THE SPECIAL RELATIONSHIP BETWEEN SOUND and LIGHT, with IMPLICATIONS for SOUND and LIGHT THERAPY John Stuart Reid ABSTRACT
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Acoustic Resonance Lab 1 Introduction 2 Sound Generation
Summer Music Technology 2013 Acoustic Resonance Lab 1 Introduction This activity introduces several concepts that are fundamental to understanding how sound is produced in musical instruments. We'll be measuring audio produced from acoustic tubes. General Notes • Work in groups of 2 or 3 • Divide up the tasks amongst your group members so everyone contributes Equipment Check Make sure you have the following: • (2) iPads • (1) Microphone • (1) Tape Measure • (1) Adjustable PVC tube with speaker • (1) Amplifier • (1) RCA to 1/8" audio cable • (1) iRig Pre-Amp • (2) Pieces of speaker wire • (1) XLR cable • (1) Pair of Alligator clips 2 Sound Generation Setup We will use one iPad to generate tones that will play through our tube. However, the iPad can't provide enough power to drive the speaker, so we need to connect it to an amplifier. From here on, we'll refer to this iPad as the Synthesizer. 1. Plug the Amplifier’s power cord into an outlet. DO NOT TURN IT ON. 2. Plug one end of the 1/8" audio cable to the iPad's headphone output jack. Plug the other end into the Amplifier’s Input jack. 3. Attach the alligator clips to the speaker wires on the Amplifier’s Output jack. Attach the other end of the clips to the speaker terminals (the speaker should be mounted to the tube). MET-lab 1 Drexel University Summer Music Technology 2013 3 Sound Analysis Setup In order to measure the audio, we need to record audio from a microphone. The other iPad will be used to record sound. -
Ultrasound Induced Cavitation and Resonance Amplification Using Adaptive Feedback Control System
Master's Thesis Electrical Engineering Ultrasound induced cavitation and resonance amplification using adaptive feedback Control System Vipul. Vijigiri Taraka Rama Krishna Pamidi This thesis is presented as part of Degree of Master of Science in Electrical Engineering with Emphasis on Signal Processing Blekinge Institute of Technology (BTH) September 2014 Blekinge Institute of Technology, Sweden School of Engineering Department of Electrical Engineering (AET) Supervisor: Dr. Torbjörn Löfqvist, PhD, LTU Co- Supervisor: Dr. Örjan Johansson, PhD, LTU Shadow Supervisor/Examiner: Dr. Sven Johansson, PhD, BTH Ultrasound induced cavitation and resonance amplification using adaptive feedback Control System Master`s thesis Vipul, Taraka, 2014 Performed in Electrical Engineering, EISlab, Dep’t of Computer Science, Electrical and Space Engineering, Acoustics Lab, dep’t of Acoustics at Lulea University of Technology ii | Page This thesis is submitted to the Department of Applied signal processing at Blekinge Institute of Technology in partial fulfilment of the requirements for the degree of Master of Science in Electrical Engineering with emphasis on Signal Processing. Contact Information: Authors: Vipul Vijigiri Taraka Rama Krishna Pamidi Dept. of Applied signal processing Blekinge Institute of Technology (BTH), Sweden E-mail: [email protected],[email protected] E-mail: [email protected], [email protected] External Advisors: Dr. Torbjörn Löfqvist Department of Computer Science, Electrical and Space Engineering Internet: www.ltu.se Luleå University of technology (LTU), Sweden Phone: +46 (0)920-491777 E-mail: [email protected] Co-Advisor: Dr. Örjan Johansson Internet: www.ltu.se Department of the built environment and natural resources- Phone: +46 (0)920-491386 -Operation, maintenance and acoustics Luleå University of technology (LTU), Sweden E-mail: [email protected] University Advisor/Examiner: Dr. -
Nuclear Acoustic Resonance Investigations of the Longitudinal and Transverse Electron-Lattice Interaction in Transition Metals and Alloys V
NUCLEAR ACOUSTIC RESONANCE INVESTIGATIONS OF THE LONGITUDINAL AND TRANSVERSE ELECTRON-LATTICE INTERACTION IN TRANSITION METALS AND ALLOYS V. Müller, G. Schanz, E.-J. Unterhorst, D. Maurer To cite this version: V. Müller, G. Schanz, E.-J. Unterhorst, D. Maurer. NUCLEAR ACOUSTIC RESONANCE INVES- TIGATIONS OF THE LONGITUDINAL AND TRANSVERSE ELECTRON-LATTICE INTERAC- TION IN TRANSITION METALS AND ALLOYS. Journal de Physique Colloques, 1981, 42 (C6), pp.C6-389-C6-391. 10.1051/jphyscol:19816113. jpa-00221175 HAL Id: jpa-00221175 https://hal.archives-ouvertes.fr/jpa-00221175 Submitted on 1 Jan 1981 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. JOURNAL DE PHYSIQUE CoZZoque C6, suppZe'ment au no 22, Tome 42, de'cembre 1981 page C6-389 NUCLEAR ACOUSTIC RESONANCE INVESTIGATIONS OF THE LONGITUDINAL AND TRANSVERSE ELECTRON-LATTICE INTERACTION IN TRANSITION METALS AND ALLOYS V. Miiller, G. Schanz, E.-J. Unterhorst and D. Maurer &eie Universit8G Berlin, Fachbereich Physik, Kiinigin-Luise-Str.28-30, 0-1000 Berlin 33, Gemany Abstract.- In metals the conduction electrons contribute significantly to the acoustic-wave-induced electric-field-gradient-tensor (DEFG) at the nuclear positions. Since nuclear electric quadrupole coupling to the DEFG is sensi- tive to acoustic shear modes only, nuclear acoustic resonance (NAR) is a par- ticularly useful tool in studying the coup1 ing of electrons to shear modes without being affected by volume dilatations. -
