Acoustic Textiles - the Case of Wall Panels for Home Environment
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White Paper: Acoustics Primer for Music Spaces
WHITE PAPER: ACOUSTICS PRIMER FOR MUSIC SPACES ACOUSTICS PRIMER Music is learned by listening. To be effective, rehearsal rooms, practice rooms and performance areas must provide an environment designed to support musical sound. It’s no surprise then that the most common questions we hear and the most frustrating problems we see have to do with acoustics. That’s why we’ve put this Acoustics Primer together. In simple terms we explain the fundamental acoustical concepts that affect music areas. Our hope is that music educators, musicians, school administrators and even architects and planners can use this information to better understand what they are, and are not, hearing in their music spaces. And, by better understanding the many variables that impact acoustical environ- ments, we believe we can help you with accurate diagnosis and ultimately, better solutions. For our purposes here, it is not our intention to provide an exhaustive, technical resource on the physics of sound and acoustical construction methods — that has already been done and many of the best works are listed in our bibliography and recommended readings on page 10. Rather, we want to help you establish a base-line knowledge of acoustical concepts that affect music education and performance spaces. This publication contains information reviewed by Professor M. David Egan. Egan is a consultant in acoustics and Professor Emeritus at the College of Architecture, Clemson University. He has been principal consultant of Egan Acoustics in Anderson, South Carolina for more than 35 years. A graduate of Lafayette College (B.S.) and MIT (M.S.), Professor Eagan also has taught at Tulane University, Georgia Institute of Technology, University of North Carolina at Charlotte, and Washington University. -
Physics of Music PHY103 Lab Manual
Physics of Music PHY103 Lab Manual Lab #6 – Room Acoustics EQUIPMENT • Tape measures • Noise making devices (pieces of wood for clappers). • Microphones, stands, preamps connected to computers. • Extra XLR microphone cables so the microphones can reach the padded closet and hallway. • Key to the infamous padded closet INTRODUCTION One important application of the study of sound is in the area of acoustics. The acoustic properties of a room are important for rooms such as lecture halls, auditoriums, libraries and theatres. In this lab we will record and measure the properties of impulsive sounds in different rooms. There are three rooms we can easily study near the lab: the lab itself, the “anechoic” chamber (i.e. padded closet across the hall, B+L417C, that isn’t anechoic) and the hallway (that has noticeable echoes). Anechoic means no echoes. An anechoic chamber is a room built specifically with walls that absorb sound. Such a room should be considerably quieter than a normal room. Step into the padded closet and snap your fingers and speak a few words. The sound should be muffled. For those of us living in Rochester this will not be a new sensation as freshly fallen snow absorbs sound well. If you close your eyes you could almost imagine that you are outside in the snow (except for the warmth, and bizarre smell in there). The reverberant sound in an auditorium dies away with time as the sound energy is absorbed by multiple interactions with the surfaces of the room. In a more reflective room, it will take longer for the sound to die away and the room is said to be 'live'. -
Making It Sound As Good As It Tastes: Noise Reverberation Reduction in a Micro Distillery Tasting Room Andrew Sheehy Montana Tech of the University of Montana
Montana Tech Library Digital Commons @ Montana Tech Graduate Theses & Non-Theses Student Scholarship Spring 2016 Making it Sound as Good as it Tastes: Noise Reverberation Reduction in a Micro Distillery Tasting Room Andrew Sheehy Montana Tech of the University of Montana Follow this and additional works at: http://digitalcommons.mtech.edu/grad_rsch Part of the Occupational Health and Industrial Hygiene Commons Recommended Citation Sheehy, Andrew, "Making it Sound as Good as it Tastes: Noise Reverberation Reduction in a Micro Distillery Tasting Room" (2016). Graduate Theses & Non-Theses. 