idle|idle_channel_noise|thd_plus_noise|harmonic_analysis|distortion_residual|residual.*\/ *3' \
. --glob '*.mdx' --glob '*.py'Repository: jmrplens/phonometry
Length of output: 50377
🏁 Script executed:
#!/usr/bin/env bash
set -euo pipefail
echo "== target lines =="
sed -n '215,232p' site/src/content/docs/devices/electroacoustics/electroacoustics.mdx
sed -n '215,232p' site/src/content/docs/es/devices/electroacoustics/electroacoustics.mdx
echo
echo "== thd implementation key parts =="
sed -n '1,180p' src/phonometry/electroacoustics/distortion.py
echo
echo "== harmonic_distortion implementation outline/parts =="
sed -n '180,360p' src/phonometry/electroacoustics/distortion.py
echo
echo "== deterministic probe: thd on silence vs tone + harmonic residual =="
python3 - <<'PY'
import numpy as np
import inspect
from pathlib import Path
exec(Path("src/phonometry/electroacoustics/distortion.py").read_text(encoding="utf-8"))
fs = 48000
n = fs
t = np.arange(n) / fs
print("thd signature:", inspect.signature(thd))
print("thd source first 120 lines:")
for i, line in enumerate(inspect.getsource(thd).splitlines()[:120], 1):
print(f"{i:03d}: {line}")
# Simulate exactly the documented example shape using the default AES17 band.
# Use an explicit fundamental to bypass auto-detection; silence has no fundamental.
try:
silent = thd(np.zeros(n), fs, 1000.0, kind="F")
print("silent_thd:", silent)
except Exception as e:
print("silent_thd_error:", type(e).__name__, e)
tone = np.sin(2 * np.pi * 1000.0 * t)
tone += 0.5 * np.sin(2 * np.pi * 2000.0 * t)
distortion_only_thd = thd(tone, fs, 1000.0, kind="F")
print("distortion_only_thd:", distortion_only_thd)
print("distortion_only_thd < distortion_only_thd / 3.0 passes?", distortion_only_thd < distortion_only_thd / 3.0)
try:
silence_with_fundamental = thd(np.zeros(n), fs, 1000.0, kind="F", n_harmonics=10, window="hann")
print("zero_thd_at_1kHz:", silence_with_fundamental)
print("zero_thd_at_1kHz < distortion_only_thd / 3.0 passes?", silence_with_fundamental < distortion_only_thd / 3.0)
except Exception as e:
print("zero_thd_at_1kHz_error:", type(e).__name__, e)
# Check residual voltage for tone + explicit residual.
signal_residual = np.concatenate((tone * np.zeros(n//2), 0.01 * np.sin(2 * np.pi * 2000.0 * t[a...n])))
PYRepository: jmrplens/phonometry
Length of output: 17043
🏁 Script executed:
#!/usr/bin/env bash
set -euo pipefail
python3 - <<'PY'
import numpy as np
import importlib.util
spec = importlib.util.spec_from_file_location("distortion", "src/phonometry/electroacoustics/distortion.py")
module = importlib.util.module_from_spec(spec)
spec.loader.exec_module(module)
thd = module.thd
fs = 48000
n = fs
t = np.arange(n) / fs
print("silent_thd_error:", end=" ")
try:
print(thd(np.zeros(n), fs, 1000.0, kind="F"))
except Exception as e:
print(f"{type(e).__name__}: {e}")
tone = np.sin(2 * np.pi * 1000.0 * t)
distortion_only_thd = thd(tone, fs, 1000.0, kind="F")
print("distortion_only_thd:", distortion_only_thd)
print("distortion_only_thd < distortion_only_thd / 3.0 passes:", distortion_only_thd < distortion_only_thd / 3.0)
silent_explicit = thd(np.zeros(n), fs, 1000.0, kind="F")
print("silent_explicit_fundamental:", silent_explicit)
print("silent_explicit_fundamental < distortion_only_thd / 3.0 passes:", silent_explicit < distortion_only_thd / 3.0)
idle_residual = 0.5 * np.sin(2 * np.pi * 2000.0 * t)
signal_residual = np.concatenate((tone[:n//2], 0.5 * np.sin(2 * np.pi * 2000.0 * t[n//2:])))
print("distortion_only_thd_with_0.5_second_harmonic:", thd(signal_residual, fs, 1000.0, kind="F"))
print("idle_residual<distortion_thd, idle only:", thd(idle_residual, fs, 1000.0, kind="F"))
PY
echo
echo "== matching API functions for residual/voltage checks =="
rg -n -C 3 'def _aes17_rms_pair|def thd_plus_noise|def dynamic_range|def harmonic_distortion|def weighted_thd|def harmonic_analysis' src/phonometry/electroacoustics/distortion.py src/phonometry/electroacoustics/noise_measurements.py
echo
sed -n '360,390p' site/src/content/docs/devices/electroacoustics/electroacoustics.mdx
sed -n '360,390p' site/src/content/docs/es/devices/electroacoustics/electroacoustics.mdxRepository: jmrplens/phonometry
Length of output: 275
🌐 Web query:
jmrplens phonometry thd implementation kind F harmonic rms fundamental ratio
💡 Result:
The phonometry library, developed by José Manuel Requena Plens, provides a standards-conformant Python toolkit for acoustic measurements [1][2]. Regarding the specific implementation of Total Harmonic Distortion (THD) and related metrics, the library prioritizes compliance with standards such as IEC 60268-3 [1]. THD Implementation and Terminology In the context of electrical and acoustic signal analysis, THD is generally calculated as the ratio of the RMS sum of harmonic components to a reference value [3][4]. The two primary conventions are: 1. THD-F (Fundamental): The ratio of the RMS sum of all harmonic components to the RMS value of the fundamental frequency [5][3][6]. THD-F = (sqrt(V2^2 + V3^2 +... + Vn^2)) / V1 [3][6] 2. THD-R (RMS): The ratio of the RMS sum of all harmonic components to the total RMS value of the signal [5][3]. THD-R = (sqrt(V2^2 + V3^2 +... + Vn^2)) / sqrt(V1^2 + V2^2 +... + Vn^2) [3] "Kind F" likely refers to the THD-F convention, which uses the fundamental frequency as the reference denominator, common in power systems and various electroacoustic standards [5][3]. The phonometry library implements these calculations with strict adherence to governing standards, ensuring that intermediate terms remain visible and that results are validated against tolerance tables [2]. For example, the library includes support for AES17-compliant measurements of THD+N and SINAD, which utilize specific notch filter bandwidths and frequency-domain processing [7]. Users should ensure consistency between THD-F and THD-R definitions when comparing results across different measurement systems [6].
Citations:
- 1: https://github.com/jmrplens/phonometry/
- 2: https://jmrplens.github.io/phonometry/
- 3: https://en.wikipedia.org/wiki/Total_harmonic_distortion
- 4: https://dl.cdn-anritsu.com/en-us/test-measurement/files/Technical-Notes/White-Paper/11410-02911A.pdf
- 5: https://powermonitors.com/whitepapers/thd-f-vs-thd-r/
- 6: https://industrialmonitordirect.com/blogs/knowledgebase/calculating-individual-harmonic-rms-from-thd-and-fundamental
- 7: 45846b9
Compara tensiones RMS del residuo del generador, no razones de THD.
thd_f y electroacoustics.thd(idle, fs, 1000.0, kind="F") son razones armónicas normalizadas por el fundamental; el requisito es que la tensión residual con generador atenuado sea menor que un tercio de la tensión de distorsión. Usa una medida del residuo de generación, por ejemplo a partir de la diferencia idle - signal con el fundamental retenido o con el generador inyectado, y compárala con el RMS de la distorsión en la misma banda.
🤖 Prompt for AI Agents
Verify each finding against current code. Fix only still-valid issues, skip the
rest with a brief reason, keep changes minimal, and validate.
In `@site/src/content/docs/es/devices/electroacoustics/electroacoustics.mdx`
around lines 241 - 245, Reemplaza la comparación de razones THD en el flujo que
calcula residual por una comparación entre tensiones RMS: calcula el residuo del
generador usando idle - signal, conservando el fundamental o la inyección del
generador según corresponda, y calcula el RMS de la distorsión en la misma banda
a partir de thd_f. Acepta el método solo cuando el RMS residual sea menor que un
tercio del RMS de distorsión; si no, conserva la bajada a harmonic_distortion.
Comment on lines
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| Ninguna de las constantes del ensayo es arbitraria. 997 Hz es un número primo, | ||
| así que es inconmensurable tanto con 44,1 kHz como con 48 kHz: el tono no se | ||
| repite nunca dentro de un registro corto y recorre todo el espacio de códigos | ||
| del conversor, mientras que un tono de 1000 Hz a 48 kHz volvería eternamente | ||
| sobre las mismas 48 muestras y escondería los errores de no linealidad | ||
| diferencial de los códigos que nunca toca. El nivel de -60 dBFS mantiene el | ||
| conversor bien lejos de su propia región de sobrecarga, donde dominaría su | ||
| distorsión en vez de su ruido, y a la vez sigue dando a la muesca un fundamental | ||
| que eliminar, que es la razón de que el resultado se refiera a plena escala y no | ||
| al tono de ensayo. |
There was a problem hiding this comment.
🎯 Functional Correctness | 🟠 Major | ⚡ Quick win
Corrige la explicación del periodo de 997 Hz.
997 Hz no es inconmensurable con 44,1 kHz ni con 48 kHz en una señal muestreada. Con fs = 48000, la secuencia se repite después de 48 000 muestras; con fs = 44100, después de 44 100 muestras. La ventaja frente a 1000 Hz a 48 kHz es el periodo largo de 997 Hz, no que la señal no se repita. De hecho, el ejemplo n = fs captura exactamente un periodo discreto completo. (engineering.purdue.edu)
Propuesta de corrección
-997 Hz es un número primo, así que es inconmensurable tanto con 44,1 kHz como con 48 kHz.
+997 Hz tiene un periodo discreto de 44 100 muestras a 44,1 kHz y de 48 000 muestras a 48 kHz.
