What is the integral of the sound intensity
The sound power emitted by sound sources cannot be recorded directly, but requires the measurement of other variables that describe the sound field, e.g. the sound pressure and the room acoustics, in order to then calculate the sound power. The following procedures can be distinguished:
Enveloping surface method (sound pressure and sound intensity method)
Reverberation room method
Comparative sound source method
These procedures are briefly outlined here. The details of the implementation of corresponding noise emission measurements according to the enveloping surface method, for example for determining the measuring points, determining room influence and background noise correction, as well as the different measurement standards are described in detail in the pocket book "Noise Measurement in Operation".
1Enveloping surface method
Of the various methods for determining the sound power level, the enveloping surface method has become the most popular in operational practice, as it can be carried out directly at the installation site of the machines if the spatial conditions and the effects of extraneous noise meet certain requirements.
At the Enveloping surface methodthe sound power emitted by a noise source throughMeasurement at numerous measuring pointson one including the sourceimaginary enveloping surface / measuring surface Srecorded (seeImage 1). When the machine is usually set up on a reflective floor, this envelope surface is either hemispherical or cuboid and ends on the floor.
To record the sound energy penetrating this area, sound pressure level measurements in accordance with DIN EN ISO 3744 to 3746 or sound intensity measurements in accordance with DIN EN ISO 9614-1, -2 and -3 can be carried out.
The enveloping surface method is based on the approach of determining the sound power P of a sound source by integrating the sound intensity I over a measuring surface S that completely surrounds the source (see Image 1):
P = (1)
with I.n= I.cos- Normal component of the sound intensity on the measuring surface.
Image 1:Acquisition of the sound power on a hemispherical measuring surface
In measuring practice, the integral described in equation 1 is approximated by dividing the measuring area S into n partial measuring areas S.idecomposed and for this the sound intensities Inidetected. The sound power then results from the following formula:
WithI.ni-Sound intensity of the partial measuring areaS.i
S.i-i-th partial measuring area
This sound power corresponds to the product of the sound intensity averaged over the measurement areaI.nand the measuring surface S.:
with`I.n- Average sound intensity flowing through the measuring surface S perpendicularly
The mean sound intensity 'I.nis determined in measuring practice by placing a sufficiently large number of measuring points evenly over the cuboid or hemispherical measuring surface S.distributed, the sound intensity is recorded perpendicular to the surface and the measured values are energetically averaged. More detailed information on the arrangement of the measuring points can be found in the corresponding measuring standards.
The sound power level LW.then results with reference to the specified reference sound power P0according to the following equation:
L.W.= 10lgdB (4)
L.W.= 10lgdB (5)
P.0=110-12W (= I0S.0) - reference sound power
I.0=110-12W / m2- reference intensity (hearing threshold)
S.0= 1m2- reference area
Equation (5) can be converted into the following sum formula:
L.W.= 10 lgdB (6)
The first summand 10 lg (/ I0) corresponds to the mean sound intensity level L.I.on the measuring surface. Since the sound intensity level LI.in a plane sound wave (ideal free field conditions) with the sound pressure level L.pmatches (see e.g. Maue "0 decibels + 0 decibels = 3 decibels"), the sound power level LW.under these conditions also calculate using the mean sound pressure level.
The sound power level LW.results from the following formula:
L.W.= `LI.+10 lgdB (7)
or in the plane sound wave (free field + far field):
L.W.= `Lp+10 lg
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