An Introduction to Acoustics

Total Page:16

File Type:pdf, Size:1020Kb

An Introduction to Acoustics An Introduction to Acoustics S.W. Rienstra & A. Hirschberg Eindhoven University of Technology 2 Oct 2021 This is an extended and revised edition of IWDE 92-06. Comments and corrections are gratefully accepted. This file may be used and printed, but for personal or educational purposes only. © S.W. Rienstra & A. Hirschberg 2004. Contents Page Preface 1 Some fluid dynamics 1 1.1 Conservation laws and constitutive equations ..................... 1 1.2 Approximations and alternative forms of the conservation laws for ideal fluids ..... 4 2 Wave equation, speed of sound, and acoustic energy 9 2.1 Order of magnitude estimates ............................. 9 2.2 Wave equation for a uniform stagnant fluid and compactness ............. 13 2.2.1 Linearization and wave equation ........................ 13 2.2.2 Simple solutions ................................. 14 2.2.3 Compactness .................................. 16 2.3 Speed of sound ..................................... 17 2.3.1 Ideal gas ..................................... 17 2.3.2 Water ...................................... 19 2.3.3 Bubbly liquid at low frequencies ........................ 19 2.4 Influence of temperature gradient ........................... 20 2.5 Influence of mean flow ................................. 22 2.6 Sources of sound .................................... 22 2.6.1 Inverse problem and uniqueness of sources ................... 22 2.6.2 Mass and momentum injection ......................... 23 2.6.3 Lighthill’s analogy ............................... 24 2.6.4 Vortex sound .................................. 27 2.7 Acoustic energy .................................... 29 2.7.1 Introduction ................................... 29 2.7.2 Kirchhoff’s equation for quiescent fluids .................... 30 2.7.3 Acoustic energy in a non-uniform flow ..................... 33 2.7.4 Acoustic energy and vortex sound ........................ 35 ii Contents 3 Green’s functions, impedance, and evanescent waves 38 3.1 Green’s functions .................................... 38 3.1.1 Integral representations ............................. 38 3.1.2 Remarks on finding Green’s functions ...................... 41 3.2 Acoustic impedance .................................. 41 3.2.1 Impedance and acoustic energy ......................... 43 3.2.2 Impedance and reflection coefficient ...................... 43 3.2.3 Impedance and causality ............................ 44 3.2.4 Impedance and surface waves .......................... 47 3.2.5 Acoustic boundary condition in the presence of mean flow ........... 48 3.2.6 Surface waves along an impedance wall with mean flow ............ 50 3.2.7 Instability, ill-posedness, and a regularization .................. 52 3.3 Evanescent waves and related behaviour ........................ 54 3.3.1 An important complex square root ....................... 54 3.3.2 The Walkman .................................. 55 3.3.3 Ill-posed inverse problem ............................ 56 3.3.4 Typical plate pitch ................................ 56 3.3.5 Snell’s law ................................... 56 3.3.6 Silent vorticity ................................. 59 4 One dimensional acoustics 62 4.1 Plane waves ...................................... 62 4.2 Basic equations and method of characteristics ..................... 64 4.2.1 The wave equation ............................... 64 4.2.2 Characteristics .................................. 65 4.2.3 Linear behaviour ................................ 66 4.2.4 Non-linear simple waves and shock waves ................... 70 4.3 Source terms ...................................... 72 4.4 Reflection at discontinuities and abrupt changes .................... 76 4.4.1 Jump in characteristic impedance ρc ...................... 76 4.4.2 Smooth change in pipe cross section ...................... 79 4.4.3 Orifice and high amplitude behaviour ...................... 79 4.4.4 Multiple junction ................................ 83 4.4.5 Reflection at a small air bubble in a pipe .................... 84 4.5 Attenuation of an acoustic wave by thermal and viscous dissipation .......... 88 4.5.1 Reflection of a plane wave at a rigid wall .................... 88 4.5.2 Viscous laminar boundary layer ........................ 92 Contents iii 4.5.3 Damping in ducts with isothermal walls. .................... 93 4.6 One dimensional Green’s function ........................... 