- •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
246 |
9 Sound Pressure Levels and Octave Bands |
Fig. 9.1 Frequency response for the A-, B-, and C-weighting
A-weighted sound pressure level (spectrum) can be calculated by adding the unweighted sound pressure level and A-weighted gain or loss as shown below:
Lp½dBA& ¼ Lp½dB& þ A weighting
Therefore, A-weighted spectrum is given by:
(33.8, 49.3, 72.8, 80, 47.2) dB at (125, 250, 500, 1000, 2000) Hz, respectively
(c) A-weighted SPL [dBA]:
LpT ½dBA& ¼ 10 log 10 |
33:8 |
þ 10 |
49:3 |
þ 10 |
72:8 |
80 |
þ 10 |
47:2 |
|
10 |
10 |
10 |
þ 1010 |
10 |
¼10 log ð2399 þ 85114 þ 1:9E7 þ 10:0E7 þ 52481Þ ¼ 10 log ð11:9E7Þ ¼ 80:8 ½dBA&
Therefore, the A-weighted SPL ¼ 80.8 [dBA].
9.5Homework Exercises
Exercise 9.1
The mathematical expression for a level is:
9.5 Homework Exercises |
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247 |
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L ½dB& ¼ 10 log 10 Ur |
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U |
|
Use the law of conservation of energy to show that the following formula for the |
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total (combined) level is valid: |
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Ltot ¼ 10 log 10 |
10L110½dB& |
þ 10L210½dB& |
þ . . . |
þ 10Ln10½dB& ½dB& |
Exercise 9.2
The sound pressure levels measured in the following five octave bands are:
Center frequency fo[Hz] |
250 |
500 |
1000 |
2000 |
4000 |
Sound pressure level Lp[dB] |
90 |
72 |
82 |
65 |
50 |
(a)Determine the unweighted sound pressure level.
(b)Determine the A-weighted spectrum of the octave bands.
(c)Calculate the A-weighted sound pressure levels.
(d)What is the PSIL and communication voice level at 1.2 m between a speaker and a listener?
(Answers): (a) 90.7 [dB]; (b) (81.3, 68.8, 82.0, 66.2, 51.0) [dBA]; (c) 84.9 [dBA];
(d) 73 [dB], shouting.
Exercise 9.3
The sound pressure levels measured in five of the octave bands are given below:
Center frequency fo[Hz] |
125 |
250 |
500 |
1000 |
2000 |
Sound pressure level Lp[dB] |
35 |
45 |
65 |
70 |
60 |
(a)Determine the unweighted sound pressure level.
(b)Determine the A-weighted spectrum of the octave bands.
(c)Calculate the A-weighted sound pressure levels.
(d)What is the PSIL and communication voice level at 1.5 m from a listener?
(Answers): (a) 71.5 [dB]; (b) (18.8, 36.3, 61.8, 70.0, 61.2) [dBA]; (b) 71.1 [dBA];
(c) 65 [dB], very loud voice.
Exercise 9.4
Given the time domain function p(t) below:
p(t) ¼ 0.02 cos (2π 500 t) + 0.04 sin (2π 1000 t)+ 0.06 cos (2π 1500 t) + 0.08 sin (2π 2000 t)[Pa]
248 |
9 Sound Pressure Levels and Octave Bands |
(a)Determine the total (combined) sound pressure level (SPL) using:
(i)The summation of the squares of the RMS pressures.
(ii)The SPLs of all individual frequencies.
(iii)The SPL spectrum of octave bands.
(b)Determine the A-weighted sound pressure level (SPL) based on the sound level conversion table.
(Answers): (a) i-iii 71.76 [dB]; (b) 72.72 [dBA].
