Copyright © 2018 John Wiley & Sons, Inc. and primarily advanced by Prof. A. Iskandar.

17-1 Speed of Sound (1 of 3) Link to heading

Learning Objectives

  • 17.01 Distinguish between a longitudinal wave and a transverse wave.
  • 17.02 Explain wavefronts and rays.
  • 17.03 Apply the relationship between the speed of sound through a material, the material’s bulk modulus, and the material’s density.
  • 17.04 Apply the relationship between the speed of sound, the distance traveled by a sound wave, and the time required to travel that distance.

17-2 Traveling Sound Waves (1 of 6) Link to heading

Learning Objectives

  • 17.05 For any particular time and position, calculate the displacement s(x,t)s(x, t) of an element of air as a sound wave travels through its location.
  • 17.06 Given a displacement function s(x,t)s(x, t) for a sound wave, calculate the time between two given displacements.
  • 17.07 Apply the relationships between wave speed vv, angular frequency ω\omega angular wave number kk, wavelength λ\lambda period TT, and frequency ƒƒ.

17-2 Traveling Sound Waves (2 of 6) Link to heading

  • 17.08 Sketch a graph of the displacement s(x)s(x) of an element of air as a function of position, and identify the amplitude sms_m and wavelength λ\lambda.
  • 17.09 For any particular time and position, calculate the pressure variation Δp\Delta p (variation from atmospheric pressure) of an element of air as a sound wave travels through its location.
  • 17.10 Sketch a graph of the pressure variation Δp(x)\Delta p(x) of an element as a function of position, and identify the amplitude Δpm\Delta p_m and wavelength λ\lambda.

17-2 Traveling Sound Waves (3 of 6) Link to heading

  • 17.11 Apply the relationship between pressure-variation amplitude Δpm\Delta p_m and displacement amplitude sms_m.
  • 17.12 Given a graph of position ss versus time for a sound wave, determine the amplitude sms_m and the period TT.
  • 17.13 Given a graph of pressure variation Δp\Delta p versus time for a sound wave, determine the amplitude \Delta p_mandtheperiod and the period T$.

17-3 Interference (1 of 6) Link to heading

17.14 If two waves with the same wavelength begin in phase but reach a common point by traveling along different paths, calculate their phase difference ϕ\phi at the point by relating the path length difference ΔL\Delta L to the wavelength λ\lambda.

  • 17.15 Given the phase difference between two sound waves with the same amplitude, wavelength, and travel direction, determine the type of interference between the waves (fully destructive interference, fully constructive interference, or indeterminate interference).
  • 17.16 Convert a phase difference between radians, degrees, and number of wavelengths.

17-4 Intensity and Sound Level (1 of 6) Link to heading

  • 17.17 Calculate the sound intensity II at a surface as the ratio of the power PP to the surface area AA.
  • 17.18 Apply the relationship between the sound intensity II and the displacement amplitude sms_m of the sound wave.
  • 17.19 Identify an isotropic point source of sound.
  • 17.20 For an isotropic point source, apply the relationship involving the emitting power PsP_s, the distance rr to a detector, and the sound intensity II at the detector.

17-4 Intensity and Sound Level (2 of 6) Link to heading

17.21 Apply the relationship between the sound level β\beta, the sound intensity II, and the standard reference intensity I0I_0.

  • 17.22 Evaluate a logarithm function (log)(\log) and an antilogarithm function (log1)(\log^{-1}).
  • 17.23 Relate the change in a sound level to the change in sound intensity.

17-5 Sources of Musical Sound (1 of 3) Link to heading

Learning Objectives

  • 17.24 Using standing wave patterns for string waves, sketch the standing wave patterns for the first several acoustical harmonics of a pipe with only one open end and with two open ends.
  • 17.25 For a standing wave of sound, relate the distance between nodes and the wavelength.
  • 17.26 Identify which type of pipe has even harmonics.
  • 17.27 For any given harmonic and for a pipe with only one open end or with two open ends, apply the relationships between the pipe length LL, the speed of sound vv, the wavelength λ\lambda the harmonic frequency ƒƒ, and the harmonic number nn.

