- •Preface
- •Objectives of the Book
- •Style
- •Prerequisites
- •The Big Picture
- •Contents
- •1.1 Review of Complex Numbers
- •1.2 Complex Numbers in Polar Form
- •1.3 Four Equivalent Forms to Represent Harmonic Waves
- •1.4 Mathematical Identity
- •1.5 Derivation of Four Equivalent Forms
- •1.5.1 Obtain Form 2 from Form 1
- •1.5.2 Obtain Form 3 from Form 2
- •1.5.3 Obtain Form 4 from Form 3
- •1.6 Visualization and Numerical Validation of Form 1 and Form 2
- •1.8 Homework Exercises
- •1.9 References of Trigonometric Identities
- •1.9.1 Trigonometric Identities of a Single Angle
- •1.9.2 Trigonometric Identities of Two Angles
- •1.10 A MATLAB Code for Visualization of Form 1 and Form 2
- •2.2 Equation of Continuity
- •2.3 Equation of State
- •2.3.1 Energy Increase due to Work Done
- •2.3.2 Pressure due to Colliding of Gases
- •2.3.3 Derivation of Equation of State
- •2.4 Derivation of Acoustic Wave Equation
- •2.5 Formulas for the Speed of Sound
- •2.5.1 Formula Using Pressure
- •2.5.2 Formula Using Bulk Modulus
- •2.5.3 Formula Using Temperature
- •2.5.4 Formula Using Colliding Speed
- •2.6 Homework Exercises
- •3.1 Review of Partial Differential Equations
- •3.1.1 Complex Solutions of a Partial Differential Equation
- •3.1.2 Trigonometric Solutions of a Partial Differential Equation
- •3.2 Four Basic Complex Solutions
- •3.3 Four Basic Traveling Waves
- •3.4 Four Basic Standing Waves
- •3.5 Conversion Between Traveling and Standing Waves
- •3.6 Wavenumber, Angular Frequency, and Wave Speed
- •3.7 Visualization of Acoustic Waves
- •3.7.1 Plotting Traveling Wave
- •3.7.2 Plotting Standing Wave
- •3.8 Homework Exercises
- •4.2 RMS Pressure
- •4.2.1 RMS Pressure of BTW
- •4.2.2 RMS Pressure of BSW
- •4.3 Acoustic Intensity
- •4.3.1 Acoustic Intensity of BTW
- •4.3.2 Acoustic Intensity of BSW
- •4.5.1 Issues with Real Impedance
- •4.6 Computer Program
- •4.7 Homework Exercises
- •4.8 References
- •4.8.1 Derivatives of Trigonometric and Complex Exponential Functions
- •4.8.2 Trigonometric Integrals
- •5.1 Spherical Coordinate System
- •5.2 Wave Equation in Spherical Coordinate System
- •5.3 Pressure Solutions of Wave Equation in Spherical Coordinate System
- •5.4 Flow Velocity
- •5.4.1 Flow Velocity in Real Format
- •5.4.2 Flow Velocity in Complex Format
- •5.5 RMS Pressure and Acoustic Intensity
- •5.7 Homework Exercises
- •6.1 Review of Pressure and Velocity Formulas for Spherical Waves
- •6.2 Acoustic Waves from a Pulsating Sphere
- •6.3 Acoustic Waves from a Small Pulsating Sphere
- •6.4 Acoustic Waves from a Point Source
- •6.4.1 Point Sources Formulated with Source Strength
- •6.4.2 Flow Rate as Source Strength
- •6.5 Acoustic Intensity and Sound Power
- •6.6 Computer Program
- •6.7 Project
- •6.8 Objective
- •6.9 Homework Exercises
- •7.1 1D Standing Waves Between Two Walls
- •7.2 Natural Frequencies and Mode Shapes in a Pipe
- •7.3 2D Boundary Conditions Between Four Walls
- •7.3.1 2D Standing Wave Solutions of the Wave Equation
- •7.3.2 2D Nature Frequencies Between Four Walls
- •7.3.3 2D Mode Shapes Between Four Walls
