Field Insulation Measurement (ISO 16283)

Standards: ISO 16283 ISO 717 ISO 12999Key references: Hopkins 2007 Vigran 2008

This guide continues from the Room Acoustics guide: the same impulse response, measured either side of a partition, yields its sound insulation. This page covers the engineering-grade measurement of ISO 16283 in the finished building: the airborne level differences $D$ , $D_{n T}$ and $R^{'}$ , the impact levels $L_{n T}^{'}$ and $L_{n}^{'}$ , the field test report, and the ISO 12999-1 uncertainty that qualifies every field value. Three close relatives have guides of their own: the reference-curve engine behind every single number in Insulation Ratings (ISO 717), the building envelope in Façade Sound Insulation, and the quick octave-band route in Sound Insulation Survey Method (ISO 10052). The laboratory characterisation of an element lives in Laboratory Insulation Measurement and the prediction of in-situ performance in Predicting Sound Insulation (EN 12354).

How do I compute DnT and R’ from a field measurement in Python?

Energy-average the source- and receiving-room levels per one-third-octave band across the microphone positions of one loudspeaker position, correct the receiving room for background noise, and pass them, with the receiving-room reverberation time, to building.airborne_insulation(l1, l2, t2, area=S, volume=V). The result carries the raw level difference d, the standardized dnt and, when area and volume are given, the apparent r_prime. If a single loudspeaker was moved between positions, repeat that for each position and combine the results with Formula (6), not the levels — see Taking the measurement. Impact measurements go through building.impact_insulation(li, t2, volume=V), and either spectrum is rated with building.weighted_rating / weighted_impact_rating.

Field airborne insulation (ISO 16283-1)

To rate a wall or floor, measure the energy-average level in the source room ( $L_{1}$ ) and the receiving room ( $L_{2}$ ) per one-third-octave band and form the level difference $D = L_{1} - L_{2}$ . Two normalisations make it comparable between rooms. The standardized level difference references the receiving-room reverberation time $T$ to $T_{0} = 0.5$ s (so with $T = 0.5$ s, $D_{n T} = D$ exactly), and the apparent sound reduction index normalises by the partition area $S$ and the Sabine absorption area $A$ :

D_{n T} = D + 10 lo g_{10} \frac{T}{T _{0}}, R^{'} = D + 10 lo g_{10} \frac{S}{A}, A = \frac{0.16 V}{T} .

Positions are energy-averaged with $L = 10 lo g_{10} (\frac{1}{n} \sum_{i} 1 0^{L_{i} /10})$ .

Field airborne insulation setup: a loudspeaker in the source room, microphones energy-averaged in source and receiving rooms across the common partition

The prime on $R^{'}$ is a convention, not decoration: primed quantities ( $R^{'}$ , $L_{n}^{'}$ , $L_{n T}^{'}$ ) are measured in the building and include every flanking path, while the unprimed $R$ and $L_{n}$ are laboratory properties of the element alone, measured with flanking suppressed. The full lab-to-field map lives in Laboratory Insulation Measurement; the prediction that bridges the two is EN 12354.

One measurement yields all three quantities, so which one goes on the report is a regulatory question, not a measurement one. $D_{n T}$ describes the room pair as the occupants experience it, and that is what most national codes for dwellings state their requirements in. $R^{'}$ describes the partition, normalised by its area, and is what a comparison against a laboratory $R_{w}$ or an EN 12354 prediction needs. Measure once, then report the quantity the requirement is written in and say which it is: an $R_{A}^{'}$ cannot be checked against a $D_{n T, A}$ limit without converting through the room’s $T$ and the partition area first — see Spanish Building Code (CTE DB-HR), which states its between-rooms requirement in $D_{n T, A}$ and its partition-wall requirement in $R_{A}$ .

import numpy as np
from phonometry import building

# Energy-average several microphone positions in one room (dB)
print(round(float(building.energy_average_level([60.0, 66.0])), 1))   # 64.0

# Field insulation per band; area S and volume V add R'
l1 = np.full(16, 80.0)                                # source-room levels
l2 = np.full(16, 40.0)                                # receiving-room levels
t2 = np.full(16, 0.5)                                 # receiving-room T (s)
ins = building.airborne_insulation(l1, l2, t2, area=10.0, volume=50.0)
print(round(float(ins.dnt[0]), 1))                   # 40.0  (= D since T = T0)
print(round(float(ins.r_prime[0]), 1))               # 38.0

# The single number comes from the ISO 717-1 engine of the ratings guide
print(building.weighted_rating(ins.dnt).rating)      # 40  DnT,w
print(building.weighted_rating(ins.r_prime).rating)  # 38  R'w

Compute l1, l2 and t2 on the same 16 one-third-octave bands from 100 Hz to 3150 Hz (obtain t2 from room_parameters(ir, fs, limits=(100, 3150), fraction=3).t30, for example) and pass them to airborne_insulation. Feed that function’s dnt (or r_prime) spectrum to weighted_rating, so every band aligns index-by-index with the ISO 717-1 reference curve.

