NF EN ISO 9614-3
Acoustics - Determination of sound power levels of noise sources using sound intensity - Part 3 : precision method for measurement by scanning
ISO 9614-3:2002 specifies a method for measuring the component of sound intensity normal to a measurement surface which is chosen so as to enclose the sound source(s) of which the sound power level is to be determined. Surface integration of the intensity component normal to the measurement surface is approximated by subdividing the measurement surface into contiguous partial surfaces, and scanning the intensity probe over each partial surface along a continuous path which covers the extent of the partial surface. The measurement instrument determines the averaged normal intensity component and averaged squared sound pressure over the duration of each scan. The scanning operation can be performed either manually or by means of a mechanical system. The octave band or band-limited weighted sound power level is calculated from the measured one-third-octave- band values. The method is applicable to any source for which a physically stationary measurement surface can be defined, and on which the sound generated by the source under test and by other significant extraneous sources are stationary in time. The source is defined by the choice of measurement surface. The method is applicable in specific test environments fulfilling all relevant requirements of ISO 9614-3. ISO 9614-3 specifies certain ancillary procedures, described in annex C, to be followed in conjunction with the sound power determination. The results are used to indicate the quality of the determination, and hence the grade of accuracy. If the quality of the determination does not meet the requirements of ISO 9614-3, the test procedure shall be modified in the manner indicated.ISO 9614-3 is not applicable to any frequency band in which the sound power of the source is found to be negative on measurement. It is applicable to sources situated in any environment which is neither so variable over time as to reduce the accuracy of the measurement of sound intensity to an unacceptable degree, nor subjects the intensity measurement probe to gas flows of unacceptable speed or unsteadiness.In some cases it will be found that the test conditions are too adverse to allow the requirements of ISO 9614-3 to be met. For example, extraneous noise levels can exceed the dynamic capability of the measuring instrument or can vary to an excessive degree during the test. In such cases the method given in ISO 9614-3 is not suitable for the determination of the sound power level of the source.
ISO 9614-3:2002 specifies a method for measuring the component of sound intensity normal to a measurement surface which is chosen so as to enclose the sound source(s) of which the sound power level is to be determined.
Surface integration of the intensity component normal to the measurement surface is approximated by subdividing the measurement surface into contiguous partial surfaces, and scanning the intensity probe over each partial surface along a continuous path which covers the extent of the partial surface. The measurement instrument determines the averaged normal intensity component and averaged squared sound pressure over the duration of each scan. The scanning operation can be performed either manually or by means of a mechanical system.
The octave band or band-limited weighted sound power level is calculated from the measured one-third-octave- band values. The method is applicable to any source for which a physically stationary measurement surface can be defined, and on which the sound generated by the source under test and by other significant extraneous sources are stationary in time. The source is defined by the choice of measurement surface. The method is applicable in specific test environments fulfilling all relevant requirements of ISO 9614-3.
ISO 9614-3 specifies certain ancillary procedures, described in annex C, to be followed in conjunction with the sound power determination. The results are used to indicate the quality of the determination, and hence the grade of accuracy. If the quality of the determination does not meet the requirements of ISO 9614-3, the test procedure shall be modified in the manner indicated.
ISO 9614-3 is not applicable to any frequency band in which the sound power of the source is found to be negative on measurement.
It is applicable to sources situated in any environment which is neither so variable over time as to reduce the accuracy of the measurement of sound intensity to an unacceptable degree, nor subjects the intensity measurement probe to gas flows of unacceptable speed or unsteadiness.
In some cases it will be found that the test conditions are too adverse to allow the requirements of ISO 9614-3 to be met. For example, extraneous noise levels can exceed the dynamic capability of the measuring instrument or can vary to an excessive degree during the test. In such cases the method given in ISO 9614-3 is not suitable for the determination of the sound power level of the source.
