prediction of room acoustics parameters

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PREDICTION OF ROOM ACOUSTICS PARAMETERS Handbook of Acoustics Chapter 9 Acoustics of Concert Halls and Rooms

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Acoustics of Concert Halls and Rooms. PREDICTION OF ROOM ACOUSTICS PARAMETERS. Handbook of Acoustics Chapter 9. SEVEN OBJECTIVE ROOM ACOUSTICS PARAMETERS IMPORTANT IN SUBJECTIVE QUALITIES OF A CONCERT HALL. • REVERBERATION TIME (RT) • EARLY DECAY TIME (EDT) • STRENGTH (G) • CLARITY (C) - PowerPoint PPT Presentation

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Page 1: PREDICTION OF ROOM ACOUSTICS PARAMETERS

PREDICTION OF ROOM

ACOUSTICS PARAMETERS

Handbook of Acoustics

Chapter 9

Acoustics of Concert Halls and Rooms

Page 2: PREDICTION OF ROOM ACOUSTICS PARAMETERS

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

Page 3: PREDICTION OF ROOM ACOUSTICS PARAMETERS

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.

Page 4: PREDICTION OF ROOM ACOUSTICS PARAMETERS

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.

Page 5: PREDICTION OF ROOM ACOUSTICS PARAMETERS

PREDICTION OF CLARITY

PREDICTION OF RELATIVESTRENGTH G:

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

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.

Page 6: PREDICTION OF ROOM ACOUSTICS PARAMETERS

SUGGESTED VALUES OF OBJECTIVE ROOM ACOUSTIC PARAMETERS IN UNOCCUPIED CONCERT HALLS FOR CLASSICAL MUSIC

(Gade, 2007)

Page 7: PREDICTION OF ROOM ACOUSTICS PARAMETERS

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)

Page 8: PREDICTION OF ROOM ACOUSTICS PARAMETERS

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

Page 9: PREDICTION OF ROOM ACOUSTICS PARAMETERS

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.

Page 10: PREDICTION OF ROOM ACOUSTICS PARAMETERS

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

Page 11: PREDICTION OF ROOM ACOUSTICS PARAMETERS

RELATIONSHIPS BETWEEN ROOM ACOUSTIC PARAMETERS AND ROOM DESIGN VARIABLES (AS DERIVED

FROM DATA FROM MORE THAN 50 HALLS ) Gade, 2007

Page 12: PREDICTION OF ROOM ACOUSTICS PARAMETERS

INTERAURAL CROSS- CORRELATION COEFFICIENT (IACC) MEASURES THE SIMULARITY OF EARLY SOUND AT THE TWO EARS. (A SMALL VALUE OF IACC CONTRIBUTES TO SPACIOUSNESS).

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

Page 13: PREDICTION OF ROOM ACOUSTICS PARAMETERS

EARLY and LATE SUPPORT

LATE SUPPORT

(Gade, 2007)

EARLY SUPPORT

EASE OF ENSEMBLE (HOW WELL THE MUSICANS CAN HEAR EACH OTHER) IS ANOTHER IMPORTANT PARAMETER FOR MUSICIANS THAT RELATES TO STearly

Page 14: PREDICTION OF ROOM ACOUSTICS PARAMETERS

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

INTIMACY, ANOTHER IMPORTANT QUALITY, IS RELATED TO INITIAL TIME DELAY GAP

(In these equations, T is the REVERBERATION TIME (RT))

Page 15: PREDICTION OF ROOM ACOUSTICS PARAMETERS

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)

Page 16: PREDICTION OF ROOM ACOUSTICS PARAMETERS

THEORY AND PRINCIPLE IN MEASUREMENT OF RASTI

Gade