95 4.6.1 Infinite uniform tube .............................. 95 4.6.2 Finite uniform tube ............................... 96 4.7 Aero-acoustical applications .............................. 97 4.7.1 Sound produced by turbulence ......................... 97 4.7.2 An isolated bubble in a turbulent pipe flow ................... 100 4.7.3 Reflection of a wave at a temperature inhomogeneity .............. 101 5 Resonators and self-sustained oscillations 107 5.1 Self-sustained oscillations, shear layers and jets .................... 107 5.2 Some resonators .................................... 113 5.2.1 Introduction .................................. 113 5.2.2 Resonance in duct segment ........................... 114 5.2.3 The Helmholtz resonator (quiescent fluid) ................... 121 5.2.4 Non-linear losses in a Helmholtz resonator ................... 123 5.2.5 The Helmholtz resonator in the presence of a mean flow ............ 124 5.3 Green’s function of a finite duct ............................ 125 5.4 Self-sustained oscillations of a clarinet ......................... 128 5.4.1 Introduction .................................. 128 5.4.2 Linear stability analysis ............................. 128 5.4.3 Rayleigh’s Criterion ............................... 130 5.4.4 Time domain simulation ............................ 130 5.5 Some thermo-acoustics ................................. 132 5.5.1 Introduction .................................. 132 5.5.2 Modulated heat transfer by acoustic flow and Rijke tube ............ 134 5.6 Flow induced oscillations of a Helmholtz resonator .................. 138 6 Spherical waves 147 6.1 Introduction ...................................... 147 6.2 Pulsating and translating sphere ............................ 147 6.3 Multipole expansion and far field approximation .................... 153 6.4 Method of images and influence of walls on radiation ................. 158 6.5 Lighthill’s theory of jet noise .............................. 161 6.6 Sound radiation by compact bodies in free space .................... 164 6.6.1 Introduction .................................. 164 6.6.2 Tailored Green’s function ............................ 165 6.6.3 Curle’s method ................................. 166 6.7 Sound radiation from an open pipe termination .................... 169 iv Contents 7 Duct acoustics 176 7.1 General formulation .................................. 176 7.2 Cylindrical ducts .................................... 178 7.3 Rectangular ducts .................................... 182 7.4 Impedance wall .................................... 183 7.4.1 Behaviour of complex modes .......................... 183 7.4.2 Attenuation ................................... 186 7.5 Annular hard-walled duct modes in uniform mean flow ................. 188 7.6 Behaviour of soft-wall modes and mean flow ...................... 192 7.7 Source expansion .................................... 194 7.7.1 Modal amplitudes ................................ 194 7.7.2 Rotating fan ................................... 194 7.7.3 Tyler and Sofrin rule for rotor-stator interaction ................. 195 7.7.4 Point source in a lined flow duct ......................... 197 7.7.5 Point source in a duct wall ........................... 200 7.7.6 Vibrating duct wall ............................... 202 7.8 Reflection and transmission .............................. 203 7.8.1 A discontinuity in diameter ........................... 203 7.8.2 The iris problem ................................. 207 7.8.3 The edge condition ............................... 209 7.9 Reflection at an unflanged open end .......................... 211 8 Approximation methods 216 8.1 Webster’s horn equation ................................ 217 8.2 Multiple scales ..................................... 220 8.3 Helmholtz resonator with non-linear dissipation .................... 224 8.4 Slowly varying ducts .................................. 229 8.5 Reflection at an isolated turning point ......................... 232 8.6 Ray acoustics in temperature gradient ......................... 236 8.7 Refraction in shear flow ................................ 241 8.8 Matched asymptotic expansions ............................ 242 8.9 Duct junction ...................................... 249 8.10 Co-rotating line-vortices ................................ 254 Contents v 9 Effects of flow and motion 259 9.1 Uniform mean flow, plane waves and edge diffraction ................. 