The scale is worth carrying: for a separating wall or floor between dwellings, national requirements typically sit around $D_{n T, w} = 50$ dB and rarely below 45 dB, so the 40 dB of this deliberately flat example would fail every one of them. Higher is better for an airborne quantity, and 5 dB is roughly the step between a construction that works and one that generates complaints.

`airborne_insulation()` parameters

Parameter	Type	Units	Range / default	Notes
`l1`	1D or 2D array	dB	one/band, or `(positions, bands)`	Source-room levels (2D is energy-averaged)
`l2`	1D or 2D array	dB	same band count	Receiving-room levels
`t2`	1D array	s	> 0, one per band	Receiving-room reverberation time
`area`	float, optional	m²	> 0, with `volume`	Partition area $S$ (enables $R^{'}$ )
`volume`	float, optional	m³	> 0, with `area`	Receiving-room volume $V$
`t0`	float	s	default `0.5`	Reference reverberation time $T_{0}$

airborne_insulation() returns an AirborneInsulationResult (d, dnt, r_prime or None). The reference-curve engine that turns any of those spectra into $R_{w}$ , $R_{w}^{'}$ or $D_{n T, w}$ , its spectrum adaptation terms and its enlarged-range variants are in Insulation Ratings (ISO 717).

Taking the measurement (ISO 16283-1 Clauses 7 and 9)

The functions consume band levels; the standard says where those levels come from, and getting that wrong changes the answer more than any of the arithmetic above.

The source (Clause 7.1, 7.2). Sound is generated with loudspeakers operated simultaneously in at least two positions, or with a single loudspeaker moved to at least two positions. Multiple loudspeakers must be of the same type, driven at the same level by similar but uncorrelated signals, and each must meet the Annex A directivity requirement. The signal is steady with a continuous spectrum, and the energy-average source-room level must not change by more than 8 dB between adjacent one-third-octave bands, at least above 100 Hz — shape the spectrum (a graphic equaliser is usually needed) or fall back to serial band-limited measurements. Loudspeakers stand at least 0.5 m from any boundary, preferably at least 1.0 m from the separating partition, measured to the centre of the nearest speaker unit; different positions must not lie in planes parallel to a boundary less than 0.7 m apart, must be at least 0.7 m apart, and at least two of them at least 1.4 m apart. When the floor is the test element and the loudspeaker is in the upper room, its base sits at least 1.0 m above the floor.

The microphones (Clause 7.3). A minimum of five positions per room — and, with a single loudspeaker moved between positions, five per room per loudspeaker position. No two positions may lie in the same plane relative to the room boundaries, and the set must not form a regular grid.

Correcting for background noise (Clause 9.2)

Measure the receiving room again with the source off, at the same positions and with the same averaging, and compare band by band with the combined signal-plus-background level $L_{s b}$ :

margin $\geq 10$ dB: use $L_{s b}$ unchanged;
$6 < margin < 10$ dB: subtract the background in energy, $L = 10 lo g_{10} (1 0^{L_{s b} /10} - 1 0^{L_{b} /10})$ (Formula 14), with both levels first reduced to one decimal place;
margin $\leq 6$ dB: apply the fixed 1.3 dB correction, and flag the band in the report as being at the limit of measurement.

import numpy as np

l2_sb = np.array([44.0, 41.0, 39.5, 38.0])   # receiving room, source on
l2_bg = np.array([30.0, 33.0, 31.0, 34.0])   # receiving room, source off
margin = l2_sb - l2_bg                       # 14.0  8.0  8.5  4.0 dB

formula_14 = 10 * np.log10(10 ** (l2_sb / 10) - 10 ** (l2_bg / 10))
l2_corr = np.where(margin >= 10.0, l2_sb,
                   np.where(margin > 6.0, formula_14, l2_sb - 1.3))
print(np.round(l2_corr, 2))     # [44.   40.25 38.84 36.7 ]  <- last band flagged

building.background_correction exists, but it implements the ISO 10140-4 laboratory rule used on Laboratory Insulation Measurement, whose upper threshold is 15 dB rather than 10 dB. Applied to field data it subtracts energy in the 10-15 dB margin band where ISO 16283-1 asks for nothing — up to 0.458 dB at a 10 dB margin — and since it acts on the receiving room that lands as over-reported insulation, band for band, in $D$ . Use the three-regime expression above for field levels.