ISO 9614-3:2002 specifies a method for measuring the component of sound intensity normal to a measurement surface which is chosen so as to enclose the sound source(s) of which the sound power level is to be determined. Surface integration of the intensity component normal to the measurement surface is approximated by subdividing the measurement surface into contiguous partial surfaces, and scanning the intensity probe over each partial surface along a continuous path which covers the extent of the partial surface. The measurement instrument determines the averaged normal intensity component and averaged squared sound pressure over the duration of each scan. The scanning operation can be performed either manually or by means of a mechanical system. The octave band or band-limited weighted sound power level is calculated from the measured one-third-octave- band values. The method is applicable to any source for which a physically stationary measurement surface can be defined, and on which the sound generated by the source under test and by other significant extraneous sources are stationary in time. The source is defined by the choice of measurement surface. The method is applicable in specific test environments fulfilling all relevant requirements of ISO 9614-3. ISO 9614-3 specifies certain ancillary procedures, described in annex C, to be followed in conjunction with the sound power determination. The results are used to indicate the quality of the determination, and hence the grade of accuracy. If the quality of the determination does not meet the requirements of ISO 9614-3, the test procedure shall be modified in the manner indicated. ISO 9614-3 is not applicable to any frequency band in which the sound power of the source is found to be negative on measurement. It is applicable to sources situated in any environment which is neither so variable over time as to reduce the accuracy of the measurement of sound intensity to an unacceptable degree, nor subjects the intensity measurement probe to gas flows of unacceptable speed or unsteadiness. In some cases it will be found that the test conditions are too adverse to allow the requirements of ISO 9614-3 to be met. For example, extraneous noise levels can exceed the dynamic capability of the measuring instrument or can vary to an excessive degree during the test. In such cases the method given in ISO 9614-3 is not suitable for the determination of the sound power level of the source.
- Avant-proposv
- Introductionvi
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1 Domaine d'application1
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2 Références normatives2
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3 Termes et définitions2
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4 Exigences générales7
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4.1 Dimension de la source de bruit en essai7
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4.2 Nature du bruit émis par la source7
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4.3 Incertitude de mesure7
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5 Environnement acoustique9
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5.1 Critères de qualification de l'environnement d'essai9
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5.2 Intensité parasite9
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5.3 Vent et écoulements gazeux9
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5.4 Température9
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5.5 Configuration de l'environnement9
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5.6 Conditions atmosphériques10
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6 Appareillage10
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6.1 Généralités10
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6.2 Etalonnage et contrôle in situ10
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6.3 Séries de valeurs temporelles d'intensité acoustique et de pression acoustique11
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7 Installation et fonctionnement de la source11
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7.1 Généralités11
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7.2 Conditions de fonctionnement de la source en essai11
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8 Mesurage du niveau d'intensité acoustique normale12
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8.1 Détermination de la surface de mesurage12
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8.2 Détermination des trajectoires de balayage et des segments12
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8.3 Mesurages13
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8.4 Actions supplémentaires16
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9 Détermination du niveau de puissance acoustique16
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9.1 Calcul des puissances acoustiques élémentaires associées à chaque élément de la surface de mesurage16
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9.2 Calcul du niveau de puissance acoustique normalisé16
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10 Informations à consigner16
- Annexe A (informative) Liste des symboles employés dans la présente partie de l'ISO 961419
- Annexe B (normative) Calcul des indicateurs de champ21
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B.1 Généralités21
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B.2 Définition des indicateurs de champ21
- Annexe C (normative) Méthode d'obtention de la classe de précision requise24
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C.1 Critères de qualification24
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C.2 Action à prendre pour améliorer la précision de la détermination25
- Annexe D (informative) Effets des écoulements d'air sur le mesurage de l'intensité acoustique28
- Annexe E (informative) Effet de l'absorption du son à l'intérieur de la surface de mesurage30
- Annexe F (informative) Surface de mesurage et procédure de balayage31
- Annexe G (informative) Méthode d'obtention des moyennes temporelles de l'intensité et de la pression quadratique à partir d'une séquence d'intensités et de pressions quadratiques moyennées sur courte durée32
- Annexe H (informative) Normalisation du niveau de puissance acoustique33
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H.1 Généralités33
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H.2 Calcul du niveau normalisé de puissance acoustique33
- Annexe I (informative) Indicateurs de champ employés dans l'ISO 9614-1, l'ISO 9614-2 et l'ISO 9614-335
- Bibliographie37
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