259 9.1.1 Lorentz or Prandtl-Glauert transformation ................... 259 9.1.2 Plane waves ................................... 260 9.1.3 Half-plane diffraction problem ......................... 261 9.2 Moving point source and Doppler shift ......................... 263 9.3 Rotating monopole and dipole with moving observer ................. 265 9.4 Ffowcs Williams & Hawkings equation for moving bodies ............... 268 Appendix 273 A Integral laws and related results 273 A.1 Reynolds’ transport theorem .............................. 273 A.2 Conservation laws ................................... 273 A.3 Normal vectors of level surfaces ............................ 275 A.4 Vector identities and theorems
Recommended publications
  • The Green-Function Transform and Wave Propagation
    1 The Green-function transform and wave propagation Colin J. R. Sheppard,1 S. S. Kou2 and J. Lin2 1Department of Nanophysics, Istituto Italiano di Tecnologia, Genova 16163, Italy 2School of Physics, University of Melbourne, Victoria 3010, Australia *Corresponding author: [email protected] PACS: 0230Nw, 4120Jb, 4225Bs, 4225Fx, 4230Kq, 4320Bi Abstract: Fourier methods well known in signal processing are applied to three- dimensional wave propagation problems. The Fourier transform of the Green function, when written explicitly in terms of a real-valued spatial frequency, consists of homogeneous and inhomogeneous components. Both parts are necessary to result in a pure out-going wave that satisfies causality. The homogeneous component consists only of propagating waves, but the inhomogeneous component contains both evanescent and propagating terms. Thus we make a distinction between inhomogenous waves and evanescent waves. The evanescent component is completely contained in the region of the inhomogeneous component outside the k-space sphere. Further, propagating waves in the Weyl expansion contain both homogeneous and inhomogeneous components. The connection between the Whittaker and Weyl expansions is discussed. A list of relevant spherically symmetric Fourier transforms is given. 2 1. Introduction In an impressive recent paper, Schmalz et al. presented a rigorous derivation of the general Green function of the Helmholtz equation based on three-dimensional (3D) Fourier transformation, and then found a unique solution for the case of a source (Schmalz, Schmalz et al. 2010). Their approach is based on the use of generalized functions and the causal nature of the out-going Green function. Actually, the basic principle of their method was described many years ago by Dirac (Dirac 1981), but has not been widely adopted.
    [Show full text]
  • Approximate Separability of Green's Function for High Frequency
    APPROXIMATE SEPARABILITY OF GREEN'S FUNCTION FOR HIGH FREQUENCY HELMHOLTZ EQUATIONS BJORN¨ ENGQUIST AND HONGKAI ZHAO Abstract. Approximate separable representations of Green's functions for differential operators is a basic and an important aspect in the analysis of differential equations and in the development of efficient numerical algorithms for solving them. Being able to approx- imate a Green's function as a sum with few separable terms is equivalent to the existence of low rank approximation of corresponding discretized system. This property can be explored for matrix compression and efficient numerical algorithms. Green's functions for coercive elliptic differential operators in divergence form have been shown to be highly separable and low rank approximation for their discretized systems has been utilized to develop efficient numerical algorithms. The case of Helmholtz equation in the high fre- quency limit is more challenging both mathematically and numerically. In this work, we develop a new approach to study approximate separability for the Green's function of Helmholtz equation in the high frequency limit based on an explicit characterization of the relation between two Green's functions and a tight dimension estimate for the best linear subspace approximating a set of almost orthogonal vectors. We derive both lower bounds and upper bounds and show their sharpness for cases that are commonly used in practice. 1. Introduction Given a linear differential operator, denoted by L, the Green's function, denoted by G(x; y), is defined as the fundamental solution in a domain Ω ⊆ Rn to the partial differ- ential equation 8 n < LxG(x; y) = δ(x − y); x; y 2 Ω ⊆ R (1) : with boundary condition or condition at infinity; where δ(x − y) is the Dirac delta function denoting an impulse source point at y.