Averaging over loudspeaker positions (Formula 6)

With multiple loudspeakers operating simultaneously (Clause 7.3.3) there is one measurement: energy-average the positions in each room, correct for background noise, and form $D_{n T}$ or $R^{'}$ once. With a single loudspeaker moved between positions (Clause 7.3.4) the standard does not average the levels across loudspeaker positions. It forms the result for each position and averages the results as transmission factors,

D_{n T} = - 10 lo g_{10} [\frac{1}{m} j = 1 \sum m 1 0^{- D_{n T, j} /10}],

which weights the worst position most. The two routes are not the same number:

import numpy as np
# `building` is the import of the airborne-insulation block above.

t2 = np.full(16, 0.5)
l1a, l2a = np.full(16, 80.0), np.full(16, 40.0)   # loudspeaker position 1
l1b, l2b = np.full(16, 83.0), np.full(16, 37.0)   # loudspeaker position 2

# Clause 7.3.4: one result per loudspeaker position, combined by Formula (6).
a = building.airborne_insulation(l1a, l2a, t2, area=10.0, volume=50.0)
b = building.airborne_insulation(l1b, l2b, t2, area=10.0, volume=50.0)
dnt = -10 * np.log10(np.mean(10.0 ** (-np.vstack([a.dnt, b.dnt]) / 10.0), axis=0))
print(round(float(dnt[0]), 1), building.weighted_rating(dnt).rating)        # 42.0 42

# Averaging the levels first instead: a different, more flattering number.
l1m = building.energy_average_level(np.vstack([l1a, l1b]), axis=0)
l2m = building.energy_average_level(np.vstack([l2a, l2b]), axis=0)
naive = building.airborne_insulation(l1m, l2m, t2, area=10.0, volume=50.0)
print(round(float(naive.dnt[0]), 1), building.weighted_rating(naive.dnt).rating)  # 43.0 43

Small rooms: the low-frequency procedure (Clause 8)

This one is easy to miss and it is mandatory. When the source and/or receiving room has a volume smaller than 25 m³ — calculated to the nearest cubic metre, so a 25.4 m³ bedroom does not trigger it and a 24.6 m³ one does — the 50 Hz, 63 Hz and 80 Hz one-third-octave bands must additionally be measured in the corners of that room (Clause 6 and Clause 8.1). Most European bedrooms and every bathroom fall under the threshold, so this is the normal case in dwelling work, not an edge case. It is in addition to the default procedure, not instead of it, and the same 25 m³ rule governs the reverberation time.

The reason is stated in the standard’s own NOTE 1: at those frequencies a small room’s field is modal, the spatial variation is large, and the central-zone average is neither repeatable nor representative of what an occupant hears. A modal pressure maximum always sits in a corner, so corner measurements bound the field from above.

How a corner measurement is taken (Clauses 8.3 and 8.4). A fixed microphone, 0.3 m to 0.4 m from each of the three boundaries forming the corner (the three distances need not be equal), at least 1.0 m from any loudspeaker — which in practice rules out the corner the loudspeaker occupies. Measure at least four corners, two at floor level and two at ceiling level, adjacent to the partition or not; each corner must be formed by three mutually perpendicular surfaces of at least 0.5 m², with no furniture within 0.5 m. Where that is impossible, corners with pair angles between 45° and 135°, or with an object such as a cupboard forming one surface, are admitted. Average at least 15 s per position. With a single loudspeaker moved between positions, take the four corners again for each position.

How the corners enter the result (Clause 8.5). For each of the three bands independently, take the highest of the measured corners — which may be a different corner in each band — as $L_{Corner}$ ; with several loudspeaker positions, energy-average those per-position maxima (Formula (12)). Then combine with the default-procedure average $L$ in a 1:2 weighting (Formula (13)):

L_{L F} = 10 lo g_{10} [\frac{1 0 ^{0.1 L_{Corner}} + 2 \cdot 1 0 ^{0.1 L}}{3}] .

$L_{L F}$ replaces $L$ in those three bands, and $D_{n T}$ or $R^{'}$ is then formed exactly as before. Because $L_{Corner}$ can exceed $L$ by several decibels, the procedure raises the source-room level and the receiving-room level alike — the effect on the level difference is whatever the two rooms do not have in common, which is precisely the information the default procedure throws away. Clause 9.1 adds the consequence for background noise: a background measurement is required in each corner used, because each band may have come from a different corner and so may need its own correction.

