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test report on noise barriers
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Technical ReportReport Number C/08/5L/20588/R01
Date 22 December 2008
Project The Laboratory Determination of Random Incidence Sound Absorption Coefficient of a Barrier
Prepared for
Tilon Composites LtdUnit 23 Rassau Industrial EstateEbbw ValeBlaenauGwentNP23 5SD
By
Allen Smalls
Sound Research Laboratories LimitedConsultants in Noise & VibrationHead Office & Laboratory: Holbrook House, Little WaldingfieldSudbury, Suffolk CO10 0THTelephone (01787) 247595 Fax (01787) 248420e-mail:[email protected]
This report shall not be reproduced, except in full, without written approval of the laboratory
1.0 Summary
Tests have been done in SRL's Laboratory at Holbrook House, Sudbury,Suffolk, to determine the sound absorption coefficient of a barrier inaccordance with BS EN ISO 354:2003, BS EN 1793-1:1998 and BS EN1793-3:1998. Calculations done in accordance with BS EN 1793-1:1998 arenot UKAS accredited.
From these measurements the required results have been derived and arepresented in both tabular and graphic form in Data Sheet 1.
The results are given in 1/3rd octave bands over the frequency range 50Hz to 10KHz, which is beyond that required by the test standard. Measurementsoutside the standard frequency range are not UKAS accredited.
......................................... ........................................Allen Smalls Trevor HickmanLaboratory Manager Executive ConsultantQuality Manager Deputy Technical Manager
For and on behalf ofSound Research Laboratories Ltd
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Contents
1.0 Summary
2.0 Details of Measurements
3.0 Description of Test
4.0 Results
Data Sheets 1
Photograph 1
Drawing 1
Appendix 1: Test Procedure
Appendix 2: Measurement Uncertainty
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2.0 Details of Measurements
2.1 Location
Sound Research Laboratories LtdHolbrook HouseLittle WaldingfieldSudburySuffolkCO10 OTH
2.2 Test Date
19 December 2008
2.3 Instrumentation and Apparatus Used
Make Description Type
E D I Microphone MultiplexerMicrophone Power Supply Unit
Norwegian Real Time Analyser 830Electronics
Brüel & Kjaer 12mm Condenser Microphones 4166 Windshields UA0237
Pre Amplifiers 2639, 2669CMicrophone Calibrator 4231Omnipower Sound Source 4296
Larson Davis 12mm Condenser Microphone 2560
Thermo Hygro Temperature & Humidity Probe
TOA Graphic Equalizer E-1231Power Amplifier DPA-800
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2.4 References
BS EN ISO 11654:1997 Sound absorbers for use in buildings.Rating of sound absorption.
ATSM C423-01 Sound Absorption and sound Absorption Coefficients by the Reverberation RoomMethod
BS EN ISO 354:2003 Measurement of sound absorption in areverberation room
BS EN 1793-1:1998 Road traffic noise reducing devices - BS EN 1793-3:1998 Test method for determining the acoustic
performance.Part 1 - Intrinsic characteristics of soundabsorption.Part 3 - Normalised traffic noise spectrum.
2.5 Personnel Present
S O’Leary TilonJ Elliott Tilon
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3.0 Description of Test
3.1 Description of Sample
Tilon Composites sound absorbent barrier, see drawing 1 for construction.
Sampling plan: Enough for test only
Sample condition: New
Details supplied by Tilon
Sample installed by Tilon
3.2 Sample Delivery date
19 December 2008
3.3 Test Procedures
The sample was mounted/located and tested in accordance with the relevantstandards. The method and procedure is described in Appendix 1. Themeasurement uncertainty is given in Appendix 2.
Standards BS EN 1793 parts 1 and 3 have additional requirements formeasurement and these have been fully included in the test procedure.
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4.0 Results
The results of the measurements are given in Data Sheet 1. The singlenumber rating and category calculated to BS EN 1793-1:1998 are listed below.
Results relate only to the items tested.
A413Barrier2
CategoryDLa,dB
Single number ratingBS EN 1793-1:1998Description in BriefSRL
Test No.
