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emission.intensity

Two-microphone (p-p) sound intensity per IEC 61043:1994 and the ISO 9614-1:1993 field indicators.

A p-p probe holds two pressure microphones a fixed distance spacing (dr) apart. The mean of the two pressures is taken as the sound pressure at the probe reference point, while the pressure differential is used to derive the particle velocity component along the probe axis (IEC 61043:1994, definition 3.2):

p(t) = (p1(t) + p2(t)) / 2
u(t) = -(1 / (rho * dr)) * integral of (p2(t) - p1(t)) dt
I = < p(t) * u(t) > (time average)

For stationary signals the time-averaged intensity reduces to the imaginary part of the one-sided cross spectrum G12 of the two microphone pressures (the frequency-domain form of the same finite-difference estimator):

I(f) = -Im{G12(f)} / (2 * pi * f * rho * dr)

The finite-difference gradient underestimates the true plane-wave intensity by the factor sin(k*dr) / (k*dr) with k = 2*pi*f/c; IEC 61043:1994 clause 7.3 specifies the probe intensity response with exactly this argument (Ff = dr * f * 2 * pi / c) and Table 3 lists the resulting nominal response (e.g. -10,5 dB at 6,3 kHz for a 25 mm separation). Below f = 0,1 * c / dr (k*dr < 0,63) the bias stays under about 0,3 dB (factor >= 0,935).

Field indicators F2 (surface pressure-intensity), F3 (negative partial power) and F4 (field non-uniformity) follow ISO 9614-1:1993 Annex A (normative), equations (A.3)-(A.9). The dynamic capability index is Ld = delta_pI0 - K (ISO 9614-1 clause 3.12, equation (10)); the instrument is adequate for a measurement when Ld > F2 (criterion 1, Annex B equation (B.1)).

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dynamic_capability_index(
pressure_residual_intensity_index: float,
bias_error_factor: float = 10.0,
) -> float

Dynamic capability index Ld (ISO 9614-1:1993, clause 3.12).

Ld = delta_pI0 - K (equation (10)), where delta_pI0 is the instrument pressure-residual intensity index (clause 3.11, equation (9); determined per IEC 61043:1994, which requires the Table 2 minima per class) and K the bias error factor of Table 1: 10 dB for precision (grade 1) and engineering (grade 2) measurements, 7 dB for survey (grade 3). The measurement arrangement is adequate when Ld > F2 (criterion 1, Annex B equation (B.1)).

Parameters

NameDescription
pressure_residual_intensity_indexdelta_pI0 in decibels.
bias_error_factorK in decibels (default 10,0).

Returns: Ld in decibels.

field_indicators(
pressure_levels: list[float] | np.ndarray,
normal_intensity: list[float] | np.ndarray,
frequencies: list[float] | np.ndarray | None = None,
) -> FieldIndicators

ISO 9614-1:1993 Annex A field indicators F2, F3 and F4.

Given the sound pressure level Lpi (dB) and the signed normal sound intensity Ini (W/m^2) measured at each of the N discrete positions on the measurement surface:

  • F2 = Lp - L|In| (equation (A.3)), with the surface pressure level from equation (A.4) and the level of the mean magnitude of the normal intensity from equation (A.5);
  • F3 = Lp - LIn (equation (A.6)), with the algebraic surface intensity level from equation (A.7);
  • F4 = (1/|mean In|) * sqrt(sum((Ini - mean In)^2) / (N - 1)) (equations (A.8)-(A.9)).

The inputs are either 1D per-position arrays (one frequency band, scalar indicators) or 2D (positions, bands) arrays (the indicators are evaluated band by band and returned as per-band arrays; the plottable form). If the algebraic mean intensity of any band is not positive the test conditions do not satisfy ISO 9614-1 in that band (clause A.2.3) and a ValueError is raised.

Parameters

NameDescription
pressure_levelsLpi at each position, in decibels; 1D (positions,) or 2D (positions, bands).
normal_intensitySigned normal intensity Ini at each position, in W/m^2; same shape as pressure_levels.
frequenciesBand centre frequencies in Hz, one per column of the 2D input (optional for 1D input, where it is ignored beyond a length check).

Returns: FieldIndicators.

FieldIndicators(
f2: float | np.ndarray,
f3: float | np.ndarray,
f4: float | np.ndarray,
frequency: np.ndarray | None = None,
)

ISO 9614-1:1993 Annex A field indicators over a measurement surface.

f2 is the surface pressure-intensity indicator (equation (A.3)), f3 the negative partial power indicator (equation (A.6)) and f4 the field non-uniformity indicator (equation (A.8)). f3 - f2 > 0 reveals negative partial power flowing through parts of the surface. The instrument’s dynamic capability index must satisfy Ld > f2 (criterion 1, equation (B.1)); the number of positions N must satisfy N > C * f4**2 (criterion 2, equation (B.2)).

With per-position and per-band input (2D arrays passed to field_indicators) the three indicators are per-band arrays and frequency carries the band centres; with 1D per-position input they are scalars and frequency is None.

FieldIndicators.plot(
ax: Axes | None = None,
*,
dynamic_capability: float | np.ndarray | None = None,
language: str = 'en',
**kwargs: Any,
) -> Axes

Plot the per-band indicators F2/F3, the Ld line and F4.