# `np` and `building` are the imports of the blocks above.

# 50, 63, 80 Hz. Four corners measured in a 22 m3 receiving room, one
# loudspeaker position; the default central-zone average alongside.
corners = np.array([                      # rows: corners, columns: the 3 bands
    [52.1, 55.4, 49.8],
    [54.6, 53.0, 51.2],
    [51.0, 56.9, 50.4],
    [53.3, 54.1, 52.7],
])
l_default = np.array([49.5, 51.2, 48.6])

l_corner = corners.max(axis=0)            # Clause 8.5: the loudest corner, per band
print(l_corner)                           # [54.6 56.9 52.7]  (three different corners)

l_lf = 10 * np.log10((10 ** (0.1 * l_corner) + 2 * 10 ** (0.1 * l_default)) / 3)
print(np.round(l_lf, 1))                  # [51.9 54.  50.4]
print(np.round(l_lf - l_default, 1))      # [2.4 2.8 1.8]  dB above the default

Field impact insulation (ISO 16283-2)

Footstep noise is rated the other way round. Instead of how much a floor blocks, impact insulation measures how much a standardized tapping machine on the floor above puts into the room below, so a higher number is worse. The energy-average impact sound pressure level $L_{i}$ in the receiving room is normalised like the airborne case, but with a sign flip on the reverberation term:

L_{n T}^{'} = L_{i} - 10 lo g_{10} \frac{T}{T _{0}}, L_{n}^{'} = L_{i} + 10 lo g_{10} \frac{A}{A _{0}}, A_{0} = 10 m^{2}, A = \frac{0.16 V}{T} .

The standardized impact level $L_{n T}^{'}$ ( $T_{0} = 0.5$ s for dwellings) needs only the receiving-room $T$ , so with $T = 0.5$ s it equals $L_{i}$ ; the normalized level $L_{n}^{'}$ (referenced to a 10 m² absorption area) also needs the receiving-room volume. Note the minus sign: more reverberation lowers $L_{n T}^{'}$ , opposite to the airborne $D_{n T}$ .

The tapping machine is not the only source ISO 16283-2 specifies. Its hammers deliver a hard, quasi-stationary excitation whose energy sits above 100 Hz, which says almost nothing about the slow low-frequency thumps occupants actually complain about — a child jumping, an adult walking barefoot. For those, the same standard specifies a rubber ball (Annex A), rated through a different engine entirely: a Fast-weighted maximum level and the A-weighted sum of ISO 717-2 Annex D, not a shifted reference curve. It has its own guide, Heavy and Soft Impact Sources.

Field impact insulation setup: a standardized tapping machine on the floor of the source room above, microphones energy-averaged in the receiving room below, and the receiving-room reverberation time

import numpy as np
from phonometry import building

# 16 one-third-octave impact levels Li (100 Hz - 3150 Hz), dB, from the
# ISO 717-2 Annex C worked example, and the receiving-room T per band.
li = np.array([62.1, 63.2, 63.5, 66.2, 68.5, 70.0, 71.7, 73.1,
               73.8, 73.5, 73.8, 73.3, 73.1, 73.0, 72.4, 71.2])
t2 = np.full(16, 0.5)

imp = building.impact_insulation(li, t2, volume=50.0)
print(round(float(imp.l_n_t[0]), 1))          # 62.1  (= Li since T = T0)
print(round(float(imp.l_n[0]), 1))            # 64.1  normalized to A0 = 10 m^2

# Weighted impact rating + spectrum adaptation term CI (ISO 717-2)
res_imp = building.weighted_impact_rating(imp.l_n_t)
print(res_imp.rating, res_imp.ci, res_imp.unfavourable_sum)   # 79 -11 28.0  ->  L'nT,w(CI)=79(-11)

# Octave-band data carry the extra -5 dB reduction (Clause 4.3.2)
octave = np.array([65.3, 64.5, 58.0, 55.8, 43.0])
print(building.weighted_impact_rating(octave).rating)  # 54

Feed impact_insulation’s l_n_t (or l_n) straight into weighted_impact_rating; the rating and $C_{I}$ reproduce the ISO 717-2 Annex C values (thirds $L_{n T, w}^{'} = 79$ , $C_{I} = - 11$ ; octave 54, $C_{I} = 0$ ).

The sign of the scale reverses here: lower is better for an impact quantity. National limits for dwellings sit in the 50 to 60 dB range, so $L_{n T, w}^{'} = 79$ dB is a bare structural floor with no covering and no floating layer, failing by roughly 20 dB — the Annex C example is a worst case, not a typical one. What it takes to close a gap of that size is a floating floor on a resilient layer or a decoupled ceiling, not a carpet; see Predicting Sound Insulation (EN 12354) and Predicting resilient-layer performance.