Acoustics & Ultrasonics
Dr.R.Vasuki Associate professor & Head Department of Physics Thiagarajar College of Engineering Madurai-625015 Science of sound that deals with origin, propagation and auditory sensation of sound. Sound production Propagation by human beings/machines Reception Classification of Sound waves Infrasonic audible ultrasonic Inaudible Inaudible < 20 Hz 20 Hz to 20,000 Hz ˃20,000 Hz Music – The sound which produces rhythmic sensation on the ears Noise-The sound which produces jarring & unpleasant effect To differentiate sound & noise Regularity of vibration Degree of damping Ability of ear to recognize the components Sound is a form of energy Sound is produced by the vibration of the body Sound requires a material medium for its propagation. When sound is conveyed from one medium to another medium there is no bodily motion of the medium Sound can be transmitted through solids, liquids and gases. Velocity of sound is higher in solids and lower in gases. Sound travels with velocity less than the velocity 8 of light. c= 3x 10 V0 =330 m/s at 0° degree Lightning comes first than thunder VT= V0+0.6 T Sound may be reflected, refracted or scattered. It undergoes diffraction and interference. Pitch or frequency Quality or timbre Intensity or Loudness Pitch is defined as the no of vibrations/sec. Frequency is a physical quantity but pitch is a physiological quantity. Mosquito- high pitch Lion- low pitch Quality or timbre is the one which helps to distinguish between the musical notes emitted by the different instruments or voices even though they have the same pitch. Intensity or loudness It is the average rate of flow of acoustic energy (Q) per unit area(A) situated normally to the direction of propagation of sound waves. -
Contribution of the Conditioning Stage to the Total Harmonic Distortion in the Parametric Array Loudspeaker
Universidad EAFIT Contribution of the conditioning stage to the Total Harmonic Distortion in the Parametric Array Loudspeaker Andrés Yarce Botero Thesis to apply for the title of Master of Science in Applied Physics Advisor Olga Lucia Quintero. Ph.D. Master of Science in Applied Physics Science school Universidad EAFIT Medellín - Colombia 2017 1 Contents 1 Problem Statement 7 1.1 On sound artistic installations . 8 1.2 Objectives . 12 1.2.1 General Objective . 12 1.2.2 Specific Objectives . 12 1.3 Theoretical background . 13 1.3.1 Physics behind the Parametric Array Loudspeaker . 13 1.3.2 Maths behind of Parametric Array Loudspeakers . 19 1.3.3 About piezoelectric ultrasound transducers . 21 1.3.4 About the health and safety uses of the Parametric Array Loudspeaker Technology . 24 2 Acquisition of Sound from self-demodulation of Ultrasound 26 2.1 Acoustics . 26 2.1.1 Directionality of Sound . 28 2.2 On the non linearity of sound . 30 2.3 On the linearity of sound from ultrasound . 33 3 Signal distortion and modulation schemes 38 3.1 Introduction . 38 3.2 On Total Harmonic Distortion . 40 3.3 Effects on total harmonic distortion: Modulation techniques . 42 3.4 On Pulse Wave Modulation . 46 4 Loudspeaker Modelling by statistical design of experiments. 49 4.1 Characterization Parametric Array Loudspeaker . 51 4.2 Experimental setup . 52 4.2.1 Results of PAL radiation pattern . 53 4.3 Design of experiments . 56 4.3.1 Placket Burmann method . 59 4.3.2 Box Behnken methodology . 62 5 Digital filtering techniques and signal distortion analysis. -
Musical Acoustics - Wikipedia, the Free Encyclopedia 11/07/13 17:28 Musical Acoustics from Wikipedia, the Free Encyclopedia
Musical acoustics - Wikipedia, the free encyclopedia 11/07/13 17:28 Musical acoustics From Wikipedia, the free encyclopedia Musical acoustics or music acoustics is the branch of acoustics concerned with researching and describing the physics of music – how sounds employed as music work. Examples of areas of study are the function of musical instruments, the human voice (the physics of speech and singing), computer analysis of melody, and in the clinical use of music in music therapy. Contents 1 Methods and fields of study 2 Physical aspects 3 Subjective aspects 4 Pitch ranges of musical instruments 5 Harmonics, partials, and overtones 6 Harmonics and non-linearities 7 Harmony 8 Scales 9 See also 10 External links Methods and fields of study Frequency range of music Frequency analysis Computer analysis of musical structure Synthesis of musical sounds Music cognition, based on physics (also known as psychoacoustics) Physical aspects Whenever two different pitches are played at the same time, their sound waves interact with each other – the highs and lows in the air pressure reinforce each other to produce a different sound wave. As a result, any given sound wave which is more complicated than a sine wave can be modelled by many different sine waves of the appropriate frequencies and amplitudes (a frequency spectrum). In humans the hearing apparatus (composed of the ears and brain) can usually isolate these tones and hear them distinctly. When two or more tones are played at once, a variation of air pressure at the ear "contains" the pitches of each, and the ear and/or brain isolate and decode them into distinct tones. -