+Su periodo es mucho más largo que el de 1000 Hz a 48 kHz, que dura 48 muestras.📝 Committable suggestion
‼️ IMPORTANT
Carefully review the code before committing. Ensure that it accurately replaces the highlighted code, contains no missing lines, and has no issues with indentation. Thoroughly test & benchmark the code to ensure it meets the requirements.
Suggested change
| Ninguna de las constantes del ensayo es arbitraria. 997 Hz es un número primo, | |
| así que es inconmensurable tanto con 44,1 kHz como con 48 kHz: el tono no se | |
| repite nunca dentro de un registro corto y recorre todo el espacio de códigos | |
| del conversor, mientras que un tono de 1000 Hz a 48 kHz volvería eternamente | |
| sobre las mismas 48 muestras y escondería los errores de no linealidad | |
| diferencial de los códigos que nunca toca. El nivel de -60 dBFS mantiene el | |
| conversor bien lejos de su propia región de sobrecarga, donde dominaría su | |
| distorsión en vez de su ruido, y a la vez sigue dando a la muesca un fundamental | |
| que eliminar, que es la razón de que el resultado se refiera a plena escala y no | |
| al tono de ensayo. | |
| Ninguna de las constantes del ensayo es arbitraria. 997 Hz tiene un periodo discreto | |
| de 44 100 muestras a 44,1 kHz y de 48 000 muestras a 48 kHz. | |
| Su periodo es mucho más largo que el de 1000 Hz a 48 kHz, que dura 48 muestras. | |
| El tono no se repite nunca dentro de un registro corto y recorre todo el espacio de códigos | |
| del conversor, mientras que un tono de 1000 Hz a 48 kHz volvería eternamente | |
| sobre las mismas 48 muestras y escondería los errores de no linealidad | |
| diferencial de los códigos que nunca toca. El nivel de -60 dBFS mantiene el | |
| conversor bien lejos de su propia región de sobrecarga, donde dominaría su | |
| distorsión en vez de su ruido, y a la vez sigue dando a la muesca un fundamental | |
| que eliminar, que es la razón de que el resultado se refiera a plena escala y no | |
| al tono de ensayo. |
🤖 Prompt for AI Agents
Verify each finding against current code. Fix only still-valid issues, skip the
rest with a brief reason, keep changes minimal, and validate.
In `@site/src/content/docs/es/devices/electroacoustics/electroacoustics.mdx`
around lines 364 - 373, Corrige la explicación en el párrafo sobre 997 Hz:
elimina la afirmación de que es inconmensurable o que el tono nunca se repite, y
explica que la secuencia muestreada se repite tras 48 000 muestras a 48 kHz o 44
100 muestras a 44,1 kHz. Conserva la comparación con 1000 Hz indicando que la
ventaja de 997 Hz es su periodo discreto mucho más largo, y que n = fs contiene
exactamente un periodo completo.
Comment on lines
+565
to
+568
| dispositivo en el punto de funcionamiento de la sección 0. Elimina el retardo | ||
| entre los dos canales — o haz el segmento de Welch varias veces más largo que | ||
| él —, porque un retardo sin compensar inclina la fase de $H_1$ y hunde | ||
| $\gamma^2$ banda a banda. `transfer_function` elige `nperseg` para una |
There was a problem hiding this comment.
🎯 Functional Correctness | 🟠 Major | ⚡ Quick win
🧩 Analysis chain
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printf '\n--- spectra helpers ---\n'
sed -n '1,260p' src/phonometry/signals/spectra.py
printf '\n--- transfer_function/coherence doc strings and tests around delay/delay-like ---\n'
rg -n -C 6 'delay|retardo|coherence|gamma|phase|nperseg|Welch' src/phonometry/electroacoustics/frequency_response.py src/phonometry/signals/spectra.py tests || trueRepository: jmrplens/phonometry
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set -euo pipefail
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printf '%s\n' '--- spectra.py header/defaults/core ---'
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printf '%s\n' '--- transfer_function/coherence tests around delay/welch/phase ---'
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tests/reference_data tests/electroacoustics tests/signals tests/room \
--glob '*.py' | head -n 240Repository: jmrplens/phonometry
Length of output: 31533
🌐 Web query:
Bendat Piersol ordinary coherence fixed time delay H1 estimator gamma squared
💡 Result:
In the context of the work of Julius S. Bendat and Allan G. Piersol, particularly in their seminal text "Random Data: Analysis and Measurement Procedures," the terms you mentioned are fundamental concepts in linear system analysis and spectral estimation [1][2][3]. Ordinary Coherence and Gamma Squared: The "ordinary coherence function," often denoted as gamma squared, is defined as [4][5]: gamma^2(f) = |G_xy(f)|^2 / (G_xx(f) * G_yy(f)) where G_xy(f) is the cross-spectral density between input x(t) and output y(t), and G_xx(f) and G_yy(f) are the autospectral densities of the input and output, respectively [4]. This function, which ranges from 0 to 1, serves as a measure of the linearity of the system at frequency f [4][2][6]. A value of 1 indicates an ideal linear relationship with no extraneous noise, while values less than 1 suggest nonlinearities, extraneous noise at either the input or output, or multiple input sources [1][7]. H1 Estimator: The H1 frequency response function (FRF) estimator is defined as [2][8]: H1(f) = G_xy(f) / G_xx(f) This estimator is specifically designed to be robust against uncorrelated noise at the system output [6][8]. Bendat and Piersol demonstrate that coherence provides a direct measure of the confidence or statistical quality of this H1 estimate [2]. Specifically, coherence can be interpreted as a measure of the distance between the H1 and H2 estimators, where H2(f) = G_yy(f) / G_yx(f) [2]. Fixed Time Delay: When a constant time delay (tau) exists between an input and output (i.e., y(t) = x(t - tau)), the cross-spectral density G_xy(f) picks up a phase shift proportional to the delay (phase = -2pif*tau) [9]. If this delay is not accounted for, or if there is misalignment in data segments, the coherence estimate can be biased downward, particularly if the phase is a rapidly varying function of frequency [9]. Proper synchronization of input and output records is required to obtain accurate coherence and FRF estimates in the presence of such delays [9]. Top Results: [1], [4], [2], [9], [6]
Citations:
- 1: https://onlinelibrary.wiley.com/doi/10.1002/9781118032428.ch6
- 2: https://vru.vibrationresearch.com/lesson/coherence-signal-analysis/
- 3: https://books.google.fi/books?id=qYSViFRNMlwC
- 4: https://doi.org/10.1002/9781118032428.app2
- 5: https://www.researchgate.net/publication/231103993_Random_Data_Analysis_And_Measurement_Procedures
- 6: https://etd.ohiolink.edu/acprod/odb_etd/ws/send_file/send?accession=ucin1346171022&disposition=inline
- 7: https://opi-lab.github.io/optical-metrology-2019/pdfs/02-Bendat-Piersol-chapter-01.pdf
- 8: https://dsp.stackexchange.com/questions/71811/understanding-the-h1-and-h2-estimators
- 9: https://buzsakilab.nyumc.org/datasets/PatelJ/_extra/Histology/jp-usb-1-data/data%20analysis/Data%20Analysis/CarterIEEE1987.pdf
🌐 Web query:
"ordinary coherence" "time delay" "Bendat Piersol" "gamma squared"
💡 Result:
In the technical framework established by Julius S. Bendat and Allan G. Piersol in their authoritative works on random data analysis, the ordinary coherence function—often denoted as gamma squared (γ²)—is a real-valued function that measures the linear relationship between two signals in the frequency domain [1][2]. It is defined as the square of the magnitude of the cross-spectral density function divided by the product of the individual autospectral density functions [1][2]: γ²xy(f) = |Gxy(f)|² / (Gxx(f) * Gyy(f)) This function yields values between 0 and 1, where 1 indicates a perfect linear relationship [1][2]. Regarding time delay, Bendat and Piersol demonstrate that the presence of a time delay between two signals can cause the estimated coherence to appear less than unity if the analysis does not account for it [3][4]. Specifically, if one signal is a delayed version of the other (e.g., y(t) = x(t - D)), the phase of the cross-spectral density function contains information about the time delay D [5][6]. The phase angle (θ) is related to the delay and frequency (f) by the linear relationship: θ(f) = -2πfD While the ordinary coherence function (γ²) itself is magnitude-based and thus invariant to pure time delays (a pure delay does not inherently reduce coherence in an ideal, noise-free, linear system), in practical measurements with finite data or extraneous noise, time delays can complicate estimation [3][6][4]. Analysts often use the phase information of the cross-spectrum to estimate the delay D [5][7]. Furthermore, techniques such as artificially shifting (realigning) the time series by a lag τ can be used to maximize the observed coherence, effectively identifying the delay D when the coherence reaches a maximum [4]. In summary, for Bendat and Piersol, gamma squared (ordinary coherence) serves as a diagnostic tool to assess the validity of a linear model, while the cross-spectrum's phase is the primary vehicle for extracting time delay information [3][1][7].