`impact_insulation()` parameters

Parameter	Type	Units	Range / default	Notes
`li`	1D or 2D array	dB	one/band, or `(positions, bands)`	Energy-average impact SPL (2D is averaged over positions)
`t2`	1D array	s	> 0, one per band	Receiving-room reverberation time
`volume`	float, optional	m³	> 0	Receiving-room $V$ (enables $L_{n}^{'}$ )
`t0`	float	s	default `0.5`	Reference reverberation time $T_{0}$

impact_insulation() returns an ImpactInsulationResult (l_n_t, l_n or None); the ISO 717-2 side of the chain is in Insulation Ratings (ISO 717).

ISO 16283 field test report (`.report()`)

The per-band field results write the test report of ISO 16283-1:2014 / ISO 16283-2:2020 Clause 14 directly, laid out like the recommended results forms (Annex B / Annex C) and the accredited field reports built on them. AirborneInsulationResult.report() renders the standardized level difference $D_{n T}$ fiche (Figure B.1) or, with quantity="r_prime", the apparent sound reduction index $R^{'}$ fiche (Figure B.2); ImpactInsulationResult.report() renders the standardized $L_{n T}^{'}$ fiche (Figure C.1) or, with quantity="l_n", the normalized $L_{n}^{'}$ fiche (Figure C.2). Each fiche names the field standard in its basis line, evaluates the ISO 717-1 / ISO 717-2 single-number rating over the 16 core one-third-octave bands (100–3150 Hz), states the quantity to one decimal place both in tabular form and as a curve against the shifted reference curve (Clause 12), boxes the field rating (DnT,w (C; Ctr), R'w (C; Ctr), L'nT,w (CI) or L'n,w (CI)) and prints the mandatory statement that the evaluation is based on field measurement results obtained by an engineering method.

verbose=True swaps the two-column table for the per-band measurement chain (the energy-average $L_{1}$ and $L_{2}$ , or $L_{i}$ , and the reverberation time $T$ beside the reported quantity), the content accredited field reports annex; it needs a result built by airborne_insulation() / impact_insulation(), which retain those inputs on the result (l1, l2/li, t2, t0). Metadata, the requirement verdict (airborne passes at or above it, impact at or below it), language="es" and the phonometry[report] extra behave exactly as in the ISO 717 fiche above.

import numpy as np
from phonometry import building, ReportMetadata

# Field airborne: source/receiving levels and T per one-third-octave band
l1 = np.array([92.3, 93.1, 94.0, 94.4, 94.8, 95.0, 95.2, 95.4,
               95.3, 95.1, 94.8, 94.4, 93.9, 93.3, 92.5, 91.6])
l2 = l1 - np.array([38.2, 40.1, 42.6, 45.2, 47.8, 50.1, 52.3, 54.0,
                    55.6, 57.1, 58.2, 59.0, 59.6, 60.1, 60.3, 59.8])
t2 = np.array([0.62, 0.58, 0.55, 0.53, 0.52, 0.50, 0.49, 0.48,
               0.47, 0.46, 0.45, 0.45, 0.44, 0.43, 0.43, 0.42])
field = building.airborne_insulation(l1, l2, t2, area=12.5, volume=30.4)
field.plot()   # per-band DnT (and R') of the measured chain (needs matplotlib)
metadata = ReportMetadata(
    specimen="Separating wall, 240 mm brick with independent lining",
    client="Example client",
    area=12.5, source_volume=32.1, receiving_volume=30.4,
    test_room="Dwelling A living room to dwelling B living room",
    test_date="2026-07-20",
    laboratory="Phonometry Reference Laboratory",
    report_id="PHN-2026-0143",
    requirement=50.0,               # DnT,w >= 50 dB -> PASS/FAIL row
)
field.report("DnTw_field.pdf", metadata=metadata)      # DnT,w (C; Ctr)
field.report("Rpw_field.pdf", quantity="r_prime",
             metadata=metadata)                        # R'w (C; Ctr)
field.report("DnTw_chain.pdf", metadata=metadata,
             verbose=True)                             # f | L1 | L2 | T | DnT

# Field impact: tapping-machine levels in the receiving room
li = np.array([58.0, 60.5, 62.0, 63.5, 65.0, 66.0, 66.5, 66.0,
               65.5, 65.0, 64.0, 62.0, 59.0, 56.0, 53.0, 50.0])
imp = building.impact_insulation(li, t2, volume=30.4)
imp.report("LnTw_field.pdf",
           metadata=ReportMetadata(requirement=58.0))  # L'nT,w (CI)

Field airborne measurement chain: the raw level difference D and the standardized DnT across the sixteen one-third-octave bands, with the reverberation correction shaded between them and the resulting DnT,w and R'w ratings annotated

The receiving-room reverberation time turns the raw level difference $D$ into the standardized $D_{n T}$ band by band; with $T$ above $T_{0} = 0.5$ s across the range, the correction lifts the curve slightly. The rating box carries both single numbers of this measurement, $D_{n T, w}$ and $R_{w}^{'}$ .