89. http://digitalcommons.mtech.edu/grad_rsch/89 This Publishable Paper is brought to you for free and open access by the Student Scholarship at Digital Commons @ Montana Tech. It has been accepted for inclusion in Graduate Theses & Non-Theses by an authorized administrator of Digital Commons @ Montana Tech. For more information, please contact [email protected]. 1 Making it Sound as Good as it Tastes: Noise Reverberation Reduction in a Micro Distillery Tasting Room Andrew John Sheehy, Dan Autenrieth, Julie Hart, and Scott Risser Montana Tech Publishable Paper submitted to Artisan Spirit Magazine 2 Abstract Noise reverberation in micro distillery tasting rooms can interfere with speech communication and negatively impact the acoustic quality of live music. Noise reverberation was characterized in a tasting room in Butte, MT by calculated and quantified methods. Sound absorbing baffles were then installed in an effort to reduce reverberation and improve room acoustics. The overall reverberation time and speech interference level were decreased by measureable amounts that corresponded with an increase in overall absorption in the space. Reverberation time decreased from 0.85 seconds to 0.49 seconds on average. -
Reverb 101: Room Reverberation and Better Listening Experiences
Reverb 101: Room Reverberation and Better Listening Experiences A great listening experience involves more than just high-quality audio equipment—the way sound moves around the room matters just as much. You don’t have to be an expert acoustician to create an impressive listening environment —just an understanding of some basic acoustic concepts will get you well on your way. The Basics of Reverberation Reverberation (or reverb) is important to think about when planning the acoustical treatments for your room. To define reverb, we first need to understand how sound travels from the source to your ear. When sound is emitted, sound waves take off in every direction. Some waves will travel the straight path from the source to your ear, and the rest will bounce around the room, ricocheting off of hard surfaces until they reach your ear or lose steam and die out. You hear the unadulterated direct sound first—then you start hearing indirect sounds as they arrive. Given that sound travels roughly 770 miles per hour, this happens very fast, and your brain interprets all the copies of sound together as one. The ratio of direct and indirect sounds determines the sound quality. That is where reverberation comes in. Reverberation is the collection of indirect sounds in an enclosed space. The more sound copies that pile up, the muddier the sound becomes. How Does Reverberation Affect the Listening Experience? When direct sound and reverberation combine in a favorable ratio, the sound is rich and full. The effect can bring music to life and even smooth out transitions between musical notes, creating a pleasant, desirable sound. -
Web-Based Psychoacoustics: Hearing Screening, Infrastructure, And
bioRxiv preprint doi: https://doi.org/10.1101/2021.05.10.443520; this version posted May 11, 2021. The copyright holder for this preprint (which was not certified by peer review) is the author/funder, who has granted bioRxiv a license to display the preprint in perpetuity. It is made available under aCC-BY-NC-ND 4.0 International license. Web-based Psychoacoustics: Hearing Screening, Infrastructure, and Validation Brittany A. Moka, Vibha Viswanathanb, Agudemu Borjiginb, Ravinderjit Singhb, Homeira Kafib, and ∗Hari M. Bharadwaja,b aDepartment of Speech, Language, and Hearing Sciences, Purdue University, West Lafayette, IN, United States bWeldon School of Biomedical Engineering, Purdue University, West Lafayette, IN, United States Abstract Anonymous web-based experiments are increasingly and successfully used in many domains of behavioral research. However, online studies of auditory perception, especially of psychoacoustic phe- nomena pertaining to low-level sensory processing, are challenging because of limited available control of the acoustics, and the unknown hearing status of participants. Here, we outline our approach to mitigate these challenges and validate our procedures by comparing web-based measurements to lab- based data on a range of classic psychoacoustic tasks. Individual tasks were created using jsPsych, an open-source javascript front-end library. Dynamic sequences of psychoacoustic tasks were imple- mented using Django, an open-source library for web applications, and combined with consent pages, questionnaires, and debriefing pages. Subjects were recruited via Prolific, a web-based human-subject marketplace. Guided by a meta-analysis of normative data, we developed and validated a screening pro- cedure to select participants for (putative) normal-hearing status; this procedure combined thresholding of scores in a suprathreshold cocktail-party task with filtering based on survey responses. -
