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Sound Sensor Experiment Guide
Sound Sensor Experiment Guide Sound Sensor Introduction: Part of the Eisco series of hand held sensors, the sound sensor allows students to record and graph data in experiments on the go. This sensor has two modes of operation. In slow mode it can be used to measure sound-pressure level in decibels. In fast mode it can display waveforms of different sound sources such as tuning forks and wind-chimes so that period and frequency can be determined. With two sound sensors, the velocity of propagation of sound in various media could be determined by timing a pulse travelling between them. The sound sensor is located in a plastic box accessible to the atmosphere via a hole in its side. Sensor Specs: Range: 0 - 110 dB | 0.1 dB resolution | 100 max sample rate Activity – Viewing Sound Waves with a Tuning Fork General Background: Sound waves when transmitted through gases, such as air, travel as longitudinal waves. Longitudinal waves are sometimes also called compression waves as they are waves of alternating compression and rarefaction of the intermediary travel medium. The sound is carried by regions of alternating pressure deviations from the equilibrium pressure. The range of frequencies that are audible by human ears is about 20 – 20,000 Hz. Sounds that have a single pitch have a repeating waveform of a single frequency. The tuning forks used in this activity have frequencies around 400 Hz, thus the period of the compression wave (the duration of one cycle of the wave) that carries the sound is about 2.5 seconds in duration, and has a wavelength of 66 cm. -
African Music Vol 6 No 2(Seb).Cdr
94 JOURNAL OF INTERNATIONAL LIBRARY OF AFRICAN MUSIC THE GORA AND THE GRAND’ GOM-GOM: by ERICA MUGGLESTONE 1 INTRODUCTION For three centuries the interest of travellers and scholars alike has been aroused by the gora, an unbraced mouth-resonated musical bow peculiar to South Africa, because it is organologically unusual in that it is a blown chordophone.2 A split quill is attached to the bowstring at one end of the instrument. The string is passed through a hole in one end of the quill and secured; the other end of the quill is then bound or pegged to the stave. The string is lashed to the other end of the stave so that it may be tightened or loosened at will. The player holds the quill lightly bet ween his parted lips, and, by inhaling and exhaling forcefully, causes the quill (and with it the string) to vibrate. Of all the early descriptions of the gora, that of Peter Kolb,3 a German astronom er who resided at the Cape of Good Hope from 1705 to 1713, has been the most contentious. Not only did his character and his publication in general come under attack, but also his account of Khoikhoi4 musical bows in particular. Kolb’s text indicates that two types of musical bow were observed, to both of which he applied the name gom-gom. The use of the same name for both types of bow and the order in which these are described in the text, seems to imply that the second type is a variant of the first. -
Lab 12. Vibrating Strings
Lab 12. Vibrating Strings Goals • To experimentally determine the relationships between the fundamental resonant frequency of a vibrating string and its length, its mass per unit length, and the tension in the string. • To introduce a useful graphical method for testing whether the quantities x and y are related by a “simple power function” of the form y = axn. If so, the constants a and n can be determined from the graph. • To experimentally determine the relationship between resonant frequencies and higher order “mode” numbers. • To develop one general relationship/equation that relates the resonant frequency of a string to the four parameters: length, mass per unit length, tension, and mode number. Introduction Vibrating strings are part of our common experience. Which as you may have learned by now means that you have built up explanations in your subconscious about how they work, and that those explanations are sometimes self-contradictory, and rarely entirely correct. Musical instruments from all around the world employ vibrating strings to make musical sounds. Anyone who plays such an instrument knows that changing the tension in the string changes the pitch, which in physics terms means changing the resonant frequency of vibration. Similarly, changing the thickness (and thus the mass) of the string also affects its sound (frequency). String length must also have some effect, since a bass violin is much bigger than a normal violin and sounds much different. The interplay between these factors is explored in this laboratory experi- ment. You do not need to know physics to understand how instruments work. In fact, in the course of this lab alone you will engage with material which entire PhDs in music theory have been written. -
The Science of String Instruments