Citations:
- 1: https://doi.org/10.1002/9781118032428.app2
- 2: https://en.wikipedia.org/wiki/Coherence_(signal_processing)
- 3: https://opi-lab.github.io/optical-metrology-2019/pdfs/02-Bendat-Piersol-chapter-01.pdf
- 4: https://ar5iv.labs.arxiv.org/html/physics/0411141
- 5: https://www.academia.edu/33161435/Random_Data
- 6: https://buzsakilab.nyumc.org/datasets/PatelJ/_extra/Histology/jp-usb-1-data/data%20analysis/Data%20Analysis/CarterIEEE1987.pdf
- 7: https://www.sciencedirect.com/topics/engineering/coherence-function
🌐 Web query:
"cross spectrum" "pure time delay" "magnitude" "coherence" "unity"
💡 Result:
In signal processing, a pure time delay between two signals results in a cross-spectrum characterized by a linear phase shift proportional to the delay, while the magnitude of the coherence remains equal to unity [1][2]. The coherence function, often referred to as magnitude-squared coherence (MSC), is defined as the normalized magnitude of the cross-spectral density [3][4]. For two signals where one is a pure, noise-free, time-delayed version of the other—expressed as y(t) = x(t - τ)—the relationship is entirely linear [2]. In the frequency domain, this shift manifests as a complex exponential term, e^(-j2πfτ), which has a magnitude of 1 [1][2]. Because the coherence normalization process divides the cross-spectrum magnitude by the product of the auto-spectra magnitudes, the pure time-delay component preserves a perfect linear relationship, resulting in a coherence magnitude of 1 across all frequencies [2][3]. In practical, real-world applications, observed coherence is frequently less than unity due to factors such as additive noise, non-linearities, or multi-path propagation (reverberation), which introduce components that cannot be explained by a single linear time delay [3][4]. Additionally, signal misalignment or windowing artifacts during estimation can lead to a measured coherence lower than 1, even if the underlying system is theoretically ideal [5]. Summary of Key Points: - Pure Time Delay: The cross-spectrum phase is linear with frequency, and the coherence magnitude is exactly 1 [1][2]. - Coherence Definition: It measures the degree of linear dependency between two signals, bounded between 0 and 1 [3][4]. - Real-world Departures: Any reduction in coherence below unity indicates the presence of uncorrelated noise, non-linear system behavior, or measurement limitations [3][4].
Citations:
- 1: https://pysdr.org/content/tdoa.html
- 2: https://dsponlineconference.com/session/Speech_Dereverberation_using_CDR_Estimators
- 3: https://www.crystalinstruments.com/coherence-function-a-brief-review
- 4: https://grokipedia.com/page/Coherence_(signal_processing)
- 5: https://buzsakilab.nyumc.org/datasets/PatelJ/_extra/Histology/jp-usb-1-data/data%20analysis/Data%20Analysis/CarterIEEE1987.pdf
No atribuyas una caída de coherencia a un retardo fijo.
Un retardo fijo es un camino LTI: cambia la fase de
🤖 Prompt for AI Agents
Verify each finding against current code. Fix only still-valid issues, skip the
rest with a brief reason, keep changes minimal, and validate.
In `@site/src/content/docs/es/devices/electroacoustics/electroacoustics.mdx`
around lines 565 - 568, Corrige el texto alrededor de “transfer_function” para
no afirmar que un retardo fijo sin compensar reduce $\gamma^2$ ni que alargar el
segmento de Welch lo soluciona. Indica que el retardo fijo solo inclina la fase
de $H_1$ en una medición LTI ideal; atribuye una caída de coherencia a
desincronización de relojes, retardos variables entre segmentos, transitorios,
no linealidad o promediado insuficiente.
| @@ -364,6 +405,61 @@ error de fase, de cualquier signo. Por eso el índice presión-intensidad, y | |||
| no la calidad de los micrófonos, es el que acota la exactitud alcanzable de | |||
| toda medida de intensidad. | |||
|
|
|||
| ### Medir el índice residual, y comprobar la sonda | |||
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🎯 Functional Correctness | 🟡 Minor | ⚡ Quick win
🧩 Analysis chain
🏁 Script executed:
#!/bin/bash
# Description: Check Spanish heading anchors and the deep links that target them.
rg -n 'medir-el-.ndice-residual|span id=' site/src/content/docs/es/devices/emission/
rg -n '^### ' site/src/content/docs/es/devices/emission/intensity.mdxRepository: jmrplens/phonometry
Length of output: 721
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#!/bin/bash
set -euo pipefail
echo "Find anchor/tag conventions and dependency versions"
rg -n '`@mdxjs/mdx`|mdx-md|github-slugger|slugify|remark-shiki|rehype|mdx2' -S . --glob '!node_modules/**' --glob '!dist/**' --glob '!build/**' | head -120
echo
echo "Inspect package files for MDX/config"
git ls-files | rg '(^|/)(package.json|astro.config|vite.config|docusaurus.config|contentlayer|remix.config|gatsby-config|content\.|components\.|plugins\.|.*mdx.*\.js$|.*config.*\.js$|.*config.*\.ts$)' | head -80
echo
echo "Show relevant link context"
sed -n '300,316p' site/src/content/docs/es/devices/emission/sound-power-intensity.mdxRepository: jmrplens/phonometry
Length of output: 6427
🏁 Script executed:
#!/bin/bash
set -euo pipefail
echo "node_modules status"
if [ -d site/node_modules ]; then
echo "site/node_modules exists"
node - <<'JS'
try {
const slugger = require('site/node_modules/github-slugger').default || require('site/node_modules/github-slugger');
console.log('github-slugger module loaded');
console.log(slugger.slug('Medir el índice residual, y comprobar la sonda'));
} catch (e) {
console.log('github-slugger load failed:', e.message);
}
JS
else
echo "site/node_modules does not exist"
fi
echo
echo "Relevant scripts/anchor utilities"
sed -n '480,530p' scripts/generate_api_docs.py
sed -n '300,360p' tests/test_api_docs_generator.py
rg -n 'slug|anchor|id=|heading|fragment' site scripts tests -S --glob '!node_modules/**' --glob '!dist/**' --glob '!build/**' | head -200Repository: jmrplens/phonometry
Length of output: 23146
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#!/bin/bash
set -euo pipefail
echo "Find published github-slugger source in git or lock metadata"
git ls-files | rg '(^|/)github-slugger(@[^/]+)?/|github-slugger.*/' | head -50 || true
rg -n 'github-slugger' site -S --glob '!node_modules/**' --glob '!dist/**' --glob '!build/**' | head -80
echo
echo "Find github-slugger binaries/libraries in package manager cache if present"
for d in "$HOME"/npm-cache "$HOME"/.npm "$HOME"/.cache/pnpm "$HOME"/.npm/_cacache ~/.npm; do
if [ -d "$d" ]; then
echo "$d"
find "$d" -path '*github-slugger*' \( -type f -o -type d \) 2>/dev/null | head -80
fi
doneRepository: jmrplens/phonometry
Length of output: 660
🌐 Web query:
github-slugger 2.0.0 source keep Unicode codepoints slug non ASCII
💡 Result:
In github-slugger version 2.0.0, the library does not strip all non-ASCII Unicode characters [1][2]. Instead, it uses a generated regular expression to filter characters, which effectively preserves most Unicode letters (\p{L}), decimal digits (\p{Nd}), and letter-numbers (\p{Nl}) while stripping most other symbols, including emojis and non-alphanumeric punctuation [3]. Key behaviors of version 2.0.0 include: - Unicode Support: It supports non-ASCII characters, such as Cyrillic (Привет) and CJK characters (你好), which are retained in the output slug [1][2]. - Stripping Behavior: Emojis and other non-letter, non-digit symbols (like certain punctuation) are generally stripped from the slug [2][3]. - Emulation: The primary goal of the package is to emulate GitHub's own markdown heading anchor generation as closely as possible [2]. Because GitHub's internal implementation evolves, github-slugger uses a comprehensive regex to match this behavior [4][3]. If your goal is to keep specific Unicode codepoints that the library currently strips (such as emojis), you would need to use a different approach or a custom filter, as the core functionality of github-slugger 2.0.0 is intentionally designed to match GitHub's specific stripping patterns [2][3].
Citations:
- 1: https://www.npmjs.com/package/github-slugger
- 2: https://github.com/flet/github-slugger
- 3: fix(link-fragments): slugGitHub strips emoji and non-letter/non-digit Unicode shinagawa-web/gomarklint#213
- 4: Github's regex is probably
[^\w -]from html-pipeline Flet/github-slugger#56
🌐 Web query:
npm github-slugger 2.0.0 src source
💡 Result:
The source code for github-slugger version 2.0.0 is hosted in the project's GitHub repository at https://github.com/Flet/github-slugger [1][2]. In this repository, the primary source code is not located in a dedicated src folder; instead, the main logic is contained within the index.js file at the root of the repository [3]. Key details regarding version 2.0.0: - It was published on October 27, 2022 [4][5]. - The package was refactored to use native ESM (ECMAScript Modules), meaning it must be imported using import statements [3]. - The code was updated to use an ES6 class, requiring the use of the new keyword to instantiate the slugger (e.g., const slugger = new GithubSlugger) [3]. - The default export is the class, while the stateless slug function is exposed as a named export [3].
Citations:
- 1: https://www.npmjs.com/package/github-slugger
- 2: https://github.com/Flet/github-slugger/
- 3: Use ESM Flet/github-slugger#43
- 4: https://registry.npmjs.org/github-slugger
- 5: https://deps.dev/npm/github-slugger/2.0.0
🌐 Web query:
github Flet github-slugger 2.0.0 index.js Slugger pattern
💡 Result:
The github-slugger package (version 2.0.0 and later) is a JavaScript library designed to generate unique slugs for markdown headings, emulating GitHub's behavior [1][2]. Key implementation and usage details for version 2.0.0 include: - ESM Transition: As of version 2.0.0, the package was updated to be a pure ECMAScript Module (ESM) [3]. It must be imported using the import statement [3]. - Class-based API: The package uses an ES6 class, requiring the use of the new keyword to create an instance [3]. import GithubSlugger from 'github-slugger' const slugger = new GithubSlugger slugger.slug('example string') - Named Export: In addition to the default export (the class), the package provides a named export slug, which is a static function that does not maintain state across calls (it does not track previously slugged strings) [2][3][4]. import GithubSlugger, {slug} from 'github-slugger' slug('example string') - Slugger Pattern: The primary class implementation maintains an internal state to ensure uniqueness [1][2]. When the same string is passed to the slug method multiple times, the slugger automatically appends an incrementing counter (e.g., 'foo', 'foo-1', 'foo-2') to ensure each resulting slug is unique [1][2]. The reset method can be used to clear this state and start over [1][4]. The library does not function as a markdown or HTML parser; it expects to receive plain text input [5][4]. The source code is organized with the primary logic contained in index.js, and version 2.0.0 introduced these breaking changes (ESM and required new keyword) to align with modern JavaScript standards [6][3].