- •7.4 3D Boundary Conditions of Rectangular Cavities
- •7.4.1 3D Standing Wave Solutions of the Wave Equation
- •7.4.2 3D Natural Frequencies and Mode Shapes
- •7.5 Homework Exercises
- •8.1 2D Traveling Wave Solutions
- •8.1.2 Wavenumber Vectors in 2D Traveling Wave Solutions
- •8.2 Wavenumber Vectors in Resonant Cavities
- •8.3 Traveling Waves in Resonant Cavities
- •8.4 Wavenumber Vectors in Acoustic Waveguides
- •8.5 Traveling Waves in Acoustic Waveguides
- •8.6 Homework Exercises
- •9.1 Decibel Scale
- •9.1.1 Review of Logarithm Rules
- •9.1.2 Levels and Decibel Scale
- •9.1.3 Decibel Arithmetic
- •9.2 Sound Pressure Levels
- •9.2.2 Sound Power Levels and Decibel Scale
- •9.2.3 Sound Pressure Levels and Decibel Scale
- •9.2.4 Sound Pressure Levels Calculated in Time Domain
- •9.2.5 Sound Pressure Level Calculated in Frequency Domain
- •9.3 Octave Bands
- •9.3.1 Center Frequencies and Upper and Lower Bounds of Octave Bands
- •9.3.2 Lower and Upper Bounds of Octave Band and 1/3 Octave Band
- •9.3.3 Preferred Speech Interference Level (PSIL)
- •9.4 Weighted Sound Pressure Level
- •9.4.1 Logarithm of Weighting
- •9.5 Homework Exercises
- •10.1 Sound Power, Acoustic Intensity, and Energy Density
- •10.2.2 Room Constant
- •10.2.3 Reverberation Time
- •10.3 Room Acoustics
- •10.3.1 Energy Density due to an Acoustic Source
- •10.3.2 Sound Pressure Level due to an Acoustic Source
- •10.4 Transmission Loss due to Acoustical Partitions
- •10.4.2 Transmission Loss (TL)
- •10.5 Noise Reduction due to Acoustical Partitions
- •10.5.1 Energy Density due to a Partition Wall
- •10.5.2 Sound Pressure Level due to a Partition Wall
- •10.5.3 Noise Reduction (NR)
- •10.6 Homework Exercises
- •11.1 Complex Amplitude of Pressure and Acoustic Impedance
- •11.1.3 Transfer Pressure
- •11.2 Complex Acoustic Impedance
- •11.3 Balancing Pressure and Conservation of Mass
- •11.4 Transformation of Pressures
- •11.5 Transformation of Acoustic Impedance
- •11.7 Numerical Method for Molding of Pipelines
- •11.8 Computer Program
- •11.9 Project
- •11.10 Homework Exercises
- •12.1.1 Equivalent Acoustic Impedance of a One-to-Two Pipe
- •12.2 Power Transmission of a One-to-Two Pipe
- •12.3 Low-Pass Filters
- •12.4 High-Pass Filters
- •12.5 Band-Stop Resonator
- •12.6 Numerical Method for Modeling of Pipelines with Side Branches
- •12.7 Project
- •12.8 Homework Exercises
- •Nomenclature
- •Appendices
- •Appendix 1: Discrete Fourier Transform
- •Discrete Fourier Transform
- •Fourier Series for Periodical Time Function
- •Formulas of Discrete Fourier Series
- •Appendix 2: Power Spectral Density
- •Power Spectral Density
- •Accumulated Sound Pressure Square
- •Sound Pressure Level in Each Band
- •References
- •Index
2.6 Homework Exercises |
47 |
! ¼ |
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¼ |
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31 nMvca2 |
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γv2 |
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where:
vca is the RMS colliding speed of particles.