Exercise 9.5
Given the sound pressure function p(t):
pðtÞ ¼ 0:03 cos ð2π 400 tÞ þ 0:04 sin ð2π 400 tÞ
þ0:06 cos ð2π 1200 tÞ þ 0:08 sin ð2π 1200 tÞ þ0:09 cos ð2π 1600 tÞ þ 0:12 sin ð2π 1600 tÞ½Pa&
(a)Calculate the unweighted sound pressure level.
(b)Calculate the A-weighted sound pressure level.
(c)Calculate the preferred speech interference level (PSIL).
(d)Determine the communication voice level at 0.6 m from a listener.
Hint: Combine the harmonic waves of the same frequencies into one harmonic wave function using the four equivalent forms.
(Answers): (a) 76.41[dB]; (b) 77.08[dBA]; (c) 70.14 [dB]; (d) raised voice.
Exercise 9.6
Given the sound pressure function p(t):
pðtÞ ¼ 0:05 cos ð800πtÞ þ 0:10 cos ð2400πtÞ þ 0:15 cos ð3200πtÞ½Pa&
(a)Calculate the unweighted sound pressure level.
(b)Calculate the A-weighted sound pressure level based on the sound level conversion table.
(c)Calculate the preferred speech interference level (PSIL).
(d)Determine the communication voice level at 0.6 m from a listener.
Answers): (a) 76.41[dB]; (b) 77.08[dBA]; (c) 70.14 [dB]; (d) raised voice.
9.5 Homework Exercises |
249 |
Exercise 9.7
The sound pressure levels measured in five of the octave bands are given below:
Center frequency fo[Hz] |
125 |
250 |
500 |
1000 |
2000 |
Sound pressure level Lp[dB] |
35 |
45 |
65 |
70 |
60 |
(a)Determine the unweighted total sound pressure level.
(b)Calculate the A-weighted sound pressure level.
(c)Calculate the preferred speech interference level (PSIL).
(d)Determine the communication voice level at 1 m from a listener.
(Answer): (a) 71.52 [dB]; (b) 71.08; (c) 65 [dB]; (d) raised voice.
Chapter 10
Room Acoustics and Acoustical Partitions
This chapter introduces room acoustics and acoustical partitions. Room acoustics studies the change of energy density at different locations due to the conditions of direct and reflected sound. Acoustical partitions are used to reduce noise from a source.
Formulas for evaluating transmission loss (TL) and noise reduction (NR) in a room due to partition walls are formulated in this chapter.
This chapter is organized into five sections as described below:
Section 10.1 introduces and defines three acoustic quantities: sound power (Sect. 10.1.1), acoustic intensity (Sect. 10.1.2), and energy density (Sect. 10.1.3). These acoustic quantities are used for deriving the formulas of transmission loss (TL) and noise reduction (NR). These three acoustic quantities are also commonly used in the analysis of room acoustics.
Section 10.2 introduces and defines three room quantities: absorption coefficient of surfaces (Sect. 10.2.1), room constant (Sect. 10.2.2), and reverberation time (Sect. 10.2.3). These room quantities are used in the analysis of room acoustics in the next section (Sect. 10.3).
Section 10.3 focuses on the analysis of room acoustics. A formula for calculating sound pressure level due to both direct and reverberant sound waves from a sound source is summarized below:
Q |
4 |
|
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LP ¼ Lw þ 10 log 4πr2 |
þ |
|
|
R |
where LP is the sound pressure level at a distance r from the acoustic source considering both the direct and reverberant sound waves, Lw is the sound power of the acoustic source, Q is the directivity factor of the acoustic, and R is room constant. The equation above will be derived in this section.
Section 10.4 introduces transmission loss (TL) due to acoustical partitions. A formula that relates the transmission loss (TL) to the incident sound pressure level (Lwi) and transmitted sound pressure level (Lwt) will be defined and is summarized
© The Author(s), under exclusive license to Springer Nature Switzerland AG 2021 |
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H. Lin et al., Lecture Notes on Acoustics and Noise Control, https://doi.org/10.1007/978-3-030-88213-6_10