The Science of String Instruments Thomas D. Rossing Editor The Science of String Instruments Editor Thomas D. Rossing Stanford University Center for Computer Research in Music and Acoustics (CCRMA) Stanford, CA 94302-8180, USA [email protected] ISBN 978-1-4419-7109-8 e-ISBN 978-1-4419-7110-4 DOI 10.1007/978-1-4419-7110-4 Springer New York Dordrecht Heidelberg London # Springer Science+Business Media, LLC 2010 All rights reserved. This work may not be translated or copied in whole or in part without the written permission of the publisher (Springer Science+Business Media, LLC, 233 Spring Street, New York, NY 10013, USA), except for brief excerpts in connection with reviews or scholarly analysis. Use in connection with any form of information storage and retrieval, electronic adaptation, computer software, or by similar or dissimilar methodology now known or hereafter developed is forbidden. The use in this publication of trade names, trademarks, service marks, and similar terms, even if they are not identified as such, is not to be taken as an expression of opinion as to whether or not they are subject to proprietary rights. Printed on acid-free paper Springer is part of Springer ScienceþBusiness Media (www.springer.com) Contents 1 Introduction............................................................... 1 Thomas D. Rossing 2 Plucked Strings ........................................................... 11 Thomas D. Rossing 3 Guitars and Lutes ........................................................ 19 Thomas D. Rossing and Graham Caldersmith 4 Portuguese Guitar ........................................................ 47 Octavio Inacio 5 Banjo ...................................................................... 59 James Rae 6 Mandolin Family Instruments........................................... 77 David J. Cohen and Thomas D. Rossing 7 Psalteries and Zithers .................................................... 99 Andres Peekna and Thomas D. -
A Framework for the Static and Dynamic Analysis of Interaction Graphs
A Framework for the Static and Dynamic Analysis of Interaction Graphs DISSERTATION Presented in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy in the Graduate School of The Ohio State University By Sitaram Asur, B.E., M.Sc. * * * * * The Ohio State University 2009 Dissertation Committee: Approved by Prof. Srinivasan Parthasarathy, Adviser Prof. Gagan Agrawal Adviser Prof. P. Sadayappan Graduate Program in Computer Science and Engineering c Copyright by Sitaram Asur 2009 ABSTRACT Data originating from many different real-world domains can be represented mean- ingfully as interaction networks. Examples abound, ranging from gene expression networks to social networks, and from the World Wide Web to protein-protein inter- action networks. The study of these complex networks can result in the discovery of meaningful patterns and can potentially afford insight into the structure, properties and behavior of these networks. Hence, there is a need to design suitable algorithms to extract or infer meaningful information from these networks. However, the challenges involved are daunting. First, most of these real-world networks have specific topological constraints that make the task of extracting useful patterns using traditional data mining techniques difficult. Additionally, these networks can be noisy (containing unreliable interac- tions), which makes the process of knowledge discovery difficult. Second, these net- works are usually dynamic in nature. Identifying the portions of the network that are changing, characterizing and modeling the evolution, and inferring or predict- ing future trends are critical challenges that need to be addressed in the context of understanding the evolutionary behavior of such networks. To address these challenges, we propose a framework of algorithms designed to detect, analyze and reason about the structure, behavior and evolution of real-world interaction networks. -
Fftuner Basic Instructions. (For Chrome Or Firefox, Not
FFTuner basic instructions. (for Chrome or Firefox, not IE) A) Overview B) Graphical User Interface elements defined C) Measuring inharmonicity of a string D) Demonstration of just and equal temperament scales E) Basic tuning sequence F) Tuning hardware and techniques G) Guitars H) Drums I) Disclaimer A) Overview Why FFTuner (piano)? There are many excellent piano-tuning applications available (both for free and for charge). This one is designed to also demonstrate a little music theory (and physics for the ‘engineer’ in all of us). It displays and helps interpret the full audio spectra produced when striking a piano key, including its harmonics. Since it does not lock in on the primary note struck (like many other tuners do), you can tune the interval between two keys by examining the spectral regions where their harmonics should overlap in frequency. You can also clearly see (and measure) the inharmonicity driving ‘stretch’ tuning (where the spacing of real-string harmonics is not constant, but increases with higher harmonics). The tuning sequence described here effectively incorporates your piano’s specific inharmonicity directly, key by key, (and makes it visually clear why choices have to be made). You can also use a (very) simple calculated stretch if desired. Other tuner apps have pre-defined stretch curves available (or record keys and then algorithmically calculate their own). Some are much more sophisticated indeed! B) Graphical User Interface elements defined A) Complete interface. Green: Fast Fourier Transform of microphone input (linear display in this case) Yellow: Left fundamental and harmonics (dotted lines) up to output frequency (dashed line). -