    [Show full text]
  • The David Crighton Lecture Professor Frank Kelly CBE FRS Thursday 12 May 2016 at 6.15 P.M
    The David Crighton Lecture Professor Frank Kelly CBE FRS Thursday 12 May 2016 at 6.15 p.m. followed by a reception at The Royal Society, Carlton House Terrace, London, SW1Y 5AG Registration will open at 5.45 p.m. Mathematics and Financial Markets Abstract: A substantial proportion of mathematics graduates, at both first degree and doctoral level, enter the financial services sector. This is hardly surprising given the importance of the sector to the economy, and the role of mathematical modelling in the valuation of instruments and the assessment of risk. What is striking is that, with some notable exceptions, few mathematicians have been actively engaged in the design of financial markets. This is undoubtedly a serious challenge with parallels from other large-scale complex networks: to design a distributed system, linking self-interested and intelligent agents, so that the outcome is effective and efficient. How would an ideal market operate, to allow liquidity between long-term investors to be provided by short- term traders? In the second part of the talk I outline some preliminary work, joint with Elena Yudovina, on this question. I describe a simplified and analytically tractable model of a limit order book where the dynamics are driven by stochastic fluctuations between supply and demand. The model has a natural interpretation for a highly traded market on short time scales where there is a separation between the time scale of trading, represented in the model, and a longer time scale on which fundamentals change. There has been considerable discussion recently of the effects of competition between multiple high- frequency traders, and of proposals aimed to slow down markets.
    [Show full text]
  • The Standing Acoustic Wave Principle Within the Frequency Analysis Of
    inee Eng ring al & ic d M e e d Misun, J Biomed Eng Med Devic 2016, 1:3 m i o c i a B l D f o e v DOI: 10.4172/2475-7586.1000116 l i a c n e r s u o Journal of Biomedical Engineering and Medical Devices J ISSN: 2475-7586 Review Article Open Access The Standing Acoustic Wave Principle within the Frequency Analysis of Acoustic Signals in the Cochlea Vojtech Misun* Department of Solid Mechanics, Mechatronics and Biomechanics, Brno University of Technology, Brno, Czech Republic Abstract The organ of hearing is responsible for the correct frequency analysis of auditory perceptions coming from the outer environment. The article deals with the principles of the analysis of auditory perceptions in the cochlea only, i.e., from the overall signal leaving the oval window to its decomposition realized by the basilar membrane. The paper presents two different methods with the function of the cochlea considered as a frequency analyzer of perceived acoustic signals. First, there is an analysis of the principle that cochlear function involves acoustic waves travelling along the basilar membrane; this concept is one that prevails in the contemporary specialist literature. Then, a new principle with the working name “the principle of standing acoustic waves in the common cavity of the scala vestibuli and scala tympani” is presented and defined in depth. According to this principle, individual structural modes of the basilar membrane are excited by continuous standing waves of acoustic pressure in the scale tympani. Keywords: Cochlea function; Acoustic signals; Frequency analysis; The following is a description of the theories in question: Travelling wave principle; Standing wave principle 1.
    [Show full text]
  • 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.
    [Show full text]
  • A Comparison Study of Normal-Incidence Acoustic Impedance Measurements of a Perforate Liner
    A Comparison Study of Normal-Incidence Acoustic Impedance Measurements of a Perforate Liner Todd Schultz1 The Mathworks, Inc, Natick, MA 01760 Fei Liu,2 Louis Cattafesta, Mark Sheplak3 University of Florida, Gainesville, FL 32611 and Michael Jones4 NASA Langley Research Center, Hampton, VA 23681 The eduction of the acoustic impedance for liner configurations is fundamental to the reduction of noise from modern jet engines. Ultimately, this property must be measured accurately for use in analytical and numerical propagation models of aircraft engine noise. Thus any standardized measurement techniques must be validated by providing reliable and consistent results for different facilities and sample sizes. This paper compares normal- incidence acoustic impedance measurements using the two-microphone method of ten nominally identical individual liner samples from two facilities, namely 50.8 mm and 25.4 mm square waveguides at NASA Langley Research Center and the University of Florida, respectively. The liner chosen for this investigation is a simple single-degree-of-freedom perforate liner with resonance and anti-resonance frequencies near 1.1 kHz and 2.2 kHz, respectively. The results show that the ten measurements have the most variation around the anti-resonance frequency, where statistically significant differences exist between the averaged results from the two facilities. However, the sample-to-sample variation is comparable in magnitude to the predicted cross-sectional area-dependent cavity dissipation differences between facilities, providing evidence that the size of the present samples does not significantly influence the results away from anti-resonance. I. Introduction ODERN turbofan engines rely on acoustic liners to suppress engine noise and meet community noise Mstandards.
