BA 7666-11, 1 Basic Concepts of Sound Contents: Definitions dB Conversion Sound Fields dB ± dB.

Slides:



Advertisements
Similar presentations
Week 1: *Fundamentals of Sound *Sound Levels and the Decibel
Advertisements

Measuring Sound Contents: The Microphone The Sound Level Meter Leq
ACOUSTICS part - 2 Sound Engineering Course
Basics of Acoustics Mn/DOT MPCA FHWA Presenters:
SOUND PRESSURE, POWER AND LOUDNESS MUSICAL ACOUSTICS Science of Sound Chapter 6.
Diploma in Aviation Medicine Introduction to Acoustics
PHYSICS OF SOUND PHYSICS OF SOUND HEARING CONSERVATION PROGRAM 1 28 Jan 2013.
SOUND ENERGY, INTENSITY AND POWER The acoustic power of a sound source is the amount of sound energy produced by a source per second. Acoustic power.
BASIC CONCEPTS IN ARCHITECTURAL ACOUSTICS ENVIRONMENTAL CONTROL III
Acoustic Wave Equation. Acoustic Variables Pressure Density – Condensation Velocity (particle) Temperature.
1 Fall 2004 Physics 3 Tu-Th Section Claudio Campagnari Lecture 3: 30 Sep Web page:
SOUND WAVES AND SOUND FIELDS Acoustics of Concert Halls and Rooms Principles of Sound and Vibration, Chapter 6 Science of Sound, Chapter 6.
PH 105 Dr. Cecilia Vogel Lecture 9. OUTLINE  Finish ear/hearing  Source power level  Sound loudness  sound intensity level  sound pressure level.
Loudness Power, intensity, intensity level,. Power and intensity Sound detector Energy: will accumulate in time Power: rate of energy transfer, stays.
The Decibel Inverse Square Law / SPL Meters AUD202 Audio and Acoustics Theory.
Lesson 3 - Logs and Levels Math Prereqs. Examples Without using your calculator, find the following: (log 10 (2) = 0.30) log 10 (10 -3 ) = log 10 (1 x.
Auditorium acoustic (continued) 1. Sound sources Sound source can be characterized by power and directivity Directivity factor Q – ratio of sound intensity.
BA , 1 Principles of Acoustic Measurements Exercises: Basic Concepts of Sound Measuring Sound Measuring Sound in Practice Basic Frequency Analysis.
Bel One Bel = log (I 1 /I 0 ), where I 1 is the absolute measured power, and I 0 is a reference power. Reference used is usually the least sound level.
DB(decibel), and so on… … background for using digital audio editors Reference.
Basic Concepts: Physics 1/25/00. Sound Sound= physical energy transmitted through the air Acoustics: Study of the physics of sound Psychoacoustics: Psychological.
Chapter 16 – Waves and Sound
ME 220 Measurements & Sensors Mechanical Measurements Applications
Lecture 2 Most basic facts from Electricity needed for understanding telecommunications Local transmission lines in the telephone system Decibels Signals.
Understanding Decibels
Loudness October 18, 2006 What is it?? The Process.
Physics 203 – College Physics I Department of Physics – The Citadel Physics 203 College Physics I Fall 2012 S. A. Yost Chapters 11 – 12 Waves and Sound.
Acoustics/Psychoacoustics Huber Ch. 2 Sound and Hearing.
Environmental Technology Noise Assessment & Abatement Module 7.0.
SOUND Longitudinal Wave Travels through some medium Cannot travel through a vacuum How does vibrating drum produce sound? Skin moving up presses air.