Show the code for this figure

import matplotlib.pyplot as plt
import numpy as np
from phonometry import building

# Field airborne: source/receiving levels and T per one-third-octave band
l1 = np.array([92.3, 93.1, 94.0, 94.4, 94.8, 95.0, 95.2, 95.4,
               95.3, 95.1, 94.8, 94.4, 93.9, 93.3, 92.5, 91.6])
l2 = l1 - np.array([38.2, 40.1, 42.6, 45.2, 47.8, 50.1, 52.3, 54.0,
                    55.6, 57.1, 58.2, 59.0, 59.6, 60.1, 60.3, 59.8])
t2 = np.array([0.62, 0.58, 0.55, 0.53, 0.52, 0.50, 0.49, 0.48,
               0.47, 0.46, 0.45, 0.45, 0.44, 0.43, 0.43, 0.42])
field = building.airborne_insulation(l1, l2, t2, area=12.5, volume=30.4)

# One line — the per-band DnT (and R') of the measured chain:
field.plot()
plt.show()

# By hand, from the result's fields:
bands = [100, 125, 160, 200, 250, 315, 400, 500,
         630, 800, 1000, 1250, 1600, 2000, 2500, 3150]
x = np.arange(len(bands))
w = building.weighted_rating(field.dnt)
fig, ax = plt.subplots()
ax.fill_between(x, field.d, field.dnt, alpha=0.2, label="10 log10(T/T0)")
ax.plot(x, field.d, "--o", label="D (level difference)")
ax.plot(x, field.dnt, "-s", label="DnT (standardized)")
ax.set_xticks(x, [str(b) for b in bands], rotation=45)
ax.set(xlabel="Frequency [Hz]", ylabel="Level difference [dB]",
       title=f"DnT,w = {w.rating} dB  (C={w.c:+d}; Ctr={w.ctr:+d})")
ax.legend()
plt.show()

Both example fiches are regenerated with make reports and kept rendered in the repository; click either preview to open the PDF.

Field airborne ISO 16283-1 example report (PDF) — Field airborne fiche (AirborneInsulationResult.report), DnT,w (C; Ctr).

Field impact ISO 16283-2 example report (PDF) — Field impact fiche (ImpactInsulationResult.report), L'nT,w (CI).

Measurement uncertainty (ISO 12999-1)

A rating without an uncertainty is only half a result. ISO 12999-1 does not re-measure anything; it tabulates the standard uncertainty $u$ of every sound-insulation quantity, derived from inter-laboratory tests, and prescribes how to expand and combine it. Which standard deviation is $u$ depends on the measurement situation (Clause 5.2):

Situation	Meaning	Standard uncertainty $u$
A	laboratory characterisation (ISO 10140)	reproducibility $σ_{R}$
B	same location, different teams	in-situ $σ_{s i t u}$
C	same location, same operator repeated	repeatability $σ_{r}$

The expanded uncertainty is $U = k u$ (Formula 2) with the coverage factor $k$ of Table 8. A two-sided interval $Y = y \pm U$ (Formula 3, $k = 1.96$ at 95 %) reports a value; the one-sided factor ( $k = 1.65$ at 95 %) declares conformity with a requirement (Formulae 4/5).

ISO 12999-1 uncertainty flow: standard uncertainty from the tables, reduced by repeated measurements and combined in quadrature, then expanded by the Table 8 coverage factor into a two-sided report or a one-sided conformity decision

from phonometry import building

# Situation B (same building, different teams) -> the in-situ standard deviation.
print(building.single_number_uncertainty("r_w", "B"))       # 0.9  dB  (Table 3)
u = building.band_uncertainty("airborne", "B")              # per-band u (Table 2)
# Look the band up; never index by position. The impact table has no 500 Hz
# band at all, so [10] would silently be 630 Hz there.
i = list(u.frequencies).index(500.0)
print(len(u.frequencies), u.uncertainties[i])      # 21 1.1  (the 500 Hz band)
u.plot()   # the per-band u(f) spectrum of Table 2 (needs matplotlib)

# Report R'w = 52 dB with a two-sided 95 % interval (k = 1.96, Table 8):
uv = building.uncertain_value(52.0, "rprime_w", "B")        # aliases resolve to r_w
print(uv.coverage_factor, round(uv.expanded_uncertainty, 1))    # 1.96 1.8
print(round(uv.lower, 1), round(uv.upper, 1))      # 50.2 53.8  ->  52 ± 1.8 dB

