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VRIJE UNIVERSITEIT BRUSSEL Acoustics - the Dept. of ...

VRIJE UNIVERSITEIT BRUSSEL Acoustics - the Dept. of ...

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86 CHAPTER 5. SOUND INSULATIONFrequency Ref. value (in dB)100 33100 33125 36160 39200 42250 45315 48400 51500 52630 53800 541000 551250 561600 562000 562500 563150 56Table 5.1: Reference values for sound insulation <strong>of</strong> a wall from ISO 717.5.2 Airborne sound insulation <strong>of</strong> a wall5.2.1 Simple lawConsider a plane sound wave which is incident ona(simple) wall. We assumefollowing conditions are met :The wall is characterized by its mass per unit area (isotropic material).It is assumed infinitely long.The wall does not absorb sound (a = 0).The wall has no stiffness and no damping. On <strong>the</strong> source side a planeharmonic wave is normally incident on <strong>the</strong> partition wall. There is nodeformation within <strong>the</strong> wall: it displaces as a whole.On <strong>the</strong> source side one can write that <strong>the</strong> air particles have a zero velocityon <strong>the</strong> wall because this wall does not move and does not absorb sound (seealso Section 4.1). Because <strong>of</strong> <strong>the</strong> acoustically hard reflection if no absorptionis present <strong>the</strong> pressure doubles at <strong>the</strong> incident side 2p i . Applying <strong>the</strong>fundamental equation <strong>of</strong> dynamics on <strong>the</strong> wall surface :2p i −p d = ma (5.7)

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