Sound Waves Physic 11 · Chapter 9.
Noise Pollution and Control
Lesson 02 Physical quantities 5 th October 2012Physical quantities1.
Terminologies in Acoustics Building Utilities 3 M.S.Chua.
Sound
Instructor: M Sc. Eng. Nagham Ali Hasan 2 nd semester 2008/2009 University of Palestine College of Applied Engineering & Urban Planning Department of Architecture,
BA , 1 Basic Frequency Analysis of Sound Contents: Frequency and Wavelength Frequency Analysis Perception of Sound.
SOUND PRESSURE, POWER AND LOUDNESS MUSICAL ACOUSTICS Science of Sound Chapter 6.
The production of sound Waves always begin with A vibrating object.
Sound Pressure, Power, and Intensity Chapter 6. Sound Pressure/Power/Intensity All three terms describe physical sensations. All three are perceived on.
Applied Psychoacoustics Lecture 2: Basic Measurement Methods, Signal Detection Theory Jonas Braasch.
Intensity of a Spherical Wave
1 Intensity Scales Exponents Logarithms dB dB SPL.
AUD203: FINAL STUDY GUIDE. HEADPHONES Remember Various Types How does noise-cancelling work.
CS Spring 2014 CS 414 – Multimedia Systems Design Lecture 3 – Digital Audio Representation Klara Nahrstedt Spring 2014.
Honors Physics Chapter 14
(8.5).  Are longitudinal waves  Require a medium to travel through  The type of medium influences the speed of the sound wave  Sound travels faster.
3. Energy in Waves Updated May 13, Index A.Waves and Amplitude 1.Amplitude and Particle Velocity 2.Impedance (of a spring) 3.Specific (acoustic)
Welcome Back Minions Now we learn about… SOUND!!! (But first a small recap…)
SOUND PRESSURE, POWER AND LOUDNESS
ARCHITECTURAL ACOUSTICS
Physics Section 12.2 Apply the sound properties of intensity and resonance Intensity is the rate at which energy flows through a unit area perpendicular.
Physics Mrs. Dimler SOUND.  Every sound wave begins with a vibrating object, such as the vibrating prong of a tuning fork. Tuning fork and air molecules.
Basic theory of sound, piezomaterials and vibrations.
What is the absolute power of a sound with an intensity of X dB IL? What is the absolute power corresponding to 20 dB IL? What is the absolute power corresponding.
~ Sound ~ The Nature of Sound  Speed of Sound  Human hearing  Doppler effect  “Seeing” with sound.
Auditory demonstration : sound level and frequency Yang-Hann Kim.
It’s All Noise Lee Hager, COHC 3M Lee Hager, COHC 3M © 3M All Rights Reserved.
Noise & Sound Graeme Murphy – National Brand Manager, Industrial Equipment.
Lesson 02 Physical quantities
The Physics of Sound.
ACOUSTICAL CALCULATIONS
Auditorium acoustic (continued)
a brief revision of principles and calculations from Building Physics
AP Physics Section 12-1 to 12-3 Sound Properties.
Sound and Intensity Transverse vs. Longitudinal Waves Sound Frequency
Properties of Sound Chapter 16 Section 2.
Sound.
Warm Up 4.4, Day 1 Graph the logarithmic function. Begin by describing the shifts. Then state the domain, range, and asymptote. Domain: ________________.
Sound 13.2.
Presentation transcript:

BA , 1 Basic Concepts of Sound Contents: Definitions dB Conversion Sound Fields dB ± dB

BA , 2 Sound /1

BA , 3 Sound and Noise /1

BA , 4 Terminology of Sound dB L eq RMS Sound Pressure Constant percentage bandwidth Noise Dose Logarithmic scales Pascal Fast Slow Impulse RMS Peak Weighting 1/1 and 1/3 Octave Analysis Percentile level Statistical analysis L 10 L 90

BA , 5 Pressure vs. Power Temperature t [°C] Power P [W] Electrical Heater Analogy Pressure p [N/m 2 = Pa] Sound Source L p [dB] Power P [W]

BA , 6 Basic Parameters of Sound Under free-field conditions: Power:P [W] Intensity:  [J/s/m 2 ] = W/m 2 Pressure:p [Pa = N/m 2 ] The Sound Intensity vector,  describes the amount and direction of flow of acoustic energy at a given position P P2P2 P2P2  r1r1 r2r2   /2

BA , 7 Propagation of Sound t = 0 t = 1/4 T t = 1/2 T t = 3/4 T t = T Compression Extension Minimum compressionMaximum compression No compression

BA , 8 Sound Pressure Pressure [Pa] Pascal Time /1

BA , 9 Sound Pressure Pascal Atmospheric Pressure Mexico City New York Pressure [Pa] Acoustic Pressure Variations

BA , Range of Sound Pressure Pressure, p [Pa] /2

BA , 11 Basic Concepts of Sound Contents: Definitions dB Conversion Sound Fields dB ± dB

BA , 12 Sound Pressure, p [Pa] Range of Sound Pressure Levels Sound Pressure Level, L p [dB] /2

BA , 13 dB – decibel Ex. 1: p= 1 Pa LpLp = 20 log = 20 log = 94 dB Ex. 2: p= 31.7 Pa LpLp = 20 log = 20 log 1.58 × = 124 dB (p 0 = 20  Pa = 20 × Pa) L p = 20 log dB re 20  Pa

BA , 14 Perception of dBs Change in Sound Level (dB) Change in Perceived Loudness Just perceptible Noticeable difference Twice (or 1/2) as loud Large change Four times (or 1/4) as loud

BA , 15 Conversion to dB using Charts dB re 20  Pa Pressure [Pa] p 0 = 20  Pa 94 dB LpLp

BA , 16 Conversion to dB using Tables dB to Pressure Ratio Pressure Ratio  db  Pressure Ratio Pressure Ratio  db  Pressure Ratio

BA , 17 Simple Rules for Conversion Sound Pressure Level, L p dB re 20  Pa Sound Pressure, p [Pa] × 100 × 10 × 2 × 3 × 4 6 dB 10 dB 20 dB 40 dB 12 dB

BA , 18 Basic Concepts of Sound Contents: Definitions dB Conversion Sound Fields dB ± dB

BA , 19 Types of Sound Sources r: L p 2r: L p  6 dB r: L p 2r: L p  3 dB r: L p 2r: L p Plane source Point source Line source /1

BA , 20 Anechoic and Reverberant Enclosures /1

BA , 21 Pressure Field Loudspeaker Microphone Enclosure

BA , 22 Sound Fields Near field Far field Free fieldReverberant field LpLp Distance, r A1A1 2 × A 1 6 dB /2

BA , 23 Directivity Index Source Location Free field L = L p L = L p + 3 dB L = L p + 6 dB L = L p + 9 dB On a flat plane At a junction of two planes At a junction of three planes Directivity Factor Directivity Index, dB

BA , 24 Pressure Increase at Walls L = L p + 3 dB L = L p + 6 dB LpLp

BA , 25 Basic Concepts of Sound Contents: Definitions dB Conversion Sound Fields dB ± dB

BA , 26 Two Sound Sources L p1 = X dB L p2 = X dB L p1 + L p2 = X + 3 dB

BA , 27 Addition of dB Levels Example: L + dB  L dB L1L2LL+LtL1L2LL+Lt 55 dB 51 dB 4 dB 1.4 dB = 56.4 dB ========== 4 dB 1.4 dB /2

BA , 28 Subtraction of Noise Levels L S+N [dB] L N [dB]

BA , 29 Subtraction of dB Levels Ex: L S+N L N  L L  L S 60 dB 53 dB 7 dB 1 dB 60  1 = 59 dB ========== L  dB  L dB L S ~ L S+N 

BA , 30 Addition of many dB values Addition of sound levels : For L 1 = L 2 = L = L N Examples: N = 2: L Total = L dB N = 10: L Total = L dB log N N L 1 + L L N = ?

BA , 31 Conclusion Sound pressure level in dB is related to 2 * Pascal. The range of human hearing is 130 dB. To add or subtract dB-values use charts or formulas

BA , 32 Literature for Further Reading Acoustic Noise Measurements Brüel & Kjær (BT ) Noise Control - Principles and Practice Brüel & Kjær (188-81)