17-6 Beats (1 of 2) Link to heading

Learning Objectives

  • 17.28 Explain how beats are produced.
  • 17.29 Add the displacement equations for two sound waves of the same amplitude and slightly different angular frequencies to find the displacement equation of the resultant wave and identify the time-varying amplitude.
  • 17.30 Apply the relationship between the beat frequency and the frequencies of two sound waves that have the same amplitude when the frequencies (or, equivalently, the angular frequencies) differ by a small amount.

17-7 The Doppler Effect (1 of 5) Link to heading

  • 17.31 Identify that the Doppler effect is the shift in the detected frequency from the frequency emitted by a sound source due to the relative motion between the source and the detector.
  • 17.32 Identify that in calculating the Doppler shift in sound, the speeds are measured relative to the medium (such as air or water), which may be moving.

17-7 The Doppler Effect (2 of 5) Link to heading

  • 17.33 Calculate the shift in sound frequency for (a) a source moving either directly toward or away from a stationary detector, (b) a detector moving either directly toward or away from a stationary source, and (c) both source and detector moving either directly toward each other or directly away from each other.
  • 17.34 Identify that for relative motion between a sound source and a sound detector, motion toward tends to shift the frequency up and motion away tends to shift it down.

17-8 Supersonic Speeds, Shock Waves (1 of 3) Link to heading

Learning Objectives

  • 17.35 Sketch the bunching of wavefronts for a sound source traveling at the speed of sound or faster.
  • 17.36 Calculate the Mach number for a sound source exceeding the speed of sound.
  • 17.37 For a sound source exceeding the speed of sound, apply the relationship between the Mach cone angle, the speed of sound, and the speed of the source.

Summary Link to heading

  • Sound Waves
    • Speed of sound waves in a medium having bulk modulus and density v=βρ(17-3)\tag{17-3} v = \sqrt{\frac{\beta}{\rho}}
  • Interference
    • If the sound waves were emitted in phase and are traveling in approximately the same direction, ϕ\phi is given by ϕ=ΔLλ2π.(17-21)\tag{17-21} \phi = \frac{\Delta L}{\lambda} 2 \pi.
  • Sound Intensity
    • The intensity at a distance rr from a point source that emits sound waves of power PsP_s is I=Ps4πr2.(17-28)\tag{17-28} I = \frac{P_s}{4\pi r^2}.
  • Sound Level in Decibel
    • The sound level b in decibels (dB) is defined β=(10dB)logII0(17-29)\tag{17-29} \beta = (10 {\rm dB}) \log \frac{I}{I_0} where I0I_0 (1012 W/m210^{-12} \ {\rm W/m^2}) is a reference intensity.
  • Standing Waves in Pipes
    • A pipe open at both ends f=vλ=nv2L,    n=1,2,3,.(17-39)\tag{17-39} f = \frac{v}{\lambda} = \frac{nv}{2L}, \ \ \ \ n = 1, 2, 3, \dots.
    • A pipe closed at one end and open at the other f=vλ=nv4L,    n=1,3,5,.(17-41)\tag{17-41} f = \frac{v}{\lambda} = \frac{nv}{4L}, \ \ \ \ n = 1, 3, 5, \dots.
  • The Doppler Effect
    • For sound the observed frequency ƒ’ƒ’ is given in terms of the source frequency ƒƒ by f=fv±vDv±vS(17-47)\tag{17-47} f’ = f \frac{v \pm v_D}{v \pm v_S}
  • Sound Intensity
    • The half-angle θ\theta of the Mach cone is given by sinθ=vvS(17-57)\tag{17-57} \sin \theta = \frac{v}{v_S}

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