Infrasound and Low Frequency Noise of a Wind Turbine
Vibrations in Physical Systems Vol.26 (2014) Infrasound and Low Frequency Noise of a Wind TurBine Malgorzata WOJSZNIS Institute of Applied Mechanics, Poznan University of Technology 3 Piotrowo Street, 60-965 Poznań [email protected] Jacek SZULCZYK Environmental Acoustics Laboratory EKO – POMIAR 4 Sloneczna Street, 64-600 Oborniki [email protected] ABstract The paper presents noise evaluation for a 2 MW wind turbine. The obtained results have been analyzed with regard to infrasound and low frequency noise generated during work of the wind turbine. The evaluation was based on standards and decrees binding in Poland. The paper presents also current literature data on the influ- ence of the infrasound and low frequency noise on a human being. It has been concluded, that the permissible levels of infrasound for the investigated wind turbine were not exceeded. Keywords: low frequency noise, infrasound, wind turbine 1. Introduction Research that has been conducted in the world for many years shows that noise can be described as sound below and above so called hearing threshold . It can be assumed that the infrasound , which cannot be heard by a human being, concerns frequencies below 20 Hz, and the ultrasound concerns frequencies above 20 kHz [1]. We receive it as me- chanical vibrations of the medium it passes through, transferring energy from the source in the form of acoustic waves. Puzyna in [1] describes infrasound as infraaccoustic vi- brations . Some investigations show that for some people the hearing level begins already at 16Hz, and sometimes even at 4Hz. Such a phenomenon occurs at appropriate condi- tions and at a high level of sound pressure [2]. -
Infrasound and Ultrasound
Infrasound and Ultrasound Exposure and Protection Ranges Classical range of audible frequencies is 20-20,000 Hz <20 Hz is infrasound >20,000 Hz is ultrasound HOWEVER, sounds of sufficient intensity can be aurally detected in the range of both infrasound and ultrasound Infrasound Can be generated by natural events • Thunder • Winds • Volcanic activity • Large waterfalls • Impact of ocean waves • Earthquakes Infrasound Whales and elephants use infrasound to communicate Infrasound Can be generated by man-made events • High powered aircraft • Rocket propulsion systems • Explosions • Sonic booms • Bridge vibrations • Ships • Air compressors • Washing machines • Air heating and cooling systems • Automobiles, trucks, watercraft and rail traffic Infrasound At very specific pitch, can explode matter • Stained glass windows have been known to rupture from the organ’s basso profunda Can incapacitate and kill • Sea creatures use this power to stun and kill prey Infrasound Infrasound can be heard provided it is strong enough. The threshold of hearing is determined at least down to 4 Hz Infrasound is usually not perceived as a tonal sound but rather as a pulsating sensation, pressure on the ears or chest, or other less specific phenomena. Infrasound Produces various physiological sensations Begin as vague “irritations” At certain pitch, can be perceived as physical pressure At low intensity, can produce fear and disorientation Effects can produce extreme nausea (seasickness) Infrasound: Effects on humans Changes in blood pressure, respiratory rate, and balance. These effects occurred after exposures to infrasound at levels generally above 110 dB. Physical damage to the ear or some loss of hearing has been found in humans and/or animals at levels above 140 dB. -
Musical Elements in the Discrete-Time Representation of Sound