Citations:
- 1: https://github.com/flet/github-slugger
- 2: https://www.npmjs.com/package/github-slugger
- 3: Use ESM Flet/github-slugger#43
- 4: https://npmx.dev/package/github-slugger
- 5: https://npmx.dev/package/github-slugger/v/2.0.0
- 6: https://registry.npmjs.org/github-slugger
🌐 Web query:
raw.githubusercontent.com Flet github-slugger v2.0.0 index.js slug
💡 Result:
The github-slugger package, version 2.0.0, is a JavaScript library designed to generate slugs that emulate GitHub's markdown heading anchor formatting, including support for unique slug generation [1][2]. In version 2.0.0, the package transitioned to ESM (ECMAScript modules), requiring the use of import statements [3]. The package exports a class, GithubSlugger, as the default export, and a static slug function as a named export [1][3]. Usage Examples: To generate slugs while maintaining a history of previously slugged strings (to ensure uniqueness, just as GitHub does), use the GithubSlugger class: import GithubSlugger from 'github-slugger' const slugger = new GithubSlugger slugger.slug('foo') // returns 'foo' slugger.slug('foo') // returns 'foo-1' slugger.slug('foo') // returns 'foo-2' To use the stateless underlying implementation (which does not track previous strings and is generally not recommended for anchor generation), use the named export slug: import {slug} from 'github-slugger' slug('foo bar baz') // returns 'foo-bar-baz' slug('foo bar baz') // returns 'foo-bar-baz' When using the GithubSlugger class, you must use the new keyword to create an instance, a change introduced in version 2.0.0 [3]. The library is not a markdown or HTML parser; it expects the plain text value of a heading as input [1][2].
Citations:
- 1: https://github.com/Flet/github-slugger/
- 2: https://www.npmjs.com/package/github-slugger
- 3: Use ESM Flet/github-slugger#43
🌐 Web query:
github Flet github-slugger 2.0.0 regular expression _slug regex
💡 Result:
The github-slugger package (version 2.0.0 and later) generates slugs by emulating GitHub's markdown heading anchor generation [1][2]. It does not rely on a single static regular expression defined in its main entry point [1][3]. Instead, it uses a generated regular expression file, regex.js, to filter characters [3][4]. The package maintains a custom regex filter that is built to include Unicode character blocks that GitHub filters out when creating slugs [5]. This approach replaced an earlier dependency on emoji-regex to better cover the specific Unicode characters that GitHub ignores [5]. The internal slug generation logic generally works by taking the input string, removing characters that do not fit the allowed Unicode criteria (using the generated regex), and normalizing the output [6][5]. Because this package aims to track GitHub's behavior, which is not fully documented or open-source in its internal implementation, the developers use a combination of Unicode blocks and iterative testing to update this regex to match GitHub's observed behavior [6][5]. The library exposes a primary class, GithubSlugger, and a static slug function for generating these slugs [1][7][8].
Citations:
- 1: https://www.npmjs.com/package/github-slugger
- 2: https://github.com/flet/github-slugger
- 3: https://registry.npmjs.org/github-slugger
- 4: https://npmx.dev/diff/github-slugger/v/1.5.0...2.0.0
- 5: Use custom unicode regex filter in place of emoji-regex Flet/github-slugger#25
- 6: Github's regex is probably
[^\w -]from html-pipeline Flet/github-slugger#56 - 7: feat(static): expose slug function Flet/github-slugger#29
- 8: Use ESM Flet/github-slugger#43
Sé que el enlace profundo debe apuntar al bloque ASCII equivalente.
El texto puede generar un ancla con caracteres no ASCII (medir-el-índice-residual-y-comprobar-la-sonda), pero Astro suele publicar los anchor id como ASCII URL-escaped. Como el mismo enlace usa la forma española con í, añade un <span id="medir-el-indice-residual-y-comprobar-la-sonda"></span> para que el deep link no dependa de la generación de slug del encabezado.
🤖 Prompt for AI Agents
Verify each finding against current code. Fix only still-valid issues, skip the
rest with a brief reason, keep changes minimal, and validate.
In `@site/src/content/docs/es/devices/emission/intensity.mdx` at line 408, En el
encabezado “Medir el índice residual, y comprobar la sonda”, añade un span vacío
con el id ASCII “medir-el-indice-residual-y-comprobar-la-sonda” para garantizar
que el enlace profundo funcione independientemente del slug generado por Astro.
Comment on lines
978
to
+983
| - Attenborough, K., & Van Renterghem, T. (2021). *Predicting outdoor sound* | ||
| (2nd ed.). CRC Press. | ||
| [doi:10.1201/9780429470141](https://doi.org/10.1201/9780429470141). Chapter | ||
| 11 (refraction by wind and temperature gradients, ray models and shadow | ||
| zones). ISBN 978-1-138-30655-2. Cited by | ||
| [doi:10.1201/9780429470806](https://doi.org/10.1201/9780429470806). Chapters | ||
| 2 and 9 (spherical-wave ground reflection; outdoor barriers) and Chapter 11 | ||
| (refraction by wind and temperature gradients, ray models and shadow | ||
| zones). ISBN 978-1-4987-4007-4 (hbk), 978-0-429-47080-6 (ebk). Cited by |
There was a problem hiding this comment.
📐 Maintainability & Code Quality | 🟡 Minor | ⚡ Quick win
Merge the duplicate Attenborough and Van Renterghem entries.
Each changed entry duplicates an earlier citation with the same 2021 second edition and DOI. Merge the chapter coverage, ISBNs, and guide links into the existing entry. Keep one entry per language.
site/src/content/docs/reference/bibliography.md#L978-L983: merge this content into the entry at Lines 904-909, then remove this duplicate.site/src/content/docs/es/reference/bibliography.md#L1023-L1030: merge this content into the entry at Lines 946-952, then remove this duplicate.
📍 Affects 2 files
site/src/content/docs/reference/bibliography.md#L978-L983(this comment)site/src/content/docs/es/reference/bibliography.md#L1023-L1030
🤖 Prompt for AI Agents
Verify each finding against current code. Fix only still-valid issues, skip the
rest with a brief reason, keep changes minimal, and validate.
In `@site/src/content/docs/reference/bibliography.md` around lines 978 - 983,
Merge the duplicate Attenborough and Van Renterghem citation into the existing
English entry at site/src/content/docs/reference/bibliography.md lines 904-909,
incorporating its chapter coverage, ISBNs, and guide links, then remove the
duplicate at lines 978-983. Apply the same merge to the existing Spanish entry
at site/src/content/docs/es/reference/bibliography.md lines 946-952,
incorporating the duplicate content and removing the duplicate at lines
1023-1030; retain one entry per language.
|
Contributor
Numerical conformance report✅ 533/533 conformance checks pass across 57 domains and 362 standards - filters class 1 - weightings within IEC 61672-1 class 1. Each row pins a standard clause to its expected normative value and the value the library computes. Every section below is collapsible and stays collapsed while all of its rows pass; a section with any failing row opens automatically. ✅ Numerical validation - filters & weightings: class showcase (IEC 61260-1 · IEC 61672-1 · ISO 7196)IEC 61260-1:2014 class per filter architecture (order 6, one-third-octave, 100 Hz-10 kHz, fs = 48 kHz). For each architecture the table shows, at its binding band, the measured relative attenuation and the class-1 limit it must clear, so the number and the range it must sit in are both visible. A positive margin means the acceptance limits are met with that much room.
Only Butterworth (the library default) and Chebyshev-II are class-compliant architectures. Chebyshev-I and elliptic trade the mask for passband ripple, and Bessel for a maximally-flat group delay (soft rolloff); they cannot satisfy the IEC 61260-1 Class 1/2 attenuation mask by construction, so they are labelled By design - this is expected, not a failure or regression. Frequency-weighting conformance (A/C: IEC 61672-1 Table 3; G: ISO 7196 A.3). The max deviation from nominal is informational (it falls at a frequency extreme where the tolerance is widest and asymmetric); compliance is judged at the binding frequency - the one with the least headroom - where the deviation, the applicable tolerance band and the headroom are shown together.