Large Scale Sound Installation Design: Psychoacoustic Stimulation
LARGE SCALE SOUND INSTALLATION DESIGN: PSYCHOACOUSTIC STIMULATION An Interactive Qualifying Project Report submitted to the Faculty of the WORCESTER POLYTECHNIC INSTITUTE in partial fulfillment of the requirements for the Degree of Bachelor of Science by Taylor H. Andrews, CS 2012 Mark E. Hayden, ECE 2012 Date: 16 December 2010 Professor Frederick W. Bianchi, Advisor Abstract The brain performs a vast amount of processing to translate the raw frequency content of incoming acoustic stimuli into the perceptual equivalent. Psychoacoustic processing can result in pitches and beats being “heard” that do not physically exist in the medium. These psychoac- oustic effects were researched and then applied in a large scale sound design. The constructed installations and acoustic stimuli were designed specifically to combat sensory atrophy by exer- cising and reinforcing the listeners’ perceptual skills. i Table of Contents Abstract ............................................................................................................................................ i Table of Contents ............................................................................................................................ ii Table of Figures ............................................................................................................................. iii Table of Tables .............................................................................................................................. iv Chapter 1: Introduction ................................................................................................................. -
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. -
Acoustic Resonance Between Ground and Thermosphere
Data Science Journal, Volume 8, 30 March 2009 ACOUSTIC RESONANCE BETWEEN GROUND AND THERMOSPHERE 1 1 2 3 1 1 4 Matsumura, M., * Iyemori, T., Tanaka, Y., Han, D., Nose, M., Utsugi, M., Oshiman, N., 5 1 6 Shinagawa, H., Odagi, Y. and Tabata, Y. *1 Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan E-mail: [email protected] 2 Faculty of Engineering, Setsunan University, Neyagawa 572-8508, Japan 3 Polar Research Institute of China, Pudong, Jinqiao Road 451, Shanghai 200136, China 4 Disaster Prevention Research Institute, Kyoto University, Uji 611-0011, Japan 5 National Institute of Information and Communications Technology, Koganei 184-8795, Japan 6Research Institute for Sustainable Humanosphere, Kyoto University, Uji 611-0011, Japan ABSTRACT Ultra-low frequency acoustic waves called "acoustic gravity waves" or "infrasounds" are theoretically expected to resonate between the ground and the thermosphere. This resonance is a very important phenomenon causing the coupling of the solid Earth, neutral atmosphere, and ionospheric plasma. This acoustic resonance, however, has not been confirmed by direct observations. In this study, atmospheric perturbations on the ground and ionospheric disturbances were observed and compared with each other to confirm the existence of resonance. Atmospheric perturbations were observed with a barometer, and ionospheric disturbances were observed using the HF Doppler method. An end point of resonance is in the ionosphere, where conductivity is high and the dynamo effect occurs. Thus, geomagnetic observation is also useful, so the geomagnetic data were compared with other data. Power spectral density was calculated and averaged for each month. Peaks appeared at the theoretically expected resonance frequencies in the pressure and HF Doppler data. -
Physics and Medicine: a Historical Perspective