0 Musical elements in the discrete-time representation of sound RENATO FABBRI, University of Sao˜ Paulo VILSON VIEIRA DA SILVA JUNIOR, Cod.ai ANTONIOˆ CARLOS SILVANO PESSOTTI, Universidade Metodista de Piracicaba DEBORA´ CRISTINA CORREA,ˆ University of Western Australia OSVALDO N. OLIVEIRA JR., University of Sao˜ Paulo e representation of basic elements of music in terms of discrete audio signals is oen used in soware for musical creation and design. Nevertheless, there is no unied approach that relates these elements to the discrete samples of digitized sound. In this article, each musical element is related by equations and algorithms to the discrete-time samples of sounds, and each of these relations are implemented in scripts within a soware toolbox, referred to as MASS (Music and Audio in Sample Sequences). e fundamental element, the musical note with duration, volume, pitch and timbre, is related quantitatively to characteristics of the digital signal. Internal variations of a note, such as tremolos, vibratos and spectral uctuations, are also considered, which enables the synthesis of notes inspired by real instruments and new sonorities. With this representation of notes, resources are provided for the generation of higher scale musical structures, such as rhythmic meter, pitch intervals and cycles. is framework enables precise and trustful scientic experiments, data sonication and is useful for education and art. e ecacy of MASS is conrmed by the synthesis of small musical pieces using basic notes, elaborated notes and notes in music, which reects the organization of the toolbox and thus of this article. It is possible to synthesize whole albums through collage of the scripts and seings specied by the user. -
Determination of Speed of Sound in the Air Using Kundt's Tube. the Exercise Aims to Determine the Speed of Sound in the Air with Kundt's Pipe's Application
Determination of speed of sound in the air using Kundt's tube. The exercise aims to determine the speed of sound in the air with Kundt's pipe's application. 1. Theory Waves could be divided into three main types: 1. Mechanical waves – waves propagate as an oscillation of the medium, for example, sea waves, sound waves and seismic waves. They are propagating consistent with classical physics laws and can exist only in water, air or solid-state. 2. Electromagnetic waves – waves propagate as continuous changes of electric and magnetic fields. This kind of waves doesn't require a medium, and it can propagate in a vacuum. Light, radio waves, TV waves, microwaves, X-rays are examples of electromagnetic waves. They propagate with the speed of light. 3. Matter waves – waves related to all objects in motion. The wavelength of matter waves is given by ℎ ℎ de Broglie formula λ = = . It is easier to detect matter waves of particles (e.g. electrons) than 푚푣 푝 heavy objects like a human. The waves can be divided into two types depending on the oscillation medium's direction with respect to wave propagation direction. If the oscillation direction is perpendicular to the propagation's direction, this kind of wave is called the transverse wave. If the oscillation direction is parallel to the propagation's direction, this kind of wave is called a longitudinal wave. A following formula is used to describe the propagation of the harmonic wave : 푦(푥, 푡) = 퐴 푠푖푛(푘푥 − ω푡), where: 푦(푥, 푡, ) – displacement as a function of position x and time t, A – amplitude of the wave, k – wavenumber equal to 2π/λ, where λ is a wavelength (distance between to minimum or maximum of the wave) ω – circular frequency equal to 2π/T, where T means oscillation period (kx-ωt) – phase of the wave. -
Wind Farm Infrasound Detectability and Its Effects on the Percep- Tion of Wind Farm Noise Amplitude Modulation
Wind farm infrasound detectability and its effects on the percep- tion of wind farm noise amplitude modulation Duc Phuc Nguyen (1), Kristy Hansen (1), Branko Zajamsek (2), Gorica Micic (2) and Peter Catcheside (2) (1) College of Science and Engineering, Flinders University, Adelaide, Australia (2) Adelaide Institute for Sleep Health, Flinders University, Adelaide, Australia ABSTRACT Some residents attribute adverse effects to the presence of wind farm (WF) infrasound. However, dominant fea- tures of windfarm noise such as infrasound, tonality and amplitude modulation span the average human hearing threshold, so attribution to infrasound is problematic. This study used a combination of pre-recorded noise stimuli, measured at 3.2 km from a wind farm, in laboratory-based listening tests to investigate human perception of infrasound and amplitude modulation at realistic sound pressure levels in a group of 14 participants. Although a small sample size warrants cautious interpretation, preliminary results suggest differential effects between self- reported non-sensitive versus noise-sensitive participants, where the latter detected infrasound above chance. Infrasound did not affect the perception of amplitude modulation. Larger studies remain needed to clarify these findings. 