Acoustic Textiles - the Case of Wall Panels for Home Environment
Acoustic Textiles - The case of wall panels for home environment Bachelor Thesis Work Bachelor of Science in Engineering in Textile Technology Spring 2013 The Swedish school of Textiles, Borås, Sweden Report number: 2013.2.4 Written by: Louise Wintzell, Ti10, [email protected] Abstract Noise has become an increasing public health problem and has become serious environment pollution in our daily life. This indicates that it is in time to control and reduce noise from traffic and installations in homes and houses. Today a plethora of products are available for business, but none for the private market. The project describes a start up of development of a sound absorbing wall panel for the private market. It will examine whether it is possible to make a wall panel that can lower the sound pressure level with 3 dB, or reach 0.3 s in reverberation time, in a normally furnished bedroom and still follow the demands of price and environmental awareness. To start the project a limitation was made to use the textiles available per meter within the range of IKEA. The test were made according to applicable standards and calculation of reverberation time and sound pressure level using Sabine’s formula and a formula for sound pressure equals sound effect. During the project, tests were made whether it was possible to achieve a sound classification C on a A-E grade scale according to ISO 11654, where A is the best, with only textiles or if a classic sound absorbing mineral wool had to be used. To reach a sound classification C, a weighted sound absorption coefficient (αw) of 0.6 as a minimum must be reached. -
Fretted Instruments, Frets Are Metal Strips Inserted Into the Fingerboard
Fret A fret is a raised element on the neck of a stringed instrument. Frets usually extend across the full width of the neck. On most modern western fretted instruments, frets are metal strips inserted into the fingerboard. On some historical instruments and non-European instruments, frets are made of pieces of string tied around the neck. Frets divide the neck into fixed segments at intervals related to a musical framework. On instruments such as guitars, each fret represents one semitone in the standard western system, in which one octave is divided into twelve semitones. Fret is often used as a verb, meaning simply "to press down the string behind a fret". Fretting often refers to the frets and/or their system of placement. The neck of a guitar showing the nut (in the background, coloured white) Contents and first four metal frets Explanation Variations Semi-fretted instruments Fret intonation Fret wear Fret buzz Fret Repair See also References External links Explanation Pressing the string against the fret reduces the vibrating length of the string to that between the bridge and the next fret between the fretting finger and the bridge. This is damped if the string were stopped with the soft fingertip on a fretless fingerboard. Frets make it much easier for a player to achieve an acceptable standard of intonation, since the frets determine the positions for the correct notes. Furthermore, a fretted fingerboard makes it easier to play chords accurately. A disadvantage of frets is that they restrict pitches to the temperament defined by the fret positions. -
Mersenne and Mixed Mathematics
Mersenne and Mixed Mathematics Antoni Malet Daniele Cozzoli Pompeu Fabra University One of the most fascinating intellectual ªgures of the seventeenth century, Marin Mersenne (1588–1648) is well known for his relationships with many outstanding contemporary scholars as well as for his friendship with Descartes. Moreover, his own contributions to natural philosophy have an interest of their own. Mersenne worked on the main scientiªc questions debated in his time, such as the law of free fall, the principles of Galileo’s mechanics, the law of refraction, the propagation of light, the vacuum problem, the hydrostatic paradox, and the Copernican hypothesis. In his Traité de l’Harmonie Universelle (1627), Mersenne listed and de- scribed the mathematical disciplines: Geometry looks at continuous quantity, pure and deprived from matter and from everything which falls upon the senses; arithmetic contemplates discrete quantities, i.e. numbers; music concerns har- monic numbers, i.e. those numbers which are useful to the sound; cosmography contemplates the continuous quantity of the whole world; optics looks at it jointly with light rays; chronology talks about successive continuous quantity, i.e. past time; and mechanics concerns that quantity which is useful to machines, to the making of instruments and to anything that belongs to our works. Some also adds judiciary astrology. However, proofs of this discipline are The papers collected here were presented at the Workshop, “Mersenne and Mixed Mathe- matics,” we organized at the Universitat Pompeu Fabra (Barcelona), 26 May 2006. We are grateful to the Spanish Ministry of Education and the Catalan Department of Universities for their ªnancial support through projects Hum2005-05107/FISO and 2005SGR-00929. -