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Data Sheet 1Data Sheet 1
The Laboratory Measurement of Random Incidence Sound Absorption to BS EN ISO 354:2003
Client: Tilon Composites Ltd
Test Date: 19/12/2008
Empty Room: Temperature: 17.2 °C Humidity: 46 %RH Pressure: 1020 mbar
Room with Sample: Temperature: 15.1 °C Humidity: 43 %RH Pressure: 1020 mbar
Sample Tilon Composites Sound Absorbent Barrier
Description:Mounting Method: A
Sample Area: 10.55 m2
Chamber Volume: 300 m3
Test 2Absorp Practical
Freq T1 T2 Coeff AbsorpHz sec sec Coeff #50* 3.87 3.74 0.0563* 4.08 2.57 0.67 n/a80* 5.27 3.20 0.57100 6.90 5.44 0.18125 7.36 4.78 0.34 0.30160 6.90 4.15 0.45200 7.16 3.61 0.64250 7.03 3.27 0.76 0.75315 6.51 2.89 0.90400 6.07 2.55 1.06500 5.10 2.24 1.17 1.00630 4.94 2.21 1.16800 5.31 2.30 1.151000 5.76 2.43 1.10 1.001250 5.62 2.46 1.051600 5.12 2.42 0.992000 4.61 2.27 1.00 1.002500 3.94 2.09 0.983150 3.23 1.87 0.944000 2.55 1.59 0.93 0.955000 1.95 1.30 0.936300* 1.43 1.03 0.888000* 1.09 0.82 0.89 n/a10000* 0.77 0.61 0.95
1.00
Class ACalculated to EN ISO 11654:1997
NRC 1.00Calculated to ASTM C 423-01
DLa 13dBCategory A4
Calculated to BS EN 1793-1:1998(Not UKAS accredited))
* Denotes frequencies outside the range covered
by BS EN ISO 354:2003 T1, empty room reverberation time
T2, room reverberation time with sample# Practical absorption coefficient, BS EN ISO 11654:1997 v3
100125
160200
250315
400500
630800
10001250
16002000
25003150
40005000
Frequency, Hz
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
1.1
1.2
Abs
orpt
ion
Coe
ffici
ent
Sound Absorption Coefficient
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Photograph 1 - Barrier Being Tested
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Drawing 1
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Appendix 1
Test Procedure
Measurements of Random Incidence Sound AbsorptionCoefficients to BS EN ISO 354:2003 - TP14 (Plane Absorbers)
In the laboratory, random incidence sound absorption coefficients are determined fromthe rate of decay of a sound field in a reverberation room, with and without a testsample installed. The rate of decay is described by the time a sound field takes todecay by 60dB, known as the reverberation time.
The reverberation room is constructed from 215mm brick, which is internally plasteredwith a reinforced concrete roof and floor. The room is rectangular and has a volumeof 300 cubic metres and a total surface area of 275m2. From the ceiling hang 10randomly positioned diffusers, each measuring 1.2m x 2.14m. The room is isolatedfrom the surrounding structure by the use of resilient mountings and seals, ensuringgood acoustic isolation.
Using at least two omnidirectional loudspeaker positions, broad band random noise isproduced in the room using an electronic generator and power amplifier. When theamplification system is switched off, the decay of sound is filtered into one-third octaveband widths and the reverberation times measured. This process is repeated for eachof six microphone positions and the values arithmetically averaged to obtain a finalvalue for each frequency.
The sample area should normally be between 10m2 and 15.7m2, this may be larger if itis suspected that the absorption properties will be low. The sample is laid on the floorof the reverberation room so that no part of it is closer than one metre from any edge ofthe boundaries. The procedure of measuring the reverberation times then repeated.
The sound absorption coefficients are calculated from the difference in decay rates foreach frequency according to the formula:
=asATS
where
is the random incidence absorption coefficientas is the increase in equivalent sound absorption area of the testAt
specimen (m2)is the area covered by the test specimen (m2)S
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The equivalent absorption area of the test specimen is further defined as:
AT = 55.3V 1c2T2
− 1c1T1
− 4V (m2 − m1 )
where
is the volume of the empty reverberation room (m3)Vis the speed of sound in the empty room (m/sec)c1is the reverberation time in the empty room (sec)T1is the power attenuation coefficient calculated according to ISO 9613-1m1using the climatic conditions that have been present in the emptyrooms during the measurement.
and have the same meanings as and but with the testc2,T2 m2 c1,T1 m1specimen in the room.
It is occasionally found that the absorption coefficient derived in this mannerreaches a value greater than unity. This is impossible, by definition, andinvestigation has shown that this anomaly is due to diffraction of the impingingsound waves at the edges of the sample. In practical terms this isinsignificant.
The measured absorption coefficients are used to calculate a single numberrating (DLa) and category, following the method set out in BS EN 1793-1:1998.
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Appendix 2
Measurement UncertaintyBS EN ISO 354:2003 - TP14
1. Introduction
The estimated values of uncertainty are based on a standard uncertaintymultiplied by a coverage factor of K = 2, which provides a level of confidence ofapproximately 95%.
Table 1: Uncertainty For Equivalent Absorption Area Measurement
9.08.15.66.74.38.14.65.05.33.23.53.12.82.72.21.81.61.6
10012516020025031540050063080010001250160020002500315040005000
Expanded uncertaintyK = 2, 95%
% of A1 or A2
Frequency, Hz
2. Estimation of Expanded Uncertainty For Sample Equivalent Sound AbsorptionArea
The expanded uncertainty, UA,m2 is estimated by using the following formulae:-
UA =uA1100
2+ uA2
1002
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` where UA is the expanded uncertainty for the sampleequivalent sound absorption area, for K = 2,95%, m2
u is the estimated expanded uncertainty for theequivalent sound absorption area, taken fromTable 1 above, K = 2, 95%, % of A1 or A2
A1 is the equivalent sound absorption area of theempty room, m2
A2 is the equivalent sound absorption area of theroom with the sample, m2
3. Estimation of expanded Uncertainty For Sound Absorption Coefficients
The expanded uncertainty for sound absorption coefficients, U , is estimatedsusing the following formulae:-
U =ssUAA
where U is the expanded uncertainty for sounds
absorption coefficients, K=2, 95%
is the sound absorption coefficients
UA is the expanded uncertainty for the sampleequivalent sound absorption area, K=2, 95%,m2
A is the sample equivalent sound absorptionarea, m2
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