1 INTRODUCTION Wind farm (WF) infrasound remains controversial and the source of substantial debate regarding potential effects of wind farm noise (WFN) on human health. The main infrasonic components of WFN can be measured many kilometres away from a wind farm, but typically at levels deemed well below the normal hearing threshold (Zajamšek et al. 2016, Turnbull, Turner, and Walsh 2012, Jakobsen 2005). The evidence for infrasound-specific effects on human health is very poor. A key hypothesis that has been advanced to explain wind farm noise related complaints, and partly supported by animal studies, suggesting that WF infrasound could potentially be detected by the ear, yet not heard, although supporting evidence from human studies remain lacking (Salt and Hullar 2010). -
A Guide to Office Acoustics
A GUIDE TO OFFICE ACOUSTICS www.acousticguide.org www.thefis.org Acoustic rafts, allowing the soffit to be exposed while reducing reverberation. First edition published April 2011 A GUIDE TO This edition published April 2015 OFFICE ACOUSTICS ISBN 978-0-9565341-1-8 World copyright reserved Copyright © 2015 FIS Published by FIS No part of this document may be reproduced or transmitted in any form or by any means electronic, chemical or mechanical, including photocopying, any information storage or retrieval system without licence or other permission in writing from the copyright owner. While every care has been taken to ensure the accuracy of the details presented in this document, we regret that FIS cannot be held responsible for any errors or omissions contained herein. 2 3 Artwork provides absorption to reduce reverberation. CONTENTS 1 Foreword . .. .. .. .. .7 . 5 Design guide to office acoustics . 19. 6 Terminology . 43 2 Introduction . .. .. .. .. .9 . Acoustic control. 19 7 Case studies . .. .. .. 51. Ceilings . .22 3 Basic acoustics . .. .. .. .. 11. Partitions. 24 8 Standards . .. .. .. 63. Doors. 30 4 Noise in offices . .. .. .. 15. Raised access flooring . .31 9 Acoustic research . .. .. .65 . Acoustic cavity barriers . .32 Noise sources . .15 Screens and furniture. 33 10 Acknowledgements . .. .. .71 . Mandatory requirements. 17 Floorcoverings. 33 The role of the acoustician. 17 Secondary glazing. 33 Internal finishes. 34 Design considerations. 34 Flanking sound. 34 Sibilance and grazing reflections. 35 Ventilation . .35 Integrating acoustic absorption into building services systems . .36 Sound rating and performance descriptors . .36 Reverberation control . .36 Intelligibilty. 36 Open plan environments . .37 Cellular environments . .39 Atria. 39 Background noise. 39 Proprietary introduced sound masking. -
Analysis of Reverberation Times and Energy Decay Curves of 1/12 Octave Bands in Performance Spaces Considering Musical Scale
Buenos Aires – 5 to 9 September, 2016 Acoustics for the 21st Century… PROCEEDINGS of the 22nd International Congress on Acoustics Concert Hall Acoustics: Paper ICA2016-676 Analysis of reverberation times and energy decay curves of 1/12 octave bands in performance spaces considering musical scale Akiho Matsuo(a), Toshiki Hanyu(b), Kazuma Hoshi(c) (a) Nihon University, Japan, [email protected] (b) Nihon University, Japan, [email protected] (c) Nihon University, Japan, hoshi@ arch.jcn.nihon-u.ac.jp Abstract Generally in the room acoustic design field, the reverberation times of 1 octave bands or 1/3 octave bands are analyzed for evaluating acoustic conditions in performance spaces such as concert halls. The center frequency in the octave bands is defined by engineering frequency intervals such as 250 Hz, 500 Hz, and 1000 Hz in the conventional analysis method. However, this definition of center frequency is not always adequate for evaluating performance spaces because music is composed of musical notes based on a musical scale, which is different from engineering frequency scales. Therefore, we studied the analysis of reverberation times and energy decay curves in 1/12 octave bands based on an equal tempered scale. Reverberation times in several concert halls were analyzed by this method. Distributions of reverberation times of 1/12 octave bands between concert halls were obtained. Next, instrumental sounds of varying pitches were convolved with impulse responses, and the reverberation times of the different pitches were analyzed from the convolved signals. As a result, variation of the reverberation times of the 1/12 octave bands and that of the different pitches corresponded well.