Tuning Forks As Time Travel Machines: Pitch Standardisation and Historicism for ”Sonic Things”: Special Issue of Sound Studies Fanny Gribenski
Tuning forks as time travel machines: Pitch standardisation and historicism For ”Sonic Things”: Special issue of Sound Studies Fanny Gribenski To cite this version: Fanny Gribenski. Tuning forks as time travel machines: Pitch standardisation and historicism For ”Sonic Things”: Special issue of Sound Studies. Sound Studies: An Interdisciplinary Journal, Taylor & Francis Online, 2020. hal-03005009 HAL Id: hal-03005009 https://hal.archives-ouvertes.fr/hal-03005009 Submitted on 13 Nov 2020 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Tuning forks as time travel machines: Pitch standardisation and historicism Fanny Gribenski CNRS / IRCAM, Paris For “Sonic Things”: Special issue of Sound Studies Biographical note: Fanny Gribenski is a Research Scholar at the Centre National de la Recherche Scientifique and IRCAM, in Paris. She studied musicology and history at the École Normale Supérieure of Lyon, the Paris Conservatory, and the École des hautes études en sciences sociales. She obtained her PhD in 2015 with a dissertation on the history of concert life in nineteenth-century French churches, which served as the basis for her first book, L’Église comme lieu de concert. Pratiques musicales et usages de l’espace (1830– 1905) (Arles: Actes Sud / Palazzetto Bru Zane, 2019). -
The Musical Kinetic Shape: a Variable Tension String Instrument
The Musical Kinetic Shape: AVariableTensionStringInstrument Ismet Handˇzi´c, Kyle B. Reed University of South Florida, Department of Mechanical Engineering, Tampa, Florida Abstract In this article we present a novel variable tension string instrument which relies on a kinetic shape to actively alter the tension of a fixed length taut string. We derived a mathematical model that relates the two-dimensional kinetic shape equation to the string’s physical and dynamic parameters. With this model we designed and constructed an automated instrument that is able to play frequencies within predicted and recognizable frequencies. This prototype instrument is also able to play programmed melodies. Keywords: musical instrument, variable tension, kinetic shape, string vibration 1. Introduction It is possible to vary the fundamental natural oscillation frequency of a taut and uniform string by either changing the string’s length, linear density, or tension. Most string musical instruments produce di↵erent tones by either altering string length (fretting) or playing preset and di↵erent string gages and string tensions. Although tension can be used to adjust the frequency of a string, it is typically only used in this way for fine tuning the preset tension needed to generate a specific note frequency. In this article, we present a novel string instrument concept that is able to continuously change the fundamental oscillation frequency of a plucked (or bowed) string by altering string tension in a controlled and predicted Email addresses: [email protected] (Ismet Handˇzi´c), [email protected] (Kyle B. Reed) URL: http://reedlab.eng.usf.edu/ () Preprint submitted to Applied Acoustics April 19, 2014 Figure 1: The musical kinetic shape variable tension string instrument prototype. -
Experiment 12
Experiment 12 Velocity and Propagation of Waves 12.1 Objective To use the phenomenon of resonance to determine the velocity of the propagation of waves in taut strings and wires. 12.2 Discussion Any medium under tension or stress has the following property: disturbances, motions of the matter of which the medium consists, are propagated through the medium. When the disturbances are periodic, they are called waves, and when the disturbances are simple harmonic, the waves are sinusoidal and are characterized by a common wavelength and frequency. The velocity of propagation of a disturbance, whether or not it is periodic, depends generally upon the tension or stress in the medium and on the density of the medium. The greater the stress: the greater the velocity; and the greater the density: the smaller the velocity. In the case of a taut string or wire, the velocity v depends upon the tension T in the string or wire and the mass per unit length µ of the string or wire. Theory predicts that the relation should be T v2 = (12.1) µ Most disturbances travel so rapidly that a direct determination of their velocity is not possible. However, when the disturbance is simple harmonic, the sinusoidal character of the waves provides a simple method by which the velocity of the waves can be indirectly determined. This determination involves the frequency f and wavelength λ of the wave. Here f is the frequency of the simple harmonic motion of the medium and λ is from any point of the wave to the next point of the same phase.