# Declaring conformity uses the ONE-sided factor (k = 1.65): does R'w provably
# clear a 50 dB requirement?
uc = building.uncertain_value(52.0, "rprime_w", "B", one_sided=True)
print(round(uc.expanded_uncertainty, 2))                # 1.48  = 1.65 x 0.9
print(round(52.0 - uc.expanded_uncertainty, 2))         # 50.52 = the lower bound
print(building.satisfies_lower_requirement(52.0, uc.expanded_uncertainty, 50.0))   # True

That is the whole content of satisfies_lower_requirement: the measured 52.0 minus the one-sided expanded uncertainty 1.48 is 50.52, which still clears 50.0, so conformity can be declared rather than merely observed. The choice of factor is the point. Reporting a value is a two-sided statement — the true value lies somewhere in an interval — and takes k = 1.96. Declaring conformity is a one-sided statement: only the lower end matters, because nothing is at stake if the wall is better than claimed, so k = 1.65 gives the same 95 % confidence on the side that counts. Using the two-sided factor here would demand 1.76 dB of margin instead of 1.48 dB and would fail results that genuinely comply.

Impact quantities offer situations B/C only (Table 4, no 500 Hz band in the 2020 edition), and $Δ L$ only situation A. Descriptors are case-insensitive with aliases (rprime_w/dnt_w→r_w, lprime_n_w→ln_w); combine independent components in quadrature with combine_uncertainties, and reduce by $m$ independent measurements with reduce_by_independent_measurements ( $u / m$ ).

The same rating, reported three ways. Which interval applies is not a property of the measurement but of the question: situation A is what a laboratory quotes for a specimen, B what two teams measuring the same installed partition should agree within, C what one team repeating itself should. B is the widest of the three that a field report can honestly claim, and it is the one that decides whether a result clears a requirement.

Show the code for this figure

import matplotlib.pyplot as plt
from phonometry import building

# The same R'w = 52 dB reported in each situation with its two-sided 95 % U.
situations = ["A", "B", "C"]
vals = [building.uncertain_value(52.0, "r_w", s) for s in situations]

fig, ax = plt.subplots(figsize=(7, 4))
ax.errorbar(situations, [v.value for v in vals],
            yerr=[v.expanded_uncertainty for v in vals],
            fmt="o", capsize=8, color="tab:blue")
for s, v in zip(situations, vals):
    ax.annotate(f"±{v.expanded_uncertainty:.1f}", (s, v.upper),
                textcoords="offset points", xytext=(8, 4))
ax.set_ylabel("R'w [dB]"); ax.set_xlabel("Measurement situation")
ax.set_title("R'w = 52 dB with 95 % expanded uncertainty (ISO 12999-1)")
fig.tight_layout()
plt.show()

`band_uncertainty()` / `single_number_uncertainty()` / `uncertain_value()` parameters

Parameter	Type	Units	Range / default	Notes
`measurand`	str	—	`'airborne'` / `'impact'` / `'impact_reduction'`	Selects Table 2 / 4 / 6
`quantity`	str	—	`'r_w'`, `'ln_w'`, `'delta_lw'` (+ aliases, `+c`/`+ctr` variants)	Single-number descriptor
`situation`	str	—	`'A'` / `'B'` / `'C'`	Measurement situation (Clause 5.2)
`value`	float	dB	—	Best estimate $y$ to attach $U$ to
`coverage`	float	—	default `0.95`	Confidence level (Table 8)
`one_sided`	bool	—	default `False`	One-sided factor for conformity checks
`upper_limit`	bool	—	default `False`	Select the $σ_{R 95}$ upper limit (airborne, situation A)

band_uncertainty() returns a BandUncertainty (frequencies, uncertainties, .to_arrays()); single_number_uncertainty() a float; uncertain_value() an UncertainValue (value, standard_uncertainty, coverage_factor, expanded_uncertainty, .lower, .upper). The read-only COVERAGE_FACTORS mapping exposes Table 8 keyed by (confidence, one_sided).

Beyond the two-room measurement

Three neighbouring measurements have guides of their own, and a fourth sits alongside them. The building envelope, measured against the level 2 m in front of it and predicted from its elements, is Façade Sound Insulation. When a full engineering measurement is more than the question deserves, the octave-band control method is Sound Insulation Survey Method (ISO 10052). Every single number quoted above comes from the reference curves of Insulation Ratings (ISO 717). And the sound-intensity route to the same quantities, which reads the transmitted power off the radiating face instead of the receiving-room level, is Sound Insulation by Intensity (ISO 15186).

