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Sound Physics 202 Professor Lee Carkner Lecture 8
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Sound More generally: sound = longitudinal wave Unlike waves on a string, a sound wave propagates outward in all 3 dimensions Example: String wave 1D, sound wave 3D
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Sound Speed For sound the velocity is: v = (B/ ) ½ Bulk modulus is like tension (how “springy” the fluid is) Density is like linear density B = - p/( V/V) Example: Water is more dense than air, so why does sound travel faster in water? It has a much larger B. Water is hard to compress
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Wave Equations The displacement of any element of air will also be in the x direction and is represented by: s(x,t) = s m cos (kx- t) This is similar to the transverse wave equation but does not involve y
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Pressure Wave
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Pressure p(x,t) = p m sin (kx - t) Where p m is the pressure amplitude p m = (v ) s m This is not an absolute pressure but rather a pressure change
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Pressure Wave Equation
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Pressure and Displacement The pressure and the displacement variations are /2 radians out of phase When the displacement is zero the pressure is a maximum and away from where pressure is low
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Interference If an observer is an equal distance from each, the sound will be in phase For a phase difference of 2 the path length difference is L L
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Constructive and Destructive L=m The sound will be at max amplitude (louder than an individual source) L = (m+½) You can also have intermediate interference making the sound louder or softer
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Interference and You Why don’t we notice interference much? Each with a different L You hear a combination of many different L Not all will have strong interference at your location You don’t hold perfectly still at the spot with maximum interference
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Intensity of Sound I = P/A The units of intensity are W/m 2 I = ½ v 2 s m 2 Compare to expression for power in a transverse wave Depends on the square of the amplitude and the frequency (wave properties)
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Intensity and Distance As you get further away from the source the intensity decreases because the area over which the power is distributed increases I = P/A = P s /(4 r 2 ) Sounds get fainter as you get further away because the energy is spread out over a larger area I falls off as 1/r 2 (inverse square law)
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Inverse Square Law Source r 2r A 1 =4 r 2 I 1 = P s /A 1 A 2 =4 (2r) 2 = 16 r 2 = 4A 1 I 2 = P s /A 2 = ¼ I 1
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Next Time Read: 17.5-17.10
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