Glossary of Ultrasound Terminology*

Total Page:16

File Type:pdf, Size:1020Kb

Glossary of Ultrasound Terminology* Glossary of Ultrasound Terminology* A Mode (Amplitude-mode): A method of echo signal display in which time is represented along the horizontal axis and echo amplitude is displayed along the vertical axis. AB Mode (Amplitude brightness-mode): A method of data presenta­ tion on the oscilloscope screen in which one coordinate represents time (depth) and the amplitude of the echo signal is displayed as both a deflection along the other coordinate and as a brightening of the display spot. Absolute Maximum (from AIUM/NEMA Standard): This means the largest possible value of a specified quantity either for an individual instrument or for all instruments of a given generic type. This value shall include effects of inaccuracies and imprecision of the measure­ ment process(es) used to determine it. Absolute Minimum (from AIUM/NEMA Standard): This means the smallest possible value of a specified quantity either for an individual instrument or for all instruments of a given generic type. This value shall include effects of inaccuracies and imprecision of the measure­ ment process(es) used to determine it. Absorbed Dose: The thermal energy imparted to matter by absorption of acoustic radiation per unit mass (or per unit volume) of irradiated material at the site of interest. Absorption: The process by which acoustic radiation imparts energy locally to the medium through which it propagates, by conversion of acoustic energy to heat. Absorption contributes to attenuation. Acoustic, Acoustical: The qualifying adjectives "acoustic" and "acous­ tical" mean containing, producing, arising from, actuated by, related to, or associated with sound. Acoustic (note 1) is used when the term being qualified designates something that has the properties, dimen­ sions, or physical characteristics associated with sound waves; acous­ tical (note 2) is used when the term being qualified does not desig- *Selected terms taken from AlUM Recommended Nomenclature [Reflections 6 0),3219801 with permission. Definitions modified from this reference are markedt. 305 306 GLOSSARY nate explicitly something that has such properties, dimensions, or physical characteristics. Note 1: The following examples qualify as having the properties or physical characteristics associated with sound waves and hence would take acoustic: impedance, output (sound power), energy wave, medium, signal, transducer. Note 2: The following examples do not have the requisite physical characteristics and therefore take acoustical: method, engineer, symbol, problem, measurement. Note 3: As illustrated in the preceding notes, usually the generic term is modified by acoustical, whereas the specific technical impli­ cation calls for acoustic. Acoustic Attenuation*: Amplitude reduction of the acoustic signal as a function of time or of propagation distance. Attenuation includes the effects of absorption, scattering, reflection, refraction, and diffraction. Acoustic Energy: Mechanical energy transported by an acoustic wave. The units are those of acoustic power times time, the joule (J) (Watt­ second) in standard international units. Acoustic Field: A distribution (in space and time) of acoustic energy. Acoustic Holography: See Holography. Acoustic Impedance: A vector quantity formed by taking the ratio of the instantaneous acoustic pressure at a surface to the instantaneous volume velocity at the surface in an acoustic field. (See also specific acoustic impedance, characteristic acoustic impedance). Acoustic Impedance Match (Colloquial): The condition of equality of Characteristic Acoustic Impedances of contiguous media, avoiding reflection of acoustic energy at the interface (see Impedance Ratio). *In this (and other similar definitions in this section), the adjective "acoustic" may be deleted when the acoustic context of the term is understood; or it may be replaced by the equivalent term "sonic" or, when appropriate, the more specific adjective "ultrasonic." These terms, which refer to the sound pressure amplitude, can also be defined in terms of intensity. The choice would be based upon the measurement technique. For example, a hydrophone probe will yield data in terms of sound pressure amplitude, and a thermocouple probe will give data in terms of intensity. The magnitude of this attenuation (or attenuation coefficient) depends upon many characteristics of the measurement system, such as the size and orientation of the transducer or transmitting and receiving transducer element, the orientation of the tissues, and electrical signal processing. The acoustic attenuation of tissue or other material in an ultrasound beam is the ratio of the signal received by the transducer relative to the signal that is received when the tissue or other material in the propagation pathway is replaced by a specified lossless medium (water, at a given temperature). GLOSSARY 307 Acoustic Impedance Mismatch: A condition of unequal Characteris­ tic Acoustic Impedances of contiguous media, causing reflection of acoustic energy at the interface (see Impedance Ratio). Acoustic Intensity: See Intensity. Acoustic Lens: A refractive element employed to redirect acoustic waves or rays in order to increase or decrease acoustic energy den­ sity in a prescribed volume or to modify phase coherence at a receiving transducer. Acoustic Power: Acoustic energy transported per unit time (usually a temporal average is quoted; e.g. I J/s) (See Average Acoustic Power). Acoustic Pressure: The instantaneous value of the total pressure mi­ nus the ambient pressure. Acoustics: Acoustics is the science of sound, including its production, transmission, and effects. Acoustic Shadow: A manifestation of reduced acoustic signal ampli­ tude in or returning from regions lying beyond an attenuating ob­ ject. It is important to distinguish between acoustic shadows and re­ gions of low reflectivity. Acoustic Streamingt: An acoustically generated time-independent transport of fluid within the body of the sonicated fluid or tissue. Acoustic Wave: A mechanical disturbance that progagates through a continuous medium. Acoustic Waveform: See Waveform. Acoustic Wavefront: The surface of equal phase in a propagating wave. Acoustic Wavelength: The acoustic wavelength is the distance between any two adjacent points at which the phase, at the same instant, dif­ fers by 21T; it corresponds to the distance traveled by the wave during one cycle; A = clf, where A is the wavelength, c is the speed of sound, and f is the frequency. For water or tissue at I MHz, the wavelength is approximately 1.5 mm. Amplitude: The magnitude of the envelope of a first-order electrical or acoustic waveform (e.g., voltage or acoustic pressure in linear acoustics. ) Amplitude Modulation Factor: The value of the expression 100 X (IAI - IBI) I IAI, expressed as a percentage