Requires per-band data (call field_indicators with 2D (positions, bands) arrays and frequencies) and matplotlib (pip install phonometry[plot]); returns the Axes.

Parameters

NameDescription
axExisting axes, or None to create a figure.
dynamic_capabilityOptional instrument dynamic capability index Ld in dB (scalar or per band), drawn as the criterion-1 reference line (Ld > F2, equation (B.1)); see dynamic_capability_index.
languageLabel language, "en" (default) or "es".
kwargsForwarded to the F2 curve plot call.

Raises

ExceptionWhen
ValueErrorIf the result carries no per-band data.
IntensityResult(
frequency: np.ndarray | None,
intensity: np.ndarray | None,
intensity_level: np.ndarray | None,
pressure_level: np.ndarray | None,
pressure_intensity_index: np.ndarray | None,
direction: np.ndarray | None,
bias_correction: np.ndarray | None,
total_intensity: float,
total_intensity_level: float,
total_pressure_level: float,
total_pressure_intensity_index: float,
total_direction: int,
max_valid_frequency: float,
)

Result of a p-p sound intensity measurement.

Per-band arrays are None unless a band fraction was requested. intensity is signed (positive along the probe axis, from microphone 1 towards microphone 2); intensity_level is computed from the magnitude, 10*lg(|I|/1e-12) dB, with the sign reported separately in direction (+1/-1). pressure_intensity_index is Lp - LI (the single-position form of the ISO 9614-1:1993 F2 indicator, equation (A.3)). bias_correction is the multiplicative factor (k*dr)/sin(k*dr) compensating the finite-difference underestimation at each band centre (IEC 61043:1994, 7.3); it is NaN at and beyond the first null k*dr >= pi. max_valid_frequency is the usable-bandwidth bound 0,1*c/spacing (bias < ~0,3 dB).

IntensityResult.plot(
ax: Axes | None = None,
*,
language: str = 'en',
**kwargs: Any,
) -> Axes

Plot Lp vs LI per band with the pressure-intensity index.

Requires per-band data (call sound_intensity(..., fraction=...)) and matplotlib (pip install phonometry[plot]); returns the Axes.

sound_intensity(
p1: list[float] | np.ndarray,
p2: list[float] | np.ndarray,
fs: int,
spacing: float,
rho: float = 1.204,
c: float = 343.0,
fraction: int | None = None,
limits: list[float] | None = None,
bias_correct: bool = False,
) -> IntensityResult

Sound intensity from a two-microphone (p-p) probe (IEC 61043:1994).

The one-sided cross spectrum G12 of the two microphone pressures is estimated with Welch-averaged, Hann-windowed segments (scipy.signal.csd) and converted to the intensity spectral density along the probe axis (definition 3.2 of IEC 61043:1994 gives the underlying p-p formulation):

I(f) = -Im{G12(f)} / (2 * pi * f * rho * spacing)

Positive intensity flows from microphone 1 towards microphone 2. The mean-square pressure is taken from the mean signal (p1 + p2)/2 at the probe reference point. When fraction is given, both quantities are integrated into octave (1) or one-third octave (3) bands using the ANSI S1.11/IEC 61260-1 band edges of phonometry.nominal_frequencies; bands without any spectral bin are dropped. Broadband totals are always computed (over limits when provided, otherwise over all positive frequencies).

The pressure-intensity index Lp - LI is reported per band and broadband; in a free plane progressive wave it equals 10*lg(rho*c/400) = 0,14 dB (IEC 61043:1994 clause 5 note), while large values flag reactive or noisy fields (compare with the instrument dynamic capability, ISO 9614-1:1993 criterion 1).

Usable bandwidth: the finite-difference gradient biases the result by the factor sin(k*spacing)/(k*spacing) (IEC 61043:1994, 7.3); results are essentially unbiased (< ~0,3 dB) below max_valid_frequency = 0,1 * c / spacing, and bias_correction provides the per-band compensation factor.

Parameters

NameDescription
p1Pressure signal of microphone 1, in pascals (1D).
p2Pressure signal of microphone 2, in pascals (1D).
fsSample rate in Hz.
spacingMicrophone separation dr, in metres.
rhoAir density, in kg/m^3. Default 1,204 (20 degC).
cSpeed of sound, in m/s. Default 343,0.
fractionNone (broadband only), 1 (octave bands) or 3 (one-third octave bands).
limits[f_min, f_max] band limits in Hz (default [12, 20000], as in phonometry.nominal_frequencies).
bias_correctIf True, apply the per-bin finite-difference correction (k*spacing)/sin(k*spacing) (IEC 61043:1994, 7.3) to the intensity spectral density before summing the band and broadband totals, so the totals no longer under-read as the frequency approaches max_valid_frequency. The reciprocal diverges as k*spacing -> pi (the first spatial-aliasing null at c/(2*spacing), inside the default band range for close spacings), so it is applied only over the probe’s usable range (up to k*spacing = pi/2) and held constant beyond, keeping the totals bounded instead of letting a few near-null bins dominate them. Default False keeps the exact legacy totals; the per-band bias_correction factor (same clamped definition) is reported either way.

Returns: IntensityResult.

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