For air at 15 C, the RMS colliding speed of particles can be calculated backward from the formula above as:
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¼ r |
¼ r: |
¼ |
h |
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i |
vca |
3c2 |
3 3402 |
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498 |
m |
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1 4 |
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Note that the RMS colliding speed of air particles is faster than the speed of sound and is related to the ratio, γ, of specific heats. Also, the ratio, γ, of specific heats is related to the ratio, α, as:
γ 3α þ 2 3α
The corresponding value of α of air is:
α ¼ 53
where α is a ratio between the total energy (rotational energy + translational energy) and the translational energy of molecules as:
12 Iaθ2ca þ 12 mav2ca ¼ α 12 mav2ca
2.6Homework Exercises
Exercise 2.1 The bulk modulus B and the density ρo of certain seawater are:
B ¼ 2:307 109 ½Pa&
hKgi
m3
Determine the speed of sound in this certain seawater.
m s
48 |
2 Derivation of Acoustic Wave Equation |
Exercise 2.2 Sound can propagate through gaseous He which has a molar mass:
h g i
M ¼ 4:003 mol
Determine the speed of sound in He at 15 C.
Hint: The ideal gas constant is the same for all gases. The ratio of specific heats
for He is 1.67.
(Answer) 1000 ms
Exercise 2.3 The average molar mass of the molecules in the air is given as:
h g i
M ¼ 28:95 mol
What is the speed of sound at 30 C?
m s
Chapter 3
Solutions of Acoustic Wave Equation
In this chapter, you will learn how to construct both traveling waves and standing waves by solving the acoustic wave equation derived in the previous chapter. We will limit the scope of this chapter to only one-dimensional plane waves. Spherical waves will be constructed by solving the acoustic wave equation derived in spherical coordinate systems in Chap. 5.
We will use three building blocks to construct both traveling waves and standing waves. Each building block represents one type of basic solution under a certain requirement. The foundation for these three building blocks is the acoustic wave equation. They are summarized as follows:
The Foundation: The acoustic wave equation Building Block 1: Basic complex solutions (BCSs)
Requirement: ωk ¼ c Building Block 2: Basic traveling waves (BTW)
Requirement: complex conjugate pairs Building Block 3: Basic standing waves (BSWs)
Requirement: same amplitude and opposite directions
© The Author(s), under exclusive license to Springer Nature Switzerland AG 2021 |
49 |
H. Lin et al., Lecture Notes on Acoustics and Noise Control, https://doi.org/10.1007/978-3-030-88213-6_3
50 |
3 Solutions of Acoustic Wave Equation |
Acoustic Wave Equation: |
, |
= |
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This is the Foundation for All Building Blocks |
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Requirement for complex solutions: |
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Basic Complex Solutions (BCSs) |
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Requirement for traveling waves: |
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Complex Conjugate Pairs |
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Basic Traveling Waves (BTWs) |
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Requirement for standing waves: |
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Same Amplitude and Opposite Directions |
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Basic Standing Waves (BSWs) |
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In Building Block 1, basic complex solutions (BCSs) are constructed based on the acoustic wave equation under the requirement ωk ¼ c. BCSs are the most direct solutions of the acoustic wave equation. But because BCSs are complex numbers, they have no physical attributes by themselves.
In Building Block 2, basic traveling waves (BTWs) are constructed using the BCSs under the requirement that the BCSs must be a complex conjugate pair. BTWs are the addition of a complex conjugate pair. Unlike BCSs, BTWs are real numbers and have physical attributes of traveling waves. Any traveling wave can be constructed by using the four BTWs.
In Building Block 3, basic standing waves (BSWs) are constructed using the BTWs under the requirement that two traveling waves are traveling in the opposite direction and have exactly the same amplitude. Any standing wave can be constructed by using the four BSWs.
These “basic” solutions and waves will be used as building blocks for acoustic analysis throughout this course. Basic solutions and waves allow for a more in-depth analysis of acoustics and noise control.
Based on the traveling waves, this chapter will demonstrate how to construct standing waves by adding two traveling waves that are moving in the opposite direction and having the same amplitude:
psðx, tÞ ¼ p ðx, tÞ þ pþðx, tÞ |
Þ |
ϕ |
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¼ A cos |
ωt þ kx þ |
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þ A cos ωt |
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¼ |
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2A cos |
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cos kx |
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