    [Show full text]
  • 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.
    [Show full text]
  • Psychoacoustics Perception of Normal and Impaired Hearing with Audiology Applications Editor-In-Chief for Audiology Brad A
    PSYCHOACOUSTICS Perception of Normal and Impaired Hearing with Audiology Applications Editor-in-Chief for Audiology Brad A. Stach, PhD PSYCHOACOUSTICS Perception of Normal and Impaired Hearing with Audiology Applications Jennifer J. Lentz, PhD 5521 Ruffin Road San Diego, CA 92123 e-mail: [email protected] Website: http://www.pluralpublishing.com Copyright © 2020 by Plural Publishing, Inc. Typeset in 11/13 Adobe Garamond by Flanagan’s Publishing Services, Inc. Printed in the United States of America by McNaughton & Gunn, Inc. All rights, including that of translation, reserved. No part of this publication may be reproduced, stored in a retrieval system, or transmitted in any form or by any means, electronic, mechanical, recording, or otherwise, including photocopying, recording, taping, Web distribution, or information storage and retrieval systems without the prior written consent of the publisher. For permission to use material from this text, contact us by Telephone: (866) 758-7251 Fax: (888) 758-7255 e-mail: [email protected] Every attempt has been made to contact the copyright holders for material originally printed in another source. If any have been inadvertently overlooked, the publishers will gladly make the necessary arrangements at the first opportunity. Library of Congress Cataloging-in-Publication Data Names: Lentz, Jennifer J., author. Title: Psychoacoustics : perception of normal and impaired hearing with audiology applications / Jennifer J. Lentz. Description: San Diego, CA : Plural Publishing,
    [Show full text]
  • Appendix a Short Course in Taylor Series
    Appendix A Short Course in Taylor Series The Taylor series is mainly used for approximating functions when one can identify a small parameter. Expansion techniques are useful for many applications in physics, sometimes in unexpected ways. A.1 Taylor Series Expansions and Approximations In mathematics, the Taylor series is a representation of a function as an infinite sum of terms calculated from the values of its derivatives at a single point. It is named after the English mathematician Brook Taylor. If the series is centered at zero, the series is also called a Maclaurin series, named after the Scottish mathematician Colin Maclaurin. It is common practice to use a finite number of terms of the series to approximate a function. The Taylor series may be regarded as the limit of the Taylor polynomials. A.2 Definition A Taylor series is a series expansion of a function about a point. A one-dimensional Taylor series is an expansion of a real function f(x) about a point x ¼ a is given by; f 00ðÞa f 3ðÞa fxðÞ¼faðÞþf 0ðÞa ðÞþx À a ðÞx À a 2 þ ðÞx À a 3 þÁÁÁ 2! 3! f ðÞn ðÞa þ ðÞx À a n þÁÁÁ ðA:1Þ n! © Springer International Publishing Switzerland 2016 415 B. Zohuri, Directed Energy Weapons, DOI 10.1007/978-3-319-31289-7 416 Appendix A: Short Course in Taylor Series If a ¼ 0, the expansion is known as a Maclaurin Series. Equation A.1 can be written in the more compact sigma notation as follows: X1 f ðÞn ðÞa ðÞx À a n ðA:2Þ n! n¼0 where n ! is mathematical notation for factorial n and f(n)(a) denotes the n th derivation of function f evaluated at the point a.