What this guide covers

Covered
ISO 16283-1:2014 (airborne field insulation: the level difference, standardized $D_{n T}$ and apparent $R^{'}$ of Clause 3.12-3.15 and the Clause 7.8 position averaging) and ISO 16283-2:2020 (impact field insulation, the same normalisations with the sign flip) through building.energy_average_level, building.airborne_insulation and building.impact_insulation, each writing the Clause 14 test report with .report(); and ISO 12999-1:2020’s tabulated standard uncertainties (the Clause 5.2 measurement situations A/B/C and the Table 8 coverage factors, one- and two-sided) via building.band_uncertainty, building.single_number_uncertainty and building.uncertain_value. The single-number ratings quoted here reuse the verified ISO 717-1/ISO 717-2 engines.
Not covered
Every field function here takes levels that the caller has already corrected for background noise (Clause 9.2 of ISO 16283-1). The measurement of the background level — source off, same positions, same averaging — is the operator’s job, and nothing here verifies that the 6 dB floor was met; the correction itself is three lines of NumPy, written out under Correcting for background noise above. (building.background_correction is the ISO 10140-4 laboratory variant and does not match the field thresholds.) ISO 16283-1/-2’s own position and procedure requirements — the counts, distances and averaging of Taking the measurement and the corner measurements of Small rooms — are documented here and checked nowhere: energy-averaging happens once positions are supplied, but nothing verifies how many were taken, where, or that the 25 m³ trigger was even tested for. The Formula (12) and (13) combination of the low-frequency procedure is the two lines of NumPy printed above, not a library function. The other members of the family are covered by their own guides: the façade part ISO 16283-3 (Façade Sound Insulation), the survey method ISO 10052 (Sound Insulation Survey Method), the rating engines ISO 717-1/-2 (Insulation Ratings) and the sound-intensity route ISO 15186-1/-2 (Sound Insulation by Intensity).

Quick answers

What does DnT,w mean?

$D_{n T, w}$ is the weighted standardized level difference. Per one-third-octave band, $D_{n T} = D + 10 lo g_{10} (T / T_{0})$ references the receiving-room reverberation time $T$ to $T_{0} = 0.5$ s, with $D = L_{1} - L_{2}$ the source-to-receiving level difference (ISO 16283-1). The ISO 717-1 reference-curve method then collapses the 16 bands from 100 Hz to 3150 Hz into the single number read at 500 Hz.

What is the difference between R and R’ in sound insulation?

The prime marks where the measurement was made: primed quantities ( $R^{'}$ , $L_{n}^{'}$ , $L_{n T}^{'}$ ) are measured in the building and include every flanking path, while the unprimed $R$ and $L_{n}$ are laboratory properties of the element alone, measured with flanking suppressed. In the field (ISO 16283-1), $R^{'} = D + 10 lo g_{10} (S / A)$ with partition area $S$ and Sabine absorption area $A = 0.16 V / T$ .

References

Hopkins, C. (2007). Sound insulation. Butterworth-Heinemann. https://doi.org/10.4324/9780080550473The comprehensive treatment of airborne and impact sound insulation: the measurement chains, the statistics of rooms behind the field quantities and the interpretation of the single-number ratings. ISBN 978-0-7506-6526-1.
International Organization for Standardization. (2014). Acoustics — Field measurement of sound insulation in buildings and of building elements — Part 1: Airborne sound insulation (ISO 16283-1:2014). The field airborne method this page implements: the level differences and normalisations.
International Organization for Standardization. (2020). Acoustics — Determination and application of measurement uncertainties in building acoustics — Part 1: Sound insulation (ISO 12999-1:2020). The standard uncertainties per measurement situation (Clause 5.2) and the Table 8 coverage factors; its precision framework builds on ISO 5725 (context, not implemented directly).
International Organization for Standardization. (2020). Acoustics — Field measurement of sound insulation in buildings and of building elements — Part 2: Impact sound insulation (ISO 16283-2:2020). The field impact method: the standardized and normalized impact levels, the Clause 14 test report and its Annex C results forms. The 2015 first edition is identical for the normalisations used here.
International Organization for Standardization. (2020). Acoustics — Rating of sound insulation in buildings and of building elements — Part 1: Airborne sound insulation (ISO 717-1:2020). The reference-curve rating and the spectrum adaptation terms C and Ctr interpreted above; also the single-number engine for the façade quantity (Annex F).
International Organization for Standardization. (2020). Acoustics — Rating of sound insulation in buildings and of building elements — Part 2: Impact sound insulation (ISO 717-2:2020). The impact reference-curve rating and the spectrum adaptation term CI, with the enlarged-range CI,50-2500 term.
Vigran, T. E. (2008). Building acoustics. CRC Press. https://doi.org/10.1201/9781482266016A compact textbook companion for the sound-transmission physics behind these measurements. ISBN 978-0-415-42853-8.

Created and maintained by José Manuel Requena Plens ORCID All projects