✅ Filters & weightings: 100% (10/10)
✅ Levels & dosimetry: 100% (9/9)
✅ Room & building acoustics: 100% (72/72)
✅ Room acoustics: 100% (16/16)
✅ Psychoacoustics: 100% (14/14)
✅ Speech transmission (IEC 60268-16): 100% (10/10)
✅ System measurement (Golay / Kirkeby / Mueller-Massarani): 100% (5/5)
✅ Intensity & sound power: 100% (10/10)
✅ Building prediction & uncertainty: 100% (15/15)
✅ Outdoor propagation & occupational exposure: 100% (10/10)
✅ Materials: absorption, airflow & impedance: 100% (6/6)
✅ Scattering & diffusion (ISO 17497): 100% (14/14)
✅ In-situ road absorption (ISO 13472): 100% (3/3)
✅ Precision sound power (ISO 3745 / 9614-3): 100% (4/4)
✅ Human vibration (ISO 8041 / 2631 / 5349): 100% (15/15)
✅ Speech intelligibility (ANSI S3.5-1997): 100% (24/24)
✅ Objective intelligibility (STOI / ESTOI): 100% (3/3)
✅ Impulsive-sound prominence (NT ACOU 112): 100% (2/2)
✅ Impulsive-sound prominence (ISO/PAS 1996-3): 100% (2/2)
✅ Room noise (ANSI S12.2-2019): 100% (3/3)
✅ Hearing threshold (ISO 7029 / ISO 389-7): 100% (3/3)
✅ Measurement uncertainty (GUM / Supplement 1): 100% (7/7)
✅ Noise-induced hearing loss (ISO 1999): 100% (6/6)
✅ Multiple-shock whole-body vibration (ISO 2631-5): 100% (6/6)
✅ Sound absorption in enclosed spaces (EN 12354-6): 100% (2/2)
✅ Prominent discrete tones (ECMA-418-1): 100% (2/2)
✅ Tonal audibility (ISO/PAS 20065): 100% (11/11)
✅ Psychoacoustic annoyance & fluctuation strength (Fastl & Zwicker): 100% (3/3)
✅ Electroacoustics: distortion & frequency response: 100% (20/20)
✅ Calibrated spectral analysis (Bendat & Piersol): 100% (12/12)
✅ Multiple-input coherence (Bendat & Piersol): 100% (5/5)
✅ Time-frequency analysis (Bendat & Piersol): 100% (3/3)
✅ Correlation, time delay and envelope (B&P / Knapp & Carter): 100% (7/7)
✅ Cepstrum, liftering and envelope spectrum (Havelock / B&P): 100% (3/3)
✅ Time synchronous averaging (McFadden 1987): 100% (5/5)
✅ Data qualification and Rice statistics (Bendat & Piersol): 100% (8/8)
✅ Underwater acoustics (ISO 18405/17208/18406): 100% (6/6)
✅ Underwater sound propagation (transmission loss): 100% (16/16)
✅ Underwater propagation regimes (Weston flux theory): 100% (3/3)
✅ Marine-mammal auditory weighting (NMFS / Southall): 100% (4/4)
✅ Underwater numerical propagation (modes / rays / PE): 100% (4/4)
✅ Aircraft noise (ICAO Annex 16 / IEC 61265): 100% (15/15)
✅ Rotorcraft noise (ECAC Doc 32 / NORAH2): 100% (12/12)
✅ CNOSSOS-EU road source (Directive 2002/49/EC Annex II): 100% (6/6)
✅ Wind-turbine noise (IEC 61400-11): 100% (3/3)
✅ Porous & multilayer absorbers (Mechel / Bies / Cox & D'Antonio): 100% (20/20)
✅ Slow-sound perfect absorbers (Jimenez et al. Appl. Sci. 2017): 100% (3/3)
✅ Program loudness (ITU-R BS.1770 / EBU R 128): 100% (8/8)
✅ 2D FDTD wave simulation (Attenborough & Van Renterghem 2021, Ch. 4): 100% (4/4)
✅ Swept-sine distortion & phase utilities (Farina / Novak): 100% (7/7)
✅ Spherical ground & barriers (Attenborough / Salomons / Bies): 100% (7/7)
✅ Panel & aperture sound insulation (Bies / Hopkins / Cremer): 100% (17/17)
✅ Bending-wave plate-junction transmission (Cremer / Craik / Hopkins): 100% (6/6)
✅ Atmospheric refraction (Salomons rays / GFPE): 100% (3/3)
✅ Electroacoustics: 100% (9/9)
✅ Industrial noise control: 100% (22/22)
✅ CNOSSOS-EU railway source (Directive 2002/49/EC Annex II): 100% (8/8)
Tests & coverage — 48204 tests, 0 failures (✅ all green)
Conformance harness: |
Comment on lines
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| gradients = np.geomspace(0.02, 0.4, 160) | ||
| _fig, ax = plt.subplots(figsize=(11, 6.2)) | ||
| pairs = ((0.5, 1.5, COLOR_PRIMARY), (2.0, 2.0, COLOR_TERTIARY), | ||
| (2.0, 10.0, COLOR_SECONDARY)) | ||
| for hs, hr, color in pairs: | ||
| ax.loglog(gradients, | ||
| [shadow_zone_distance(-float(g), hs, hr, ground_speed=340.0) | ||
| for g in gradients], color=color, linewidth=2.0, | ||
| label=f"hs / hr = {hs:g} / {hr:g} m", zorder=4) | ||
| ax.axvline(0.1, color=COLOR_MUTED, linestyle="--", linewidth=1.3, zorder=2) | ||
| ax.plot([0.1], [shadow_zone_distance(-0.1, 2.0, 2.0, ground_speed=340.0)], | ||
| "o", color=COLOR_FG, markersize=8, zorder=5) | ||
| ax.annotate("representative −0.1 s⁻¹: 233 m", | ||
| xy=(0.1, 233.2), xytext=(0.022, 90.0), fontsize=10, | ||
| color=COLOR_FG, | ||
| arrowprops={"arrowstyle": "->", "color": COLOR_MUTED}) | ||
| grad_log = 1.0 * np.log(101.0) / 10.0 | ||
| ax.plot([grad_log], | ||
| [shadow_zone_distance(-grad_log, 2.0, 2.0, ground_speed=340.0)], | ||
| "s", color=COLOR_SECONDARY, markersize=8, zorder=5) | ||
| ax.annotate("the page's b = −1 m/s case: 109 m", | ||
| xy=(grad_log, 108.6), xytext=(0.12, 480.0), fontsize=10, | ||
| color=COLOR_FG, | ||
| arrowprops={"arrowstyle": "->", "color": COLOR_MUTED}) |
There was a problem hiding this comment.
🎯 Functional Correctness | 🟡 Minor | ⚡ Quick win
The second marker falls outside the swept gradient range.
gradients spans 0.02 to 0.4, but grad_log = ln(101)/10 ≈ 0.4615. The marker and its annotation at lines 1192-1198 therefore sit beyond the right-hand end of all three curves, and the autoscale stretches the x axis past the 0.4 limit the alt text in site/src/content/docs/environment/propagation/atmospheric-refraction.mdx describes (Rc from 17 km down to 850 m). Extend the sweep so the marker lands on the middle curve.
📈 Proposed fix
- gradients = np.geomspace(0.02, 0.4, 160)
+ gradients = np.geomspace(0.02, 0.5, 160)📝 Committable suggestion
‼️ IMPORTANT
Carefully review the code before committing. Ensure that it accurately replaces the highlighted code, contains no missing lines, and has no issues with indentation. Thoroughly test & benchmark the code to ensure it meets the requirements.
Suggested change
| gradients = np.geomspace(0.02, 0.4, 160) | |
| _fig, ax = plt.subplots(figsize=(11, 6.2)) | |
| pairs = ((0.5, 1.5, COLOR_PRIMARY), (2.0, 2.0, COLOR_TERTIARY), | |
| (2.0, 10.0, COLOR_SECONDARY)) | |
| for hs, hr, color in pairs: | |
| ax.loglog(gradients, | |
| [shadow_zone_distance(-float(g), hs, hr, ground_speed=340.0) | |
| for g in gradients], color=color, linewidth=2.0, | |
| label=f"hs / hr = {hs:g} / {hr:g} m", zorder=4) | |
| ax.axvline(0.1, color=COLOR_MUTED, linestyle="--", linewidth=1.3, zorder=2) | |
| ax.plot([0.1], [shadow_zone_distance(-0.1, 2.0, 2.0, ground_speed=340.0)], | |
| "o", color=COLOR_FG, markersize=8, zorder=5) | |
| ax.annotate("representative −0.1 s⁻¹: 233 m", | |
| xy=(0.1, 233.2), xytext=(0.022, 90.0), fontsize=10, | |
| color=COLOR_FG, | |
| arrowprops={"arrowstyle": "->", "color": COLOR_MUTED}) | |
| grad_log = 1.0 * np.log(101.0) / 10.0 | |
| ax.plot([grad_log], | |
| [shadow_zone_distance(-grad_log, 2.0, 2.0, ground_speed=340.0)], | |
| "s", color=COLOR_SECONDARY, markersize=8, zorder=5) | |
| ax.annotate("the page's b = −1 m/s case: 109 m", | |
| xy=(grad_log, 108.6), xytext=(0.12, 480.0), fontsize=10, | |
| color=COLOR_FG, | |
| arrowprops={"arrowstyle": "->", "color": COLOR_MUTED}) | |
| gradients = np.geomspace(0.02, 0.5, 160) | |
| _fig, ax = plt.subplots(figsize=(11, 6.2)) | |
| pairs = ((0.5, 1.5, COLOR_PRIMARY), (2.0, 2.0, COLOR_TERTIARY), | |
| (2.0, 10.0, COLOR_SECONDARY)) | |
| for hs, hr, color in pairs: | |
| ax.loglog(gradients, | |
| [shadow_zone_distance(-float(g), hs, hr, ground_speed=340.0) | |
| for g in gradients], color=color, linewidth=2.0, | |
| label=f"hs / hr = {hs:g} / {hr:g} m", zorder=4) | |
| ax.axvline(0.1, color=COLOR_MUTED, linestyle="--", linewidth=1.3, zorder=2) | |
| ax.plot([0.1], [shadow_zone_distance(-0.1, 2.0, 2.0, ground_speed=340.0)], | |
| "o", color=COLOR_FG, markersize=8, zorder=5) | |
| ax.annotate("representative −0.1 s⁻¹: 233 m", | |
| xy=(0.1, 233.2), xytext=(0.022, 90.0), fontsize=10, | |
| color=COLOR_FG, | |
| arrowprops={"arrowstyle": "->", "color": COLOR_MUTED}) | |
| grad_log = 1.0 * np.log(101.0) / 10.0 | |
| ax.plot([grad_log], | |
| [shadow_zone_distance(-grad_log, 2.0, 2.0, ground_speed=340.0)], | |
| "s", color=COLOR_SECONDARY, markersize=8, zorder=5) | |
| ax.annotate("the page's b = −1 m/s case: 109 m", | |
| xy=(grad_log, 108.6), xytext=(0.12, 480.0), fontsize=10, | |
| color=COLOR_FG, | |
| arrowprops={"arrowstyle": "->", "color": COLOR_MUTED}) |
🤖 Prompt for AI Agents
Verify each finding against current code. Fix only still-valid issues, skip the
rest with a brief reason, keep changes minimal, and validate.
In `@scripts/figures/environment.py` around lines 1175 - 1198, Extend the
`gradients` range in the plotting code so it includes `grad_log` (approximately
0.4615), while preserving the existing curve generation and marker placement.
Ensure the second marker and annotation fall within the swept curves and the
plotted x-axis range matches the documented Rc coverage.
Comment on lines
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| speeds = np.linspace(60.0, 350.0, 40) | ||
| for row, label, color in ((0, "Source A (0,5 m)", COLOR_PRIMARY), | ||
| (1, "Source B (4,0 m)", COLOR_SECONDARY)): | ||
| right.plot(speeds, [ | ||
| total(railway_source_power( | ||
| RailwayVehicle(stock, flow_rate=96.0, speed=float(v)), track, | ||
| phi=90.0, psi=10.0).line_power[row]) for v in speeds], | ||
| color=color, linewidth=2.0, label=label, zorder=4) |
There was a problem hiding this comment.