Series Physics and Medicine 1 Physics and medicine: a historical perspective Stephen F Keevil Nowadays, the term medical physics usually refers to the work of physicists employed in hospitals, who are concerned Lancet 2011; 379: 1517–24 mainly with medical applications of radiation, diagnostic imaging, and clinical measurement. This involvement in Published Online clinical work began barely 100 years ago, but the relation between physics and medicine has a much longer history. In April 18, 2012 this report, I have traced this history from the earliest recorded period, when physical agents such as heat and light DOI:10.1016/S0140- 6736(11)60282-1 began to be used to diagnose and treat disease. Later, great polymaths such as Leonardo da Vinci and Alhazen used See Comment pages 1463 physical principles to begin the quest to understand the function of the body. After the scientifi c revolution in the and 1464 17th century, early medical physicists developed a purely mechanistic approach to physiology, whereas others applied This is the fi rst in a Series of ideas derived from physics in an eff ort to comprehend the nature of life itself. These early investigations led directly fi ve papers about physics to the development of specialties such as electrophysiology, biomechanics, and ophthalmology. Physics-based medical and medicine technology developed rapidly during the 19th century, but it was the revolutionary discoveries about radiation and Department of Medical radioactivity at the end of the century that ushered in a new era of radiation-based medical diagnosis and treatment, Physics, Guy’s and St Thomas’ thereby giving rise to the modern medical physics profession. -
Chapter 12: Physics of Ultrasound
Chapter 12: Physics of Ultrasound Slide set of 54 slides based on the Chapter authored by J.C. Lacefield of the IAEA publication (ISBN 978-92-0-131010-1): Diagnostic Radiology Physics: A Handbook for Teachers and Students Objective: To familiarize students with Physics or Ultrasound, commonly used in diagnostic imaging modality. Slide set prepared by E.Okuno (S. Paulo, Brazil, Institute of Physics of S. Paulo University) IAEA International Atomic Energy Agency Chapter 12. TABLE OF CONTENTS 12.1. Introduction 12.2. Ultrasonic Plane Waves 12.3. Ultrasonic Properties of Biological Tissue 12.4. Ultrasonic Transduction 12.5. Doppler Physics 12.6. Biological Effects of Ultrasound IAEA Diagnostic Radiology Physics: a Handbook for Teachers and Students – chapter 12,2 12.1. INTRODUCTION • Ultrasound is the most commonly used diagnostic imaging modality, accounting for approximately 25% of all imaging examinations performed worldwide nowadays • Ultrasound is an acoustic wave with frequencies greater than the maximum frequency audible to humans, which is 20 kHz IAEA Diagnostic Radiology Physics: a Handbook for Teachers and Students – chapter 12,3 12.1. INTRODUCTION • Diagnostic imaging is generally performed using ultrasound in the frequency range from 2 to 15 MHz • The choice of frequency is dictated by a trade-off between spatial resolution and penetration depth, since higher frequency waves can be focused more tightly but are attenuated more rapidly by tissue The information in an ultrasonic image is influenced by the physical processes underlying propagation, reflection and attenuation of ultrasound waves in tissue IAEA Diagnostic Radiology Physics: a Handbook for Teachers and Students – chapter 12,4 12.1. -
On the Behaviour of Living Cells Under the Influence of Ultrasound
fluids Review On the Behaviour of Living Cells under the Influence of Ultrasound David M. Rubin, Nicole Anderton, Charl Smalberger, Jethro Polliack, Malavika Nathan and Michiel Postema * School of Electrical and Information Engineering, University of the Witwatersrand, Johannesburg, 1 Jan Smuts Laan, 2050 Braamfontein, South Africa; [email protected] (D.M.R.); [email protected] (N.A.); [email protected] (C.S.); [email protected] (J.P.); [email protected] (M.N.) * Correspondence: [email protected]; Tel.: +27-11-7177237 Received: 19 September 2018; Accepted: 22 October 2018; Published: 26 October 2018 Abstract: Medical ultrasound technology is available, affordable, and non-invasive. It is used to detect, quantify, and heat tissue structures. This review article gives a concise overview of the types of behaviour that biological cells experience under the influence of ultrasound only, i.e., without the presence of microbubbles. The phenomena are discussed from a physics and engineering perspective. They include proliferation, translation, apoptosis, lysis, transient membrane permeation, and oscillation. The ultimate goal of cellular acoustics is the detection, quantification, manipulation and eradication of individual cells. Keywords: cellular acoustics; ultrasound-induced lysis; acoustic microparticle manipulation; ultrasound-induced cell translation; micro-acoustics; non-bubble-assisted sonoporation 1. Introduction Ultrasound technology is available, affordable and non-invasive. Therefore, it finds widespread application in medicine. Ultrasound is well established as an imaging modality in medical diagnostics, and, more recently, its use has been extended to therapy. Ultrasonic therapeutic modalities in current clinical practice are high-intensity focussed ultrasound (HIFU) [1], extracorporeal shockwave lithotrypsy [2], ultrasound contrast agent-assisted drug delivery [3], and combinations of some of these modalities [4].