    [Show full text]
  • Physics of Ultrasound TI Precision Labs – Ultrasonic Sensing
    Physics of Ultrasound TI Precision Labs – Ultrasonic Sensing Presented by Akeem Whitehead Prepared by Akeem Whitehead Definition of Ultrasound Sound Frequency Spectrum Ultrasound is defined as: • sound waves with a frequency above the upper limit of human hearing at -destructive testing EarthquakeVolcano Human hearing Animal hearingAutomotiveWater park level assist sensingLiquid IdentificationMedical diagnosticsNon Acoustic microscopy 20kHz. • having physical properties that are 0 20 200 2k 20k 200k 2M 20M 200M identical to audible sound. • a frequency some animals use for Infrasound Audible Ultrasound navigation and echo location. This content will focus on ultrasonic systems that use transducers operating between 20kHz up to several GHz. >20kHz 2 Acoustics of Ultrasound When ultrasound is a stimulus: When ultrasound is a sensation: Generates and Emits Ultrasound Wave Detects and Responds to Ultrasound Wave 3 Sound Propagation Ultrasound propagates as: • longitudinal waves in air, water, plasma Particles at Rest • transverse waves in solids The transducer’s vibrating diaphragm is the source of the ultrasonic wave. As the source vibrates, the vibrations propagate away at the speed of sound to Longitudinal Wave form a measureable ultrasonic wave. Direction of Particle Motion Direction of The particles of the medium only transport the vibration is Parallel Wave Propagation of the ultrasonic wave, but do not travel with the wave. The medium can cause waves to be reflected, refracted, or attenuated over time. Transverse Wave An ultrasonic wave cannot travel through a vacuum. Direction of Particle Motion λ is Perpendicular 4 Acoustic Properties 100 90 Ultrasonic propagation is affected by: 80 1. Relationship between density, pressure, and temperature 70 to determine the speed of sound.
    [Show full text]
  • Call Numbers
    Call numbers: It is our recommendation that libraries NOT put J, +, E, Ref, etc. in the call number field in front of the Dewey or other call number. Use the Home Location field to indicate the collection for the item. It is difficult if not impossible to sort lists if the call number fields aren’t entered systematically. Dewey Call Numbers for Non-Fiction Each library follows its own practice for how long a Dewey number they use and what letters are used for the author’s name. Some libraries use a number (Cutter number from a table) after the letters for the author’s name. Other just use letters for the author’s name. Call Numbers for Fiction For fiction, the call number is usually the author’s Last Name, First Name. (Use a comma between last and first name.) It is usually already in the call number field when you barcode. Call Numbers for Paperbacks Each library follows its own practice. Just be consistent for easier handling of the weeding lists. WCTS libraries should follow the format used by WCTS for the items processed by them for your library. Most call numbers are either the author’s name or just the first letters of the author’s last name. Please DO catalog your paperbacks so they can be shared with other libraries. Call Numbers for Magazines To get the call numbers to display in the correct order by date, the call number needs to begin with the date of the issue in a number format, followed by the issue in alphanumeric format.
    [Show full text]
  • Minorities and Women in Television See Little Change, While Minorities Fare Worse in Radio
    RunningRunning inin PlacePlace Minorities and women in television see little change, while minorities fare worse in radio. By Bob Papper he latest figures from the RTNDA/Ball State Uni- Minority Population vs. Minority Broadcast Workforce versity Annual Survey show lit- 2005 2004 2000 1995 1990 tle change for minorities in tel- evision news in the past year but Minority Population in U.S. 33.2% 32.8% 30.9% 27.9% 25.9% slippage in radio news. Minority TV Workforce 21.2 21.8 21.0 17.1 17.8 TIn television, the overall minority Minority Radio Workforce 7.9 11.8 10.0 14.7 10.8 workforce remained largely un- Source for U.S. numbers: U.S. Census Bureau changed at 21.2 percent, compared with last year’s 21.8 percent. At non-Hispanic stations, the the stringent Equal Employment minority workforce in TV news is up minority workforce also remained Opportunity rules were eliminated in 3.4 percent. At the same time, the largely steady at 19.5 percent, com- 1998. minority population in the U.S. has pared with 19.8 percent a year ago. News director numbers were increased 7.3 percent. Overall, the After a jump in last year’s minority mixed, with the percentage of minor- minority workforce in TV has been at radio numbers, the percentage fell this ity TV news directors down slightly to 20 percent—plus or minus 3 per- year.The minority radio news work- 12 percent (from 12.5 percent last cent—for every year in the past 15.
    [Show full text]