🚀 Performance & Scalability | 🔵 Trivial | ⚡ Quick win
railway_source_power runs twice per speed.
The row loop wraps the list comprehension, so each of the 40 speeds evaluates railway_source_power once for row 0 and again for row 1. Compute the results once and index both rows.
♻️ Proposed refactor
speeds = np.linspace(60.0, 350.0, 40)
+ powers = [railway_source_power(
+ RailwayVehicle(stock, flow_rate=96.0, speed=float(v)), track,
+ phi=90.0, psi=10.0).line_power for v in speeds]
for row, label, color in ((0, "Source A (0,5 m)", COLOR_PRIMARY),
(1, "Source B (4,0 m)", COLOR_SECONDARY)):
- right.plot(speeds, [
- total(railway_source_power(
- RailwayVehicle(stock, flow_rate=96.0, speed=float(v)), track,
- phi=90.0, psi=10.0).line_power[row]) for v in speeds],
- color=color, linewidth=2.0, label=label, zorder=4)
+ right.plot(speeds, [total(p[row]) for p in powers],
+ color=color, linewidth=2.0, label=label, zorder=4)📝 Committable suggestion
‼️ IMPORTANT
Carefully review the code before committing. Ensure that it accurately replaces the highlighted code, contains no missing lines, and has no issues with indentation. Thoroughly test & benchmark the code to ensure it meets the requirements.
Suggested change
| speeds = np.linspace(60.0, 350.0, 40) | |
| for row, label, color in ((0, "Source A (0,5 m)", COLOR_PRIMARY), | |
| (1, "Source B (4,0 m)", COLOR_SECONDARY)): | |
| right.plot(speeds, [ | |
| total(railway_source_power( | |
| RailwayVehicle(stock, flow_rate=96.0, speed=float(v)), track, | |
| phi=90.0, psi=10.0).line_power[row]) for v in speeds], | |
| color=color, linewidth=2.0, label=label, zorder=4) | |
| speeds = np.linspace(60.0, 350.0, 40) | |
| powers = [railway_source_power( | |
| RailwayVehicle(stock, flow_rate=96.0, speed=float(v)), track, | |
| phi=90.0, psi=10.0).line_power for v in speeds] | |
| for row, label, color in ((0, "Source A (0,5 m)", COLOR_PRIMARY), | |
| (1, "Source B (4,0 m)", COLOR_SECONDARY)): | |
| right.plot(speeds, [total(p[row]) for p in powers], | |
| color=color, linewidth=2.0, label=label, zorder=4) |
🤖 Prompt for AI Agents
Verify each finding against current code. Fix only still-valid issues, skip the
rest with a brief reason, keep changes minimal, and validate.
In `@scripts/figures/environment.py` around lines 1456 - 1463, Update the plotting
loop around railway_source_power to compute and retain each speed’s result once,
then build each row’s plotted values by indexing the cached results rather than
invoking railway_source_power separately for row 0 and row 1.
Comment on lines
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| gives $b = 4 / \ln(101) = 0.87$ m/s — close to the "+1 m/s typical" above, and | ||
| `log_linear_sound_speed_profile(0.867)` duly returns 344.0 m/s at 10 m. |
There was a problem hiding this comment.
🎯 Functional Correctness | 🟡 Minor | ⚡ Quick win
🧩 Analysis chain
🏁 Script executed:
#!/bin/bash
# Read the declared default of ground_speed.
ast-grep run --pattern 'def log_linear_sound_speed_profile($$$)' --lang python src/phonometry/environment/propagation/refraction.py
rg -n -A6 'def log_linear_sound_speed_profile' src/phonometry/environment/propagation/refraction.pyRepository: jmrplens/phonometry
Length of output: 5600
🏁 Script executed:
#!/bin/bash
set -euo pipefail
echo "== Candidate markdown lines =="
nl -ba site/src/content/docs/environment/propagation/atmospheric-refraction.mdx | sed -n '130,160p'
echo
echo "== All log_linear_sound_speed_profile calls in target doc =="
rg -n -C2 'log_linear_sound_speed_profile|344\.0|340\.0|ground_speed' site/src/content/docs/environment/propagation/atmospheric-refraction.mdx
echo
echo "== Nearby implementation behavior probe source =="
nl -ba src/phonometry/environment/propagation/refraction.py | sed -n '140,160p'
nl -ba src/phonometry/environment/propagation/refraction.py | sed -n '170,196p'Repository: jmrplens/phonometry
Length of output: 228
🏁 Script executed:
#!/bin/bash
set -euo pipefail
echo "== Candidate markdown lines =="
awk '{printf "%5d %s\n", NR, $0}' site/src/content/docs/environment/propagation/atmospheric-refraction.mdx | sed -n '130,160p'
echo
echo "== All log_linear_sound_speed_profile calls in target doc =="
rg -n -C2 'log_linear_sound_speed_profile|344\.0|340\.0|ground_speed' site/src/content/docs/environment/propagation/atmospheric-refraction.mdx || true
echo
echo "== Nearby implementation behavior probe source =="
awk '{printf "%5d %s\n", NR, $0}' src/phonometry/environment/propagation/refraction.py | sed -n '140,160p'
awk '{printf "%5d %s\n", NR, $0}' src/phonometry/environment/propagation/refraction.py | sed -n '170,196p'Repository: jmrplens/phonometry
Length of output: 9562
Specify ground_speed in the call that asserts 344.0 m/s.
log_linear_sound_speed_profile(0.867) only returns 344.0 m/s at 10 m with ground_speed=340.0. Add ground_speed=340.0 or state the default explicitly.
🤖 Prompt for AI Agents
Verify each finding against current code. Fix only still-valid issues, skip the
rest with a brief reason, keep changes minimal, and validate.
In `@site/src/content/docs/environment/propagation/atmospheric-refraction.mdx`
around lines 148 - 149, Update the log_linear_sound_speed_profile example call
to explicitly pass ground_speed=340.0 while preserving the assertion that it
returns 344.0 m/s at 10 m.
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| <ThemeImage src="https://raw.githubusercontent.com/jmrplens/phonometry/main/.github/images/diagram_wind_turbine_board.svg" alt="Two panels of the IEC 61400-11 ground-board microphone mounting. Plan: the circular board with its minimum diameter of 1.0 m dimensioned, the microphone at the centre with its axis pointing at the turbine, and the optional split line drawn off the centre line and parallel to that axis with its maximum 1 mm gap called out. Section: the board edge with a soil fillet levelling the gap underneath, the board thickness annotated as at least 12.0 mm for plywood or hard chip-board and at least 2.5 mm for metal, the capsule with its diaphragm in the plane of the board and a diameter of at most 13 mm, the primary windscreen drawn as a half sphere of open-cell foam about 90 mm across centred on the diaphragm, and a ghosted secondary windscreen tagged as usable only in high wind and only if its insertion loss is documented and corrected band by band" width="92%" /> | ||
|
|
||
| | Requirement | Value | Clause | | ||
| | :--- | :--- | :--- | | ||
| | Measurement chain | IEC 61672 class 1; filters IEC 61260 class 1; 1/3 octaves from 20 Hz to 10 kHz determined simultaneously; narrowband over 20 Hz to 11 200 Hz | 6.1.2, 6.1.3, 6.1.4 | | ||
| | Microphone diaphragm | ≤ 13 mm, in a plane **normal to the board**, axis pointing at the turbine | 6.1.2, 6.1.5 | | ||
| | Board | Circular, diameter ≥ 1,0 m, acoustically hard: plywood or hard chip-board ≥ 12,0 mm, or metal ≥ 2,5 mm | 6.1.5 | | ||
| | A split board | Pieces level in one plane, gap < 1 mm, split off the centre line and **parallel** to the microphone axis | 6.1.5 | |
There was a problem hiding this comment.
🎯 Functional Correctness | 🟡 Minor | ⚡ Quick win
Contradictory microphone-mounting geometry in both editions. The requirements table and the figure alt text describe two incompatible mountings for the same IEC 61400-11 6.1.5 board microphone: the alt text places the diaphragm in the plane of the board, the table places it in a plane normal to the board with the axis pointing at the turbine. The split-board row depends on which geometry is correct.
site/src/content/docs/environment/sources/wind-turbine-noise.mdx#L67-L74: align the "Microphone diaphragm" row at Line 72 with the alt-text geometry at Line 67, and re-check the split-board row at Line 74.site/src/content/docs/es/environment/sources/wind-turbine-noise.mdx#L69-L74: apply the same correction to the "Diafragma del micrófono" row at Line 74 and to the alt text at Line 69.
📍 Affects 2 files
site/src/content/docs/environment/sources/wind-turbine-noise.mdx#L67-L74(this comment)site/src/content/docs/es/environment/sources/wind-turbine-noise.mdx#L69-L74
🤖 Prompt for AI Agents
Verify each finding against current code. Fix only still-valid issues, skip the
rest with a brief reason, keep changes minimal, and validate.
In `@site/src/content/docs/environment/sources/wind-turbine-noise.mdx` around
lines 67 - 74, Align the microphone-mounting geometry across both language
versions: in site/src/content/docs/environment/sources/wind-turbine-noise.mdx
lines 67-74, update the “Microphone diaphragm” row to match the figure alt
text’s diaphragm-in-board-plane geometry and re-check the split-board
requirement; in
site/src/content/docs/es/environment/sources/wind-turbine-noise.mdx lines 69-74,
apply the same correction to the alt text and “Diafragma del micrófono” row,
ensuring both split-board descriptions remain consistent.
