Page 706 - Automotive Engineering Powertrain Chassis System and Vehicle Body
P. 706

Interior noise: Assessment and control    C HAPTER 21.1

           Therefore, it can be seen that L t is dependent on the area  concrete floors and ceilings. In one particular case (by
           of the panel.                                      way of example only), the adjoining brick wall is 4.8-m
             Also, L t is found to be dependent on the absorption  wide and 3.1-m high with 550-mm nominal thickness,
           (A) of the receiving room for a given intensity (I ) in the  and forms the whole of the common area between the
           source room. A receiving room with little absorption will  two rooms. One of the rooms is larger and is termed the
           have a higher sound pressure level than one with a large  receiving room. It has a depth of 20.2 m and a volume of
                                                                    3
           absorption.                                        200 m . The adjoining room has a depth of 4 m and
                                                                             3
             The sound TL for the panel and the NR in the suite  a volume of 60 m and is known as the source room. The
           can be thus related.                               receiving room is isolated from the surrounding structure
             Power incident on the panel                      and adjoining room by the use of resilient mountings and
                                                              seals.
             P i ¼ I i S                         (21.1.115)     Broadband white noise is produced in the source room
                                                              using a minimum of two loudspeakers. The average
             Power absorbed by the receiving room             sound pressure levels in each room are determined using
                                                              distributed arrays of microphones, connected to a suit-
             P t ¼ I t A                         (21.1.116)   able third octave analyser. The difference in the averaged
                                                              sound pressure levels forms the NR (shown as the upper
                         P i
             TL ¼ 10 log 10                                   curve in the left hand plot of Fig. 21.1-16). From this,
                         P t
                                                              and the knowledge of the 1/3 octave reverberation times
                           I i S
             TL ¼ 10 log 10                                   (also shown in Fig. 21.1-16), the measured SRI or TL can
                           I t A                              be found (shown as the lower curve in the left-hand plot

                                   S                          of Fig. 21.1-16).
             TL ¼ L i   L t þ 10 log 10          (21.1.117)     The absorption coefficient of the test panel may be
                                   A
                                                              measured according to standard procedures in an im-
             The difference in levels between the two rooms is  pedance tube or in a reverberation chamber (Section
           known as the noise reduction or NR                 21.1.9.1). The impedance tube method is restricted to
                                                              small samples of material and sound of normal incidence

                           I i                                and therefore when testing the acoustic absorption of
             NR ¼ 10 log 10    ¼ L i   L t       (21.1.118)
                           I t                                enclosure panels, a test based on measurements is made
                                                              in a reverberation chamber.
                                S
             TL ¼ NR þ 10 log 10                 (21.1.119)     It should be noted that both TL and absorption data
                                A                             are obtained from tests performed in reverberation
                                                              chambers with diffuse fields where the sound impinges
             According to the relations developed by Sabine, the
           absorption of the receiving room is related to its re-  on the material samples with an essentially random angle
           verberation time (T) – the time in seconds required for  of incidence. These ideal conditions may not be found in
           the level of the sound to drop by 60 dB. Therefore,  the case of a practical enclosure. In addition to this, the
                                                              laboratory tests may have been performed on a single
                 0:161 V                                      panel in isolation. The TL, and, to a lesser extent, ab-
             A ¼                                 (21.1.120)   sorption characteristics of a panel depend on the panel
                    T
                                                              dimensions and on its mounting arrangement. Therefore,
                                                    3
           where V is the volume of the receiving room (m ). The  the published laboratory specifications may not be fully
           reverberation time for each 1/3 octave band can readily  realistic in the case of an enclosure made up of a number
           be measured in the receiving room using a real-time  of panels mounted in a variety of ways.
           analyser.                                            When examining the acoustic performance of enclo-
             The transmission suite is constructed in such a way  sure panels it is important to consider absorption char-
           as to:                                             acteristics as fully as the TL qualities, if the detrimental
                                                              effects of acoustic resonances within the enclosure are to
             restrict the transmission of sound to paths passing di-
             rectly through the test panel;                   be avoided. In addition to TL data, manufacturers of
                                                              acoustic enclosures might also quote sound transmission
             provide a source field which impinges with random
             angles of incidence on the test panel.           class (STC) values for panels. The STC parameter was
                                                              developed based on studies made with noise sources
           For such tests, a panel could be mounted and sealed in an  typical of multifamily dwellings, and provides a conve-
           aperture within the brick dividing wall between two  nient and fairly successful single index specification of
           rectangular reverberant rooms, both of which may be  the transmission characteristics of a panel. To determine
           constructed from 215-mm brick with reinforced      the STC of a panel, the TL is measured in the sixteen


                                                                                                      717
   701   702   703   704   705   706   707   708   709   710   711