- •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 |
1 Complex Numbers for Harmonic Functions |
1.1Review of Complex Numbers
This section and the next section cover the basic formulas of complex numbers in either high schoolor college-level mathematics courses. The goal of these two sections is to refresh your knowledge of complex numbers for harmonic functions. You can skim through these two sections if you already know these formulas.
So what are complex numbers? The polynomial equation:
X2 þ 1 ¼ 0
does not have a solution that can be represented by real numbers. Instead, the solution of this polynomial equation can be represented by the complex numbers:
p
X ¼ 1
The square root of -1 is not a real number and has been defined as an imaginary number.
Hence, a combination of a real and an imaginary number is called a complex number.
For example:
Z ¼ a þ jb
where a and b are real numbers, j is the imaginary number, and the bold face character indicates that Z is a complex number.
The following are some properties of complex numbers:
• The square of the imaginary number j is 1. That is:
j2 ¼ 1
• The absolute value of a complex number is called its modulus. That is:
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a2 þ b2 |
• The complex conjugate of Z ¼ a + jb is defined as:
Z ¼ a jb
• The addition of a complex conjugate function pair is a real number as shown:
Z þ Z ¼ a þ jb þ a jb ¼ 2a
The star symbol (*) indicates the complex conjugate of Z.
1.2 Complex Numbers in Polar Form |
3 |
1.2Complex Numbers in Polar Form
A complex number can be presented in both rectangular and polar coordinates as:
Z ¼ Ar þ jAi ¼ Ar2 þ Ai2 |
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Note that the complex number in polar coordinates (shown above) is formulated using trigonometric functions such as cosine and sine functions. The complex number in polar coordinates can be further expressed in a complex exponential format using Euler’s formula. Euler’s formula shows the relationship between the trigonometric functions and complex exponential functions:
e jθ ¼ cos ðθÞ j sin ðθÞ
Based on Euler’s formula, a complex number can be presented as a complex exponential function in polar form as:
Z ¼ Að cos ðθÞ þ j sin ðθÞÞ ¼ Aejθ
4 |
1 Complex Numbers for Harmonic Functions |
Imag
Real
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Based on the equation above, a real or imaginary number can be expressed in the complex exponential format as:
1 ¼ cos ð0Þ þ j sin ð0Þ ¼ e jð0Þ
π |
π |
π |
j ¼ cos 2 |
þ j sin 2 ¼ e |
jð2Þ |
1 ¼ cos ðπÞ þ j sin ðπÞ ¼ e jðπÞ |
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j ¼ cos 2 þ j sin 2 |
¼ e jð 2Þ |
1.3Four Equivalent Forms to Represent Harmonic Waves
A summary of the four equivalent forms for simple harmonic motion is shown in this section. The derivations of these four equivalent forms are shown in the following sections.
Four equivalent forms can be used to describe simple harmonic motion. The following is a summary of four equivalent forms used to describe simple harmonic motions:
(Form 1) |
Ac cos (ωt) As sin (ωt) |
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A cos (ωt + ϕ) |
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(Form 3) |
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Ae jðωtþϕÞ þ Ae jðωtþϕÞ |
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(Form 4) |
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ejωt |
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Real trigonometric function Real trigonometric function Complex conjugate function pair
Complex conjugate function pair
where A, Ac, and As are real numbers and have the relationships shown in the following table. In the figure below, A is a positive number; Ac and As are either positive or negative numbers. Therefore, the phase angle ϕ is between π and π, and
1.3 Four Equivalent Forms to Represent Harmonic Waves |
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Note that Form 1 and Form 2 are formulated using real numbers (R). Form 3 and Form 4 are formulated using complex numbers (C). In addition, Form 1 and Form 4 are formulated using implicit phase (IP) of ϕ. Form 2 and Form 3 are formulated using explicit phase (EP) of ϕ. According to these properties, the four forms above can be rearranged into the following table:
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R: Real Trigonometric Function |
IP: Implicit Phase of |
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EP: Explicit Phase of |
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Geometric Relationship |
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Geom 2 |
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Geom 3 |
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Note that Form 3 can also be expressed as:
(Form 3) 12 Ae jðωtþϕÞ þ Ae jðωtþϕÞ ¼ 12 Aejωtejϕ þ Ae jωte jϕ (Form 3.5)
Also, Form 3 and Form 4 are often expressed with a Re[] function which takes the real part of the complex number as Form 3’ and Form 4’.
(Form 3) |
21 |
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Ae jðωtþϕÞ |
þ Ae jðωtþϕÞ |
¼ Re |
Ae jðωtþϕÞ |
jAs e |
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(Form 4) |
2 |
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jωt |
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jωt |
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(Form 4’) |
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1 |
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jωt |
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