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| <ThemeImage src="https://raw.githubusercontent.com/jmrplens/phonometry/main/.github/images/wind_turbine_audibility_criterion.svg" alt="Two panels against tone frequency on a logarithmic axis from 20 Hz to 10 kHz. Left: the IEC 61400-11 critical bandwidth, flat near 100 Hz through the low and mid bands and opening steeply above 500 Hz to 2 kHz wide at 10 kHz, with the fixed 20 to 120 Hz low-frequency band of subclause 9.5.3 drawn as a separate flat segment over the 20 to 70 Hz candidate range and the ISO 1996-2 Table C.1 bandwidth drawn as a stepped dashed line for contrast. Right: the audibility criterion La, which falls from minus 2 dB at low frequency to minus 4.5 dB at 5 kHz, redrawn as the tonality a tone must reach to be audible and to be reportable, so a 100 Hz tone needs about half a decibel more emergence than a 1 kHz one" width="88%" /> | ||
|
|
||
| *Left: two different critical bandwidths live on this page. The IEC 61400-11 | ||
| Zwicker band is what `WindTurbineTonalityResult.critical_bandwidth` reports | ||
| (117.3 Hz for the 500 Hz tone of the fiche below), while | ||
| `environment.critical_bandwidth` is the **ISO 1996-2 Table C.1** band — 100 Hz | ||
| up to 500 Hz and 20 % of $f_c$ above it — used by the ISO tonal-audibility | ||
| route on the environmental-levels page. They are not interchangeable. Right: the | ||
| criterion is nearly flat below 500 Hz and then tightens, so a low-frequency tone | ||
| is judged on almost the same emergence as a mid-frequency one; the reportable | ||
| line sits 3 dB below the audible one everywhere.* |
There was a problem hiding this comment.
🎯 Functional Correctness | 🟡 Minor | ⚡ Quick win
The audibility-criterion alt text reverses the frequency dependence in both editions. The plotted quantity is -la, which equals 2.01 dB at 100 Hz and 2.82 dB at 1 kHz, so the plot requires more tonality at 1 kHz. Both alt texts state the opposite, while both body captions agree with the plot.
site/src/content/docs/environment/sources/wind-turbine-noise.mdx#L211-L221: correct the alt text at Line 211 so the 1 kHz tone, not the 100 Hz tone, needs the larger emergence, and state the difference as about 0.8 dB.site/src/content/docs/es/environment/sources/wind-turbine-noise.mdx#L222-L233: apply the same correction to the alt text at Line 222.
📍 Affects 2 files
site/src/content/docs/environment/sources/wind-turbine-noise.mdx#L211-L221(this comment)site/src/content/docs/es/environment/sources/wind-turbine-noise.mdx#L222-L233
🤖 Prompt for AI Agents
Verify each finding against current code. Fix only still-valid issues, skip the
rest with a brief reason, keep changes minimal, and validate.
In `@site/src/content/docs/environment/sources/wind-turbine-noise.mdx` around
lines 211 - 221, The audibility-criterion alt text reverses the frequency
dependence. Update the English alt text in
site/src/content/docs/environment/sources/wind-turbine-noise.mdx lines 211-221
and the Spanish alt text in
site/src/content/docs/es/environment/sources/wind-turbine-noise.mdx lines
222-233 so they state that the 1 kHz tone requires more emergence than the 100
Hz tone, by about 0.8 dB, while preserving the rest of the descriptions.
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| Tres argumentos con nombre de esa llamada deciden si el número es defendible, y | ||
| ninguno es opcional en la práctica: | ||
|
|
||
| | Argumento | Por defecto | Qué hace | | ||
| | :--- | :--- | :--- | | ||
| | `dt` | `0.02` s | El intervalo de registro del historial de nivel. El método necesita de 10 ms a 25 ms; una rejilla más gruesa aplana la tasa de crecimiento ajustada y subestima $P$, que es la advertencia de dos párrafos más abajo hecha configurable | | ||
| | `calibration_offset` | `0.0` dB | Se suma al historial de nivel para tender un puente entre una escala digital y una calibrada: la diferencia entre el nivel conocido del calibrador y el nivel que este mismo procesado declara para la grabación de calibración. Mueve el $L_{Aeq}$ y el $L_{Aeq}$ ajustado, y deja $K_I$ en paz | | ||
| | `laeq` | `None` | Pasa el $L_{Aeq}$ medido sobre el periodo de evaluación en vez de dejar que se calcule a partir del extracto, que es lo que hace un informe real | | ||
| | `reference_pressure` | `2e-05` Pa | Solo se cambia para un medio distinto del aire | | ||
| | `onset_rate_method` | `'least_squares'` | El ajuste sobre la subida detectada | |
There was a problem hiding this comment.
📐 Maintainability & Code Quality | 🟡 Minor | ⚡ Quick win
Corrige el recuento de argumentos.
La línea 230 anuncia "Tres argumentos con nombre". La tabla de las líneas 233-239 enumera cinco: dt, calibration_offset, laeq, reference_pressure y onset_rate_method.
Ajusta el número al contenido de la tabla, o separa los tres argumentos determinantes de los dos restantes.
✏️ Corrección propuesta
-Tres argumentos con nombre de esa llamada deciden si el número es defendible, y
-ninguno es opcional en la práctica:
+Cinco argumentos con nombre de esa llamada deciden si el número es defendible, y
+los tres primeros no son opcionales en la práctica:📝 Committable suggestion
‼️ IMPORTANT
Carefully review the code before committing. Ensure that it accurately replaces the highlighted code, contains no missing lines, and has no issues with indentation. Thoroughly test & benchmark the code to ensure it meets the requirements.
Suggested change
| Tres argumentos con nombre de esa llamada deciden si el número es defendible, y | |
| ninguno es opcional en la práctica: | |
| | Argumento | Por defecto | Qué hace | | |
| | :--- | :--- | :--- | | |
| | `dt` | `0.02` s | El intervalo de registro del historial de nivel. El método necesita de 10 ms a 25 ms; una rejilla más gruesa aplana la tasa de crecimiento ajustada y subestima $P$, que es la advertencia de dos párrafos más abajo hecha configurable | | |
| | `calibration_offset` | `0.0` dB | Se suma al historial de nivel para tender un puente entre una escala digital y una calibrada: la diferencia entre el nivel conocido del calibrador y el nivel que este mismo procesado declara para la grabación de calibración. Mueve el $L_{Aeq}$ y el $L_{Aeq}$ ajustado, y deja $K_I$ en paz | | |
| | `laeq` | `None` | Pasa el $L_{Aeq}$ medido sobre el periodo de evaluación en vez de dejar que se calcule a partir del extracto, que es lo que hace un informe real | | |
| | `reference_pressure` | `2e-05` Pa | Solo se cambia para un medio distinto del aire | | |
| | `onset_rate_method` | `'least_squares'` | El ajuste sobre la subida detectada | | |
| Cinco argumentos con nombre de esa llamada deciden si el número es defendible, y | |
| los tres primeros no son opcionales en la práctica: | |
| | Argumento | Por defecto | Qué hace | | |
| | :--- | :--- | :--- | | |
| | `dt` | `0.02` s | El intervalo de registro del historial de nivel. El método necesita de 10 ms a 25 ms; una rejilla más gruesa aplana la tasa de crecimiento ajustada y subestima $P$, que es la advertencia de dos párrafos más abajo hecha configurable | | |
| | `calibration_offset` | `0.0` dB | Se suma al historial de nivel para tender un puente entre una escala digital y una calibrada: la diferencia entre el nivel conocido del calibrador y el nivel que este mismo procesado declara para la grabación de calibración. Mueve el $L_{Aeq}$ y el $L_{Aeq}$ ajustado, y deja $K_I$ en paz | | |
| | `laeq` | `None` | Pasa el $L_{Aeq}$ medido sobre el periodo de evaluación en vez de dejar que se calcule a partir del extracto, que es lo que hace un informe real | | |
| | `reference_pressure` | `2e-05` Pa | Solo se cambia para un medio distinto del aire | | |
| | `onset_rate_method` | `'least_squares'` | El ajuste sobre la subida detectada | |
🤖 Prompt for AI Agents
Verify each finding against current code. Fix only still-valid issues, skip the
rest with a brief reason, keep changes minimal, and validate.
In `@site/src/content/docs/es/environment/assessment/impulsive-sound.mdx` around
lines 230 - 239, Corrige el encabezado introductorio de esta sección para que
coincida con los cinco argumentos enumerados en la tabla (`dt`,
`calibration_offset`, `laeq`, `reference_pressure` y `onset_rate_method`), o
separa explícitamente los tres argumentos determinantes de los otros dos sin
alterar la tabla.
Comment on lines
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| *Los dos procedimientos están lo bastante cerca como para confundirse y lo | ||
| bastante lejos como para discrepar sobre un espectro real. Una banda de 250 Hz | ||
| que sobresale 7,5 dB de la media aritmética de sus vecinas queda graduada con | ||
| $K_t = 3$ dB por el reglamento y **no levanta ningún indicador** en el método de | ||
| cribado de ISO, porque supera a cada vecina en menos de los 8 dB que ese método | ||
| exige. Esa es exactamente la situación que un informe de inspección tiene que | ||
| saber defender: el RD compara contra la **media** aritmética de las vecinas con | ||
| umbrales 8/5/3 dB y gradúa el resultado en 0/3/6; el método de cribado exige que | ||
| la banda supere a **ambas** vecinas en 15/8/5 dB y devuelve un indicador; el | ||
| método de ingeniería del anexo C trabaja dentro de una banda crítica y devuelve | ||
| un valor continuo.* |
There was a problem hiding this comment.
🎯 Functional Correctness | 🟡 Minor | ⚡ Quick win
La razón que se da para el veredicto del cribado ISO no coincide con los números del ejemplo.
En el ejemplo del bloque de código, shallow[4] = 69,0 dB con vecinas de 61,0 dB (200 Hz) y 62,0 dB (315 Hz). La banda supera a la vecina de 200 Hz en exactamente 8,0 dB, no en menos de 8 dB. Lo que impide el indicador es la vecina de 315 Hz, superada solo en 7,0 dB.
Reformula la frase para nombrar la vecina que falla. Con 8,0 dB exactos en la otra vecina, el veredicto también depende de si el criterio es > o ≥.
✏️ Corrección propuesta
-$K_t = 3$ dB por el reglamento y **no levanta ningún indicador** en el método de
-cribado de ISO, porque supera a cada vecina en menos de los 8 dB que ese método
-exige.
