Auditorium acoustic (continued) 1. Sound sources Sound source can be characterized by power and directivity Directivity factor Q – ratio of sound intensity.

Slides:



Advertisements
Similar presentations
SYDNEY OPERA HOUSE.
Advertisements

SOUND PRESSURE, POWER AND LOUDNESS MUSICAL ACOUSTICS Science of Sound Chapter 6.
Basic Acoustics Inverse square law Reinforcement/cancellation
ROOM ACOUSTICS DEFINITION: INTRODUCTION SOUND ABSORPTION
PHY 102: Waves & Quanta Topic 3 Energy in wave motion
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.
SPH3U Exam Review Waves and Sound.
Auditorium Acoustics Chapter 23. Sound Propagation Free field sound pressure proportional to 1/r SPL drops 6 dB with every doubling of distance. Indoors.
Technology in Architecture Lecture 17 Sound in Enclosed Spaces Reverberation Auditorium Design Lecture 17 Sound in Enclosed Spaces Reverberation Auditorium.
Auditorium Acoustics 1. Sound propagation (Free field)
Reflections Diffraction Diffusion Sound Observations Report AUD202 Audio and Acoustics Theory.
Chapter 12 SOUND.
Chapter 14 Sound.
BASIC CONCEPTS IN ARCHITECTURAL ACOUSTICS ENVIRONMENTAL CONTROL III
Bike Generator Project Each lab section will build 1 bike generator Each lab group will build 1 energy board Connect and test energy board and bike generator.
A tutorial on acoustic measurements for the non-technician
Music Physics 202 Professor Lee Carkner Lecture 10.
Sound Transmission and Echolocation Sound transmission –Sound properties –Attenuation Echolocation –Decoding information from echos.
GEOMETRICAL DESIGN STUDIES ACOUSTICS OF CONCERT HALLS AND ROOMS Handbook of Acoustics, Chapter 9 Long, Architectural Acoustics, Chapter 19.
STUDIOS AND LISTENING ROOMS
Sound.
Acoustics Seminary 3. Problem 3.1 Getting acquainted with Fletcher curves The 10 kHz sinusoidal signal of a wave generator is connected to a loudspeaker.
1 Live Sound Reinforcement Audio measurements. 2 Live Sound Reinforcement One of the most common terms you will come across when handling any type of.
L6 and L7 Sound Intensity, Sound Level/Loudness (Decibels), The Ear.
Sound. Sound waves are longitudinal pressure waves.
Chapter 12 Preview Objectives The Production of Sound Waves
1 Sound Propagation in Different Environments What is Sound? Free Field Sound Field Rooms Sound in Motion.
Sound waves How they are generated and travel
Supervisor: Dr. Boaz Rafaely Student: Limor Eger Dept. of Electrical and Computer Engineering, Ben-Gurion University Goal Directional analysis of sound.
BA , 1 Basic Concepts of Sound Contents: Definitions dB Conversion Sound Fields dB ± dB.
Sound. Speed of sound in solids, liquids, and gases Speed of sound in gas (air): 344 m/sec. Speed of sound in liquid (water): 1100 m/sec Speed of sound.
Chapter 17 Sound Waves: part two HW 2 (problems): 17.22, 17.35, 17.48, 17.58, 17.64, 34.4, 34.7, Due Friday, Sept. 11.
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.
 Space… the sonic frontier. Perception of Direction  Spatial/Binaural Localization  Capability of the two ears to localize a sound source within an.
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.
Timo Haapsaari Laboratory of Acoustics and Audio Signal Processing April 10, 2007 Two-Way Acoustic Window using Wave Field Synthesis.
© Houghton Mifflin Harcourt Publishing Company Preview Objectives The Production of Sound Waves Frequency of Sound Waves The Doppler Effect Chapter 12.
Instructor: M Sc. Eng. Nagham Ali Hasan 2 nd semester 2008/2009 University of Palestine College of Applied Engineering & Urban Planning Department of Architecture,
SOUND PRESSURE, POWER AND LOUDNESS MUSICAL ACOUSTICS Science of Sound Chapter 6.
Properties of Sound There are several ways in which sounds can differ from one another. they can be louder or softer they can be of a high or low pitch.
Shrishail Kamble Acoustics is usually very broadly defined as "the science of sound." Hall Acoustics The shaping and equipping of an enclosed space to.
Sound Pressure, Power, and Intensity Chapter 6. Sound Pressure/Power/Intensity All three terms describe physical sensations. All three are perceived on.
Loudness level (phon) An equal-loudness contour is a measure of sound pressure (dB SPL), over the frequency spectrum, for which a listener perceives a.
Types of Sound Wave Reflections Unless properly controlled, reflected sounds can be detrimental to accurate monitoring Axial – 2 surface reflections Tangential.
Sound Waves Vibration of a tuning fork
Technology in Architecture
Chapter 12 Preview Objectives The Production of Sound Waves
SOUND PRESSURE, POWER AND LOUDNESS
ARCHITECTURAL ACOUSTICS
SOUND FUNDAMENTALS Prepared by:SHUBHAM UMAKANT GUPTA En no
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.
SPATIAL HEARING Ability to locate the direction of a sound. Ability to locate the direction of a sound. Localization: In free field Localization: In free.
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 Waves Vibration of a tuning fork.
Sound.
Room and Auditorium Acoustics
Loudness level (phon) An equal-loudness contour is a measure of sound pressure (dB SPL), over the frequency spectrum, for which a listener perceives a.
Auditorium Acoustics 1. Sound propagation (Free field)
The Importance of In-Mask Communications
Loudness level (phon) An equal-loudness contour is a measure of sound pressure (dB SPL), over the frequency spectrum, for which a listener perceives a.
Properties of sound.
Auditorium acoustic (continued)
ROOM ACOUSTICS.
Technology in Architecture
 Designing Auditoria.
Sound and Intensity Transverse vs. Longitudinal Waves Sound Frequency
Sound Intensity = Power / Area (Watts / Meter2)
Auditorium Acoustics 1. Sound propagation (Free field)
Sound, Decibels, Doppler Effect
Presentation transcript:

Auditorium acoustic (continued) 1. Sound sources Sound source can be characterized by power and directivity Directivity factor Q – ratio of sound intensity in front of the source to the averaged sound intensity Intensity drop as : Intensity level : For spherical source Q=1, for hemispherical Q=2, for source in a corner (which radiates into one- quarter of a sphere) Q=4 1

2. Sound sources in a room The distribution of sound level in a room can be considered as a sound field Three regions in a sound field: Near field - distance from the source is small compared to dimensions of the source. Intensity varies with location and depends on the type of the source. Free field – intensity drops as 1/r 2 (r is distance from the source). Intensity level drops 6dB when distance r doubles Reverberant field – region where reflected sound becomes important r Near fieldFree field Reverberant field 2

The shown temperatures are samples of a field

3. The Bass Loss Problem When sound drops off according to the inverse square law, the sound further from the source is not only perceived as less loud but also as deficient in the bass frequencies. This is a natural result of the human hearing response as revealed by the equal loudness curves. There is a bass discrimination in the human hearing response for soft sounds.inverse square lawequal loudness curves bass discrimination 4

Phon is equal to the sound pressure level in decibels at f = 1 kHz Equal Loudness Curves 30 Hz: 103 dB ~ 80 phons;( ) dB = 83 dB ~ 50 phons 200Hz: 76 dB ~ 80 phons; (76 -20) dB = 56 dB ~ 60 phons 5

4. Loudspeaker placemat A. Single-source system Preferred in most auditoriums. Generally consists of a cluster of loudspeakers with selected directivity factors Q. Preferred location in the center of the room, over the speaker head. (Vertical displacement of the source is not distracting because of our inability to localize sound in a vertical plane.) Aimed toward the listeners at the rear of the auditorium. B. Distributed-speaker system Useful for long room with low ceiling. Each unit mounted in the ceiling covers 60 ◦ - 90 ◦ If room is long it is important to have electronic time delay for rear speakers to avoid echo. Speakers should not be placed along the side walls because some listeners will hear sound from several loudspeakers at the same time Speakers should not be placed on each side of the stage or front wall, because some listeners will hear sound from one of the speakers before they hear the direct sound. 6

5. Acoustic diffusers are used to maintain the acoustic energy in a room, but at the same time removing strong echoes. Acoustic diffusion occurs in a haphazard (irregular) way in many historical buildings through the use of ornate wall decorations and statues. Modern rooms rarely have such decorations but may include curved walls or other architectural features to achieve some of the same effect 7