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

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

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1.7. SOURCE POWER 21with W 0 = 10 −12 W <strong>the</strong> reference level.One have to pay attention to <strong>the</strong> terms we use because all those differentlevels have <strong>the</strong> same units (dB).1.7.2 The sound field produced by a point sourceFor a spherical source <strong>the</strong> source power is W = I4πr 2 , with I <strong>the</strong> intensityaccording to <strong>the</strong> radius <strong>of</strong> this sphere on a distance r from <strong>the</strong> source. In adistant sound field r ≫ λ we can write I = p2 effρcand thus :W = p2 eff 4πr2ρc(1.38)from which one can get an expression for <strong>the</strong> effective sound pressure, measuredat a distance r from <strong>the</strong> source :√Wρcp eff =(1.39)4πr 2With known source acoustic power <strong>the</strong> sound pressure can be calculatedin a given point. The effective sound pressure decreases with increasingdistance 1 . One may rewrite Equation 1.39 as a function <strong>of</strong> values in dB.r√412Wp eff = ρc = 400 for air4πr 2⇒ p 2 eff = 412W4πr 2⇒p2 eff 412W=400∗10 −12 4πr 2 400∗10 −12⇒ L p = L W −10log(4πr 2 )For r = 1 one has approximately :L p = L W −10 (1.40)

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