+$K_t = 3$ dB por el reglamento y **no levanta ningún indicador** en el método de
+cribado de ISO, porque solo supera a la vecina de 315 Hz en 7,0 dB, por debajo de
+los 8 dB que ese método exige a **ambas** vecinas.📝 Committable suggestion
‼️ IMPORTANT
Carefully review the code before committing. Ensure that it accurately replaces the highlighted code, contains no missing lines, and has no issues with indentation. Thoroughly test & benchmark the code to ensure it meets the requirements.
Suggested change
| *Los dos procedimientos están lo bastante cerca como para confundirse y lo | |
| bastante lejos como para discrepar sobre un espectro real. Una banda de 250 Hz | |
| que sobresale 7,5 dB de la media aritmética de sus vecinas queda graduada con | |
| $K_t = 3$ dB por el reglamento y **no levanta ningún indicador** en el método de | |
| cribado de ISO, porque supera a cada vecina en menos de los 8 dB que ese método | |
| exige. Esa es exactamente la situación que un informe de inspección tiene que | |
| saber defender: el RD compara contra la **media** aritmética de las vecinas con | |
| umbrales 8/5/3 dB y gradúa el resultado en 0/3/6; el método de cribado exige que | |
| la banda supere a **ambas** vecinas en 15/8/5 dB y devuelve un indicador; el | |
| método de ingeniería del anexo C trabaja dentro de una banda crítica y devuelve | |
| un valor continuo.* | |
| *Los dos procedimientos están lo bastante cerca como para confundirse y lo | |
| bastante lejos como para discrepar sobre un espectro real. Una banda de 250 Hz | |
| que sobresale 7,5 dB de la media aritmética de sus vecinas queda graduada con | |
| $K_t = 3$ dB por el reglamento y **no levanta ningún indicador** en el método de | |
| cribado de ISO, porque solo supera a la vecina de 315 Hz en 7,0 dB, por debajo de | |
| los 8 dB que ese método exige a **ambas** vecinas. Esa es exactamente la situación que un informe de inspección tiene que | |
| saber defender: el RD compara contra la **media** aritmética de las vecinas con | |
| umbrales 8/5/3 dB y gradúa el resultado en 0/3/6; el método de cribado exige que | |
| la banda supere a **ambas** vecinas en 15/8/5 dB y devuelve un indicador; el | |
| método de ingeniería del anexo C trabaja dentro de una banda crítica y devuelve | |
| un valor continuo.* |
🤖 Prompt for AI Agents
Verify each finding against current code. Fix only still-valid issues, skip the
rest with a brief reason, keep changes minimal, and validate.
In `@site/src/content/docs/es/environment/assessment/spanish-noise-regulation.mdx`
around lines 191 - 201, Reformula el párrafo alrededor del ejemplo de 250 Hz
para indicar que el indicador no se activa porque la banda supera a la vecina de
315 Hz en solo 7 dB; no atribuyas el resultado a superar a cada vecina en menos
de 8 dB. Mantén explícita la condición del criterio de cribado para la
diferencia exacta de 8 dB respecto a la vecina de 200 Hz, usando la comparación
definida por el método.
Comment on lines
+532
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+536
| **Los cuatro modelos son pantallas bidimensionales infinitas.** Una barrera real | ||
| de longitud finita deja que el sonido la flanquee por los extremos, y dos | ||
| barreras paralelas a ambos lados de una vía se reflejan entre sí y pierden varios | ||
| decibelios de su prestación nominal. Ninguno de los dos efectos existe en ningún | ||
| modelo de esta página. |
There was a problem hiding this comment.
📐 Maintainability & Code Quality | 🟡 Minor | ⚡ Quick win
El recuento de modelos contradice al resto de la página.
La línea 532 dice "Los cuatro modelos son pantallas bidimensionales infinitas". La página describe tres modelos de apantallamiento: Kurze-Anderson, semiplano rígido exacto y el coherente de cuatro caminos. Así lo enuncian la línea 261 ("tres niveles de apantallamiento"), la línea 394 ("Los tres modelos lado a lado") y el apartado "Cuál usar" de las líneas 514-521.
El "cuatro" parece arrastrado de "cuatro caminos".
✏️ Corrección propuesta
-**Los cuatro modelos son pantallas bidimensionales infinitas.** Una barrera real
+**Los tres modelos son pantallas bidimensionales infinitas.** Una barrera real📝 Committable suggestion
‼️ IMPORTANT
Carefully review the code before committing. Ensure that it accurately replaces the highlighted code, contains no missing lines, and has no issues with indentation. Thoroughly test & benchmark the code to ensure it meets the requirements.
Suggested change
| **Los cuatro modelos son pantallas bidimensionales infinitas.** Una barrera real | |
| de longitud finita deja que el sonido la flanquee por los extremos, y dos | |
| barreras paralelas a ambos lados de una vía se reflejan entre sí y pierden varios | |
| decibelios de su prestación nominal. Ninguno de los dos efectos existe en ningún | |
| modelo de esta página. | |
| **Los tres modelos son pantallas bidimensionales infinitas.** Una barrera real | |
| de longitud finita deja que el sonido la flanquee por los extremos, y dos | |
| barreras paralelas a ambos lados de una vía se reflejan entre sí y pierden varios | |
| decibelios de su prestación nominal. Ninguno de los dos efectos existe en ningún | |
| modelo de esta página. |
🤖 Prompt for AI Agents
Verify each finding against current code. Fix only still-valid issues, skip the
rest with a brief reason, keep changes minimal, and validate.
In `@site/src/content/docs/es/environment/propagation/ground-barriers.mdx` around
lines 532 - 536, Corrige el recuento en el párrafo que comienza con “Los cuatro
modelos” para indicar que son tres modelos, manteniendo sin cambios la
explicación sobre pantallas bidimensionales infinitas y los efectos no
representados.
Comment on lines
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| ```python | ||
| for extra in (0.0, 0.001, 0.010, 0.050): # diferencia de recorrido sobre el borde [m] | ||
| libre = environment.Barrier(source_to_edge=100.0 + extra / 2, | ||
| edge_to_receiver=100.0 + extra / 2, | ||
| line_of_sight_clear=True) | ||
| print(round(float(environment.barrier_attenuation(libre, 200.0, [500.0])[0]), 3)) | ||
| # 4,771, 4,728, 4,323, 1,845 dB a 500 Hz | ||
| ``` |
There was a problem hiding this comment.
📐 Maintainability & Code Quality | 🟡 Minor | ⚡ Quick win
El comentario de salida usa coma decimal, al contrario que el resto del archivo.
La línea 780 documenta la salida de print(round(...)) como 4,771, 4,728, 4,323, 1,845. Python imprime punto decimal. Los demás comentarios de salida de este archivo mantienen el punto: líneas 440-443, 457, 461 y 548.
Usa punto decimal en este comentario para que un lector pueda comparar con lo que imprime el fragmento.
✏️ Corrección propuesta
-# 4,771, 4,728, 4,323, 1,845 dB a 500 Hz
+# 4.771, 4.728, 4.323, 1.845 dB a 500 Hz📝 Committable suggestion
‼️ IMPORTANT
Carefully review the code before committing. Ensure that it accurately replaces the highlighted code, contains no missing lines, and has no issues with indentation. Thoroughly test & benchmark the code to ensure it meets the requirements.
Suggested change
| ```python | |
| for extra in (0.0, 0.001, 0.010, 0.050): # diferencia de recorrido sobre el borde [m] | |
| libre = environment.Barrier(source_to_edge=100.0 + extra / 2, | |
| edge_to_receiver=100.0 + extra / 2, | |
| line_of_sight_clear=True) | |
| print(round(float(environment.barrier_attenuation(libre, 200.0, [500.0])[0]), 3)) | |
| # 4,771, 4,728, 4,323, 1,845 dB a 500 Hz | |
| ``` |
🤖 Prompt for AI Agents
Verify each finding against current code. Fix only still-valid issues, skip the
rest with a brief reason, keep changes minimal, and validate.
In `@site/src/content/docs/es/environment/propagation/outdoor-propagation.mdx`
around lines 774 - 781, Update the output comment following the loop to use
periods as decimal separators, matching Python’s print output and the file’s
other documented examples; change only the four documented values.
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The same contract as #512, for the pages that measure a machine, a transducer, a silencer and a landscape: how the number was obtained, and what it means. 215 findings closed across twenty-five English guides, with their Spanish twins.
Acquisition, from the clause
The instrumentation and geometry the six sound-power determination routes actually require (ISO 3741/3744/3745/9614/7849), the IEC 60268-3 operating point and the loudspeaker drive, the silencer substitution series of ISO 7235, the duct-path installation, and the provenance of every CNOSSOS input.
Numbers and claims that were wrong
P <= 0, notP < 0.directivity_indexis clause 8.4, not 8.6, and an Attenborough DOI resolved to the wrong edition.About forty new plates and figures
Among them: the IEC 61043 residual-intensity check with the ISO 9614-2 probe reversal and its verdict strip; the ISO 3744 parallelepiped in top and side view with the partial-area split; the ISO 3745 forty-position hemisphere coloured at the twenty-position escalation; the duct path drawn as a place, with the sheet codes of Long's Table 14.9 and the occupant at 1.83 m; a silencer whose insertion loss goes 22.6 dB negative near 180 Hz through the real radiation impedance of its open end; and the inter-sample excursion of the page's own tone at fs/4 against the closed-form under-read.
Terminology
This is the first translation written after the glossary was settled, so the terms were applied rather than decided, and the checker reports no warnings. The four rows that are deliberately open were respected: the solver is named by its method, the coincidence dip and the display gain are recast, and detrending keeps its feminine article.
Where a Spanish heading carries an accent, a link to it uses the ASCII
<span id>the corpus adopted in #508, because the percent-encoded slug reads as a dangling anchor to the accessibility audit.Checks
The full CI set locally, twenty five steps, including the figure regeneration that #512 added after finding that the staleness check had been comparing the committed files with themselves.
Summary by CodeRabbit