- •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
242 |
9 Sound Pressure Levels and Octave Bands |
acceptance of the new designation of the octave bands, the SIL was adapted to new octave bands and renamed preferred speech interference level (PSIL). PSIL is defined as the arithmetic average of SPL in the 500, 1000, and 2000 Hz octave bands [4,7]:
PSIL Lp500 þ Lp1000 þ Lp2000
3
PSIL curves
9.4Weighted Sound Pressure Level
Weightings were developed as a method to better subjectively evaluate the impact of noise on the human ear. The human ear is more sensitive to sounds at certain frequency ranges. Therefore, we apply weighting corresponding to sensitivity at different frequencies.
As mentioned in Sect. 9.2.5, weighting cannot be applied in SPL in the time domain. The weighted SPL can only be calculated in the frequency domain. The
9.4 Weighted Sound Pressure Level |
243 |
formula for calculating RMS pressure, which is used for calculating SPL, in the frequency domain is derived by Parseval’s theorem as shown in the flowchart below. Parseval’s theorem was proved in Sect. 9.2.5:
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Parseval s Theorem |
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Apply Weighting( |
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9.4.1Logarithm of Weighting
A weighted RMS pressure is an RMS pressure multiplied by a weighting factor W as:
P2RMS,w ¼ P2RMS ∙ W
Note that the weightings are applied to the square of RMS pressure. Assume that an RMS pressure PRMS has a sound pressure level of Lp as:
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The weighted sound pressure level Lp, w of the weighted RMS pressure is:
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¼ Lp þ 10 log 10ðWÞ
Based on the equations above, there are two ways to calculate the weighted sound pressure level Lp, w:
1.Applying the weighting W by multiplying P2RMS ∙ W:
2.Applying the weighting W by adding 10log10(W)
244 |
9 Sound Pressure Levels and Octave Bands |
It is easier to calculate the weighted sound pressure level Lp, w by adding 10log10(W) as a gain or loss of dB than by multiplying P2RMS ∙ W.
9.4.2A-Weighted Decibels (dBA)
There are three weightings that were initially introduced for noise levels corresponding to different ranges.
A-weighting is for levels below 55 dB.
B-weighting is for levels between 55 and 85 dB.
C-weighting is for levels above 85 dB.
However, A-weighting is used today to evaluate the response of human hearing at all levels. The three weightings 10log10(W) in dB to be added as a gain/loss for different frequencies are shown in the figure below. The table below also gives the A-weighting for some frequencies.
When sound pressure levels are measured, their spectrum is applied by the weighting attenuation at different frequencies to generate weighted sound pressure levels. The resulting spectral levels can be added by the dB addition rule to find the total (combined) weighted sound pressure levels. Weighted SPLs have units in dB, with the weighting letter appended (i. e., dBA) to indicate the type of weighting. A-weighting can be applied to narrow or m-octave band spectrums and can be either an analog filter or, in the case of digital equipment, simply an attenuation applied to the calculated spectrum.
Example 9.7
Given the octave band spectrum below:
Center frequency fo[Hz] |
125 |
250 |
500 |
1000 |
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Sound pressure level Lp[dB] |
50 |
58 |
76 |
80 |
46 |
(a)What is the PSIL and communication voice level at a distance of 1.2 m between the speaker and the listener?
(b)Determine the A-weighted spectrum.
(c)Calculate the A-weighted sound pressure levels.
Example 9.7: Solution
(a) Preferred speech interference level (PSIL) is calculated based on the three bands:
PSIL |
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76 þ 80 þ 46 |
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In PSIL curves of Sect. 9.3.3, based on PSIL¼67.3 dB and Distance ¼ 1.2 m., the voice level required is approximately “very loud voice”; see figure below:
9.4 Weighted Sound Pressure Level |
245 |
Table 9.1 Sound level conversion chart from a flat response to A-weighting
1 Octave band |
Frequency |
A-weighting |
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[Hz] |
[dB] |
0 |
31.5 |
39.5 |
1 |
63 |
26.2 |
2 |
125 |
16.2 |
3 |
250 |
8.7 |
4 |
500 |
3.2 |
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1000 |
0 |
6 |
2000 |
1.2 |
7 |
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1.1 |
9 |
16,000 |
6.7 |
(b) A-weighted spectrum.
Get A-weighting from Table 9.1 (or Fig. 9.1) and calculate:
Center frequency fo[Hz] |
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250 |
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33.8 |
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72.8 |
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pRMS2 |
2399 |
85,114 |
1.9E7 |
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52,481 |
11.9E7 |
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