Purdue University, Physics 220

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Purdue University, Physics 220 Lecture 21 Sound Lecture 21 Purdue University, Physics 220

Purdue University, Physics 220 Sound Waves Lecture 21 Purdue University, Physics 220

Purdue University, Physics 220 Speed of Sound In gas: the speed of sound depends on the composition and is proportional to the square root of the absolute temperature, Medium Speed (m/s) Air 343 Helium 1000 Water 1480 Steel 5790 Comparison of speed in solid, liquid, gas, helium is fun here. T in Kelvin T = 0 0C or 273 K Lecture 21 Purdue University, Physics 220

Purdue University, Physics 220 Intensity and Pitch For Sound Waves I = p02 / (2 r v) (po is the pressure amplitude) Proportional to p02 Loudness Loudness perception is logarithmic Threshold for hearing I0 = 10-12 W/m2 b = (10 dB) log10 ( I / I0) b2 – b1 = (10 dB) log10(I2/I1) Pitch Perception of frequency Lecture 21 Purdue University, Physics 220

Purdue University, Physics 220 Decibels Sound intensity level   = (10 dB) log10 ( I / I0) Units: Bels A ratio of 107 indicates a sound intensity of 7 bels or 70 decibels (dB) An intensity of 0 dB corresponds to the hearing threshold Intensity increase by factor 10  intensity level adds 10 dB Adding 3 dB to the intensity level doubles the intensity (log102=0.3) Alexander Graham Bell (1847-1922) Lecture 21 Purdue University, Physics 220

Purdue University, Physics 220 Question If 1 person can shout with loudness 50 dB. How loud will it be when 100 people shout? A) 52 dB B) 70 dB C) 150 dB b100 – b1 = (10 dB) log10(I100/I1) b100 = 50 + (10 dB) log10(100/1) b100 = 50 + 20 Lecture 21 Purdue University, Physics 220

Purdue University, Physics 220 Standing Sound Waves Pipe open at both ends Lecture 21 Purdue University, Physics 220

Purdue University, Physics 220 Standing Sound Waves Pipe open at one end Lecture 21 Purdue University, Physics 220

Standing Waves in Pipes Open at both ends: Pressure node at end l = 2 L / n n=1,2,3, ... Open at one end: Pressure antinode at closed end: l = 4 L / n n=1,3,5, ... Lecture 21 Purdue University, Physics 220

Purdue University, Physics 220 Organ Pipe Example A 0.9 m organ pipe (open at both ends) is measured to have it’s n=2 harmonic at a frequency of 382 Hz. What is the speed of sound in the pipe? Pressure node at each end. l = 2 L / n n=1,2,3.. l = L for n=2 harmonic f = v / l v = f l = (382 s-1 ) (0.9 m) = 343 m/s Lecture 21 Purdue University, Physics 220

Purdue University, Physics 220 iClicker What happens to the fundamental frequency of a closed pipe, if the air (v=343 m/s) is replaced by helium (v=972 m/s)? A) Increases B) Same C) Decreases Lecture 21 Purdue University, Physics 220

Purdue University, Physics 220 Timbre Fourier decomposition Fundamental + Overtones Lecture 21 Purdue University, Physics 220

Superposition & Interference Consider two harmonic waves A and B meeting at x=0. Same amplitudes, but 2 = 1.15 x 1. The displacement versus time for each is shown below: A(1t) B(2t) What does C(t) = A(t) + B(t) look like? Lecture 21 Purdue University, Physics 220

Superposition & Interference Consider two harmonic waves A and B meeting at x=0. Same amplitudes, but 2 = 1.15 x 1. The displacement versus time for each is shown below: A(1t) B(2t) CONSTRUCTIVE INTERFERENCE DESTRUCTIVE INTERFERENCE C(t) = A(t) + B(t) Lecture 21 Purdue University, Physics 220

Purdue University, Physics 220 Beats Add two cosines and remember the identity: where and cos(Lt) Beat Frequency: Lecture 21 Purdue University, Physics 220

Doppler Effect Moving Source Lecture 21 Purdue University, Physics 220

Doppler Effect Moving Source When source is coming toward you (vs > 0) Distance between waves decreases Frequency increases When source is going away from you (vs < 0) Distance between waves increases Frequency decreases fo = fs / (1- vs/v) Lecture 21 Purdue University, Physics 220

Purdue University, Physics 220 iClicker A police car passes you with its siren on. The frequency of the sound you hear from its siren after the car passes A) Increases B) Decreases C) Same Lecture 21 Purdue University, Physics 220

Doppler Effect Moving Observer Lecture 21 Purdue University, Physics 220

Doppler Effect Moving Observer When moving toward source (vo < 0) Distance between waves decreases Frequency increases When away from source (vo > 0) Distance between waves increases Frequency decreases fo = fs (1- vo/v) Lecture 21 Purdue University, Physics 220

Moving Observer and Source Combine: fo = fs (1-vo/v) / (1-vs/v) A: You are driving along the highway at 65 mph, and behind you a police car, also traveling at 65 mph, has its siren turned on. B: You and the police car have both pulled over to the side of the road, but the siren is still turned on. In which case does the frequency of the siren seem higher to you? A) Case A B) Case B C) same vs f vo f’ v Lecture 21 Purdue University, Physics 220