PREDICTION OF ROOM ACOUSTICS PARAMETERS

Slides:



Advertisements
Similar presentations
© 2010 Pearson Education, Inc. Conceptual Physics 11 th Edition Chapter 21: MUSICAL SOUNDS.
Advertisements

Angelo Farina Dip. di Ingegneria Industriale - Università di Parma Parco Area delle Scienze 181/A, Parma – Italy
Angelo Farina Dip. di Ingegneria Industriale - Università di Parma Parco Area delle Scienze 181/A, Parma – Italy
Acoustical parameters ISO 3382
SYN-AUD-CON Acoustic Test and Measurement Seminar The Early Sound Field: Properties, Perceptual Attributes, and Measurement Methods NEIL THOMPSON SHADE.
Basic Acoustics Inverse square law Reinforcement/cancellation
ROOM ACOUSTICS DEFINITION: INTRODUCTION SOUND ABSORPTION
Abigail Stefaniw Room Acoustics for Classrooms: measurement techniques University of Georgia Classroom Acoustics Seminar.
Kristela Milan III - Galileo. Sound surrounds us all the time. From the chirping of birds when we wake up to the croaking of frogs at night. All the sounds.
Auditorium Acoustics Chapter 23. Sound Propagation Free field sound pressure proportional to 1/r SPL drops 6 dB with every doubling of distance. Indoors.
Room Acoustics. Reverberation Reverberation direct sound reflected sounds.
Chapter-8 Room and Auditorium Acoustics 1.Criteria in Acoustical Design The acoustical quality of a room is determined largely by its Reverberation time.
Auditorium Acoustics 1. Sound propagation (Free field)
Interference and beats. Objectives Investigate and analyze characteristics of waves, including frequency and amplitude. Investigate and analyze behaviors.
Vocabulary to know Acoustics is the Science that deals with the waves, frequency, amplitude, pitch, transmission, reception, control, effects, and production.
Vern J. Ostdiek Donald J. Bord Chapter 6 Waves and Sound (Section 5)
Acoustics of Concert Halls and Rooms SOME BASICS OF ARCHITECTURAL ACOUSTICS Auditorium Acoustics Science of Sound, Chapter 23 Principles of Vibration and.
Reflections Diffraction Diffusion Sound Observations Report AUD202 Audio and Acoustics Theory.
ELEC 407 DSP Project Algorithmic Reverberation – A Hybrid Approach Combining Moorer’s reverberator with simulated room IR reflection modeling Will McFarland.
PREDICTION OF ROOM ACOUSTICS PARAMETERS
3-D Sound and Spatial Audio MUS_TECH 348. Cathedral / Concert Hall / Theater Sound Altar / Stage / Screen Spiritual / Emotional World Subjective Music.
Reflection Based Scatter Updated for Odeon 12 Reflection Based Scatter A scattering method that combines Roughness and Diffraction effects Claus Lynge.
SUBJECTIVE ATTRIBUTES OF SOUND Acoustics of Concert Halls and Rooms Science of Sound, Chapters 5,6,7 Loudness, Timbre.
Dr. Jie ZouPHY Chapter 4 (Hall) Sound Propagation.
PH 105 Dr. Cecilia Vogel Lecture 4. OUTLINE  Room Acoustics  concert hall properties.
Fiber-Optic Communications James N. Downing. Chapter 2 Principles of Optics.
SUBJECTIVE AND OBJECTIVE ROOM ACOUSTIC PARAMETERS Acoustics of Concert Halls and Rooms Science of Sound, Chapter 23 Concert Halls and Opera Houses (Beranek.
GEOMETRICAL DESIGN STUDIES ACOUSTICS OF CONCERT HALLS AND ROOMS Handbook of Acoustics, Chapter 9 Long, Architectural Acoustics, Chapter 19.
PH 105 Dr. Cecilia Vogel Lecture 4. OUTLINE  Room Acoustics  direct and early sound  precedence effect  echoes and anechoic chamber  reverberation.
STUDIOS AND LISTENING ROOMS
NORMAL MODES AND COUPLED ROOMS ACOUSTICS OF CONCERT HALLS AND ROOMS Principles of Vibration and Sound Chapters 6 and 11.
Reverberation parameters and concepts Absorption co-efficient
So far: Historical overview of speech technology  basic components/goals for systems Quick review of DSP fundamentals Quick overview of pattern recognition.
EE513 Audio Signals and Systems Noise Kevin D. Donohue Electrical and Computer Engineering University of Kentucky.
ROOM ACOUSTIC MEASUREMENTS ACOUSTICS OF CONCERT HALLS AND ROOMS Handbook of Acoustics, Chapter 9 Schroeder (1965)
Acoustics Reverberation.
Architectural Acoustics II Indoor Acoustical Phenomena Prof S K Tang.
-ِAcoustics -Arch 353 -Dr. Abdelrahman Elbakheit -References الصوتيات, د. سعود صادق حسن.1.
SOUND IN THE WORLD AROUND US. OVERVIEW OF QUESTIONS What makes it possible to tell where a sound is coming from in space? When we are listening to a number.
Chapter 5: Normal Hearing. Objectives (1) Define threshold and minimum auditory sensitivity The normal hearing range for humans Define minimum audible.
Acoustics of classrooms, restaurants and offices Eng.Ivaylo Hristev.
Fundamentals of Audio Production. Chapter 1 1 Fundamentals of Audio Production Chapter One: The Nature of Sound.
L 18 Auditorium and Room Acoustics. Dekelbaum Concert Hall at the U MD Smith Center.
Room Acoustics Bouncing Around October 27, Music and Other Sounds Come from a source. The source is not isolated, it is in an environment. The environment.
Sound field descriptors Eng.Ivaylo Hristev. Contents 1. Wave acoustics. Room resonances. 2. Ray acoustics. Raytracing. 3.Statistical acoustics. Reverberation.
3-D Sound and Spatial Audio
EE Audio Signals and Systems Room Acoustics Kevin D. Donohue Electrical and Computer Engineering University of Kentucky.
3-D Sound and Spatial Audio MUS_TECH 348. Environmental Acoustics, Perception and Audio Processing: Envelopment.
ARCHITECTURAL ACOUSTICS
Room and Auditorium Acoustics
ACOUSTICS Aural Comfort & Noise.
EE599-2 Audio Signals and Systems
Auditorium Acoustics 1. Sound propagation (Free field)
Propagation of Sound and Vibration
ROOM ACOUSTICS MEASUREMENT AND ASSESSMENT METHODS.
Radio Coverage Prediction in Picocell Indoor Networks
Sound absorption 16 November 2012 Sound Absorption.
? If a tree fell in a wood and there was no-one there to hear it – would it make a sound?
PREDICTION OF ROOM ACOUSTICS PARAMETERS
Interference and beats
Architectural Acoustics
ROOM ACOUSTICS.
ACOUSTICS part – 4 Sound Engineering Course
Auditorium Acoustics Science of Sound, Chapter 23
Bouncing Around October 26, 2007
Physics of Music, Spring 2018
Auditorium Acoustics 1. Sound propagation (Free field)
NORMAL MODES AND COUPLED ROOMS
Kierunek „Elektronika”, rok II
AUDITORIUM ACOUSTICS REFERENCES:
Presentation transcript:

PREDICTION OF ROOM ACOUSTICS PARAMETERS Acoustics of Concert Halls and Rooms PREDICTION OF ROOM ACOUSTICS PARAMETERS Handbook of Acoustics Gade, Chapter 9 (2007)

•REVERBERATION TIME (RT) •STRENGTH (G) •CLARITY (C) SEVEN OBJECTIVE ROOM ACOUSTICS PARAMETERS IMPORTANT IN SUBJECTIVE QUALITIES OF A CONCERT HALL •REVERBERATION TIME (RT) •EARLY DECAY TIME (EDT) •STRENGTH (G) •CLARITY (C) •LATERAL ENERGY FRACTION (LEF) •INTERAURAL CROSS CORRELATION (IACC) •EARLY SUPPORT (STearly) Gade, 2007

REVERBERATION TIME SABINE EQUATION: RT = 0.161 V/(ΣSiαi + 4mV) V is volume, Si is area of surface with absorption coefficient αi and m is air absorption per unit volume. Sabine equation applies quite well to rooms whose dimensions are larger than the sound wavelength and whose absorption is well distributed throughout the room. NORRIS-EYRING EQUATION: RT = - 4v/cS ln(1-<α>) <α> is average random-incidence absorption coefficient For rooms with one or more very absorbing surfaces the Norris-Eyring equation usually gives a better RT value.

IMPULSE RESPONSE THE BASIC SOURCE OF INFORMATION ABOUT THE AUDIBLE PROPERTIES OF THE SOUND FIELD IN A ROOM IS THE IMPULSE RESPONSE SIGNAL. WHEN RECORDED WITH A MULTICHANNEL TECHNIQUE TO PRESERVE THE INFORMATION ABOUT DIRECTION OF INCIDENCE IT CONTAINS ALL AVAILABLE INFORMATION FOR A GIVEN SOURCE AND RECEIVER LOCATION.

PREDICTION OF RELATIVE STRENGTH G: PREDICTION OF CLARITY CLARITY---The degree to which every detail of the performance can be perceived With exponential decay, the expected value of C becomes a function of RT alone: Cexp = 10 log [exp(1.104/RT) – 1] dB PREDICTION OF RELATIVE STRENGTH G: In a diffuse field: G = 10 log (RT/V) + 45 dB Sound strength G decreases with distance. The rate of decrease ΔG can be modeled in several ways.

SUGGESTED VALUES OF OBJECTIVE ROOM ACOUSTIC PARAMETERS IN UNOCCUPIED CONCERT HALLS FOR CLASSICAL MUSIC (Gade, 2007)

To minimize sound absorption in order to obtain strong reverberance (for classical music): •Keep the row-to-row distance and chair width small •Seat design: minimum absorption with minimum difference between occupied and empty seats (low back rests and upholster only surfaces covered by seated person) •Thick upholstery on seat (~80 mm) and back rest (~50 mm) to minimize difference between empty and occupied seats)

ABSORPTION COEFFICIENTS OF SEATING AREAS IN CONCERT HALLS FOR THREE DIFFERENT DEGREES OF UPHOLSTRY, BOTH EMPTY AND OCCUPIED (Gade, 2007)

PREDICTION BY COMPUTER SIMULATION COMPUTER SIMULATIONS TAKE INTO ACCOUNT THE GEOMETRY AND ACTUAL DISTRIBUTION OF THE ABSORPTION MATERIALS IN A ROOM AS WELL AS THE ACTUAL SOURCE AND RECEIVER POSITION. ROOM GEOMETRY IS REPRESENTED BY A 3-D CAD MODEL WHICH MAY ALREADY HAVE BEEN CREATED BY THE ARCHITECTS WHEN GEOMETRY IS COMPLETE, THE ABSORPTION VALUES FOR EACH OCTAVE BAND, THE SCATTER, AND THE ACOUSTIC TRANSPARENCY ARE ASSIGNED TO EACH SURFACE. SOURCE AND RECEIVER ARE ENTERED MOST MODELS DISREGARD PHASE AND USE AN ENERGY APPROXIMATION. THE SOUND PROPAGATION IS STUDIED BY (MILLIONS OF) RAYS DRAWN FROM SOURCE TO RECEIVER.

SCALE MODEL PREDICTION SCALE MODELING IS MORE EXPENSIVE AND TIME-CONSUMING THAN COMPUTER MODELING, BUT IS REGARDED AS MORE RELIABLE IN LARGE ROOMS WITH A LOT OF IRREGULAR SURFACES OR OBJECTS THAT DIFFRACT SOUND WAVES. IN TESTING A 1 : m SCALE MODEL, THE ACOUSTIC TEST FREQUENCY IS INCREASED BY A FACTOR m SO THAT THE RATIO OF WAVELENGTH TO LINEAR DIMENSIONS REMAINS THE SAME

RELATIONSHIPS BETWEEN ROOM ACOUSTIC PARAMETERS AND ROOM DESIGN VARIABLES (AS DERIVED FROM DATA FROM MORE THAN 50 HALLS ) Gade, 2007

LISTENER ENVELOPMENT (LEV), THE IMPRESSION OF BEING INSIDE AND SURROUNDED BY THE REVERBERANT SOUND FIELD, IS ONE IMPORTANT ASPECT OF SPACIOUSNESS. LATERAL ENERGY FRACTION (LEF) MEASURES THE AMOUNT OF EARLY ENERGY ARRIVING FROM THE SIDES INTERAURAL CROSS- CORRELATION COEFFICIENT (IACC) MEASURES THE SIMULARITY OF EARLY SOUND AT THE TWO EARS. (A SMALL VALUE OF IACC CONTRIBUTES TO SPACIOUSNESS).

EARLY and LATE SUPPORT EARLY SUPPORT LATE SUPPORT (Gade, 2007) EASE OF ENSEMBLE (HOW WELL THE MUSICANS CAN HEAR EACH OTHER) IS ANOTHER IMPORTANT PARAMETER FOR MUSICIANS THAT RELATES TO STearly

TIMBRE or TONE COLOR TIMBRE DESCRIBES THE ROOM INFLUENCE ON THE BALANCE BETWEEN HIGH, MIDDLE, AND LOW FREQUENCIES (whether the sound is harsh, bright, hollow, warm, etc.) BASS RATIO (BR) IS A GOOD MEASURE OF WARMTH (In these equations, T is the REVERBERATION TIME (RT)) INTIMACY, ANOTHER IMPORTANT QUALITY, IS RELATED TO INITIAL TIME DELAY GAP

SPEECH INTELLIGIBILITY THE MOST COMMON WAY TO ASSESS SPEECH INTELLIGIBILITY IS BY THE SPEECH TRANSMISSION INDEX (STI). THIS IS BASED ON THE IDEA THAT SPEECH CAN BE MODELED AS AN AMPLITUDE-MODULATED SIGNAL IN WHICH THE DEGREE OF MODULATION CARRIES THE SPEECH INFORMATION. STI IS MEASURED BY USING 7 BANDS OF NOISE EACH MODULATED BY 14 FREQUENCIES A FASTER MEASUREMENT METHOD USING ONLY TWO CARRIER BANDS AND FOUR PLUS FIVE MODULATION FREQUENCIES IS CALLED RAPID STI (RASTI)

THEORY AND PRINCIPLE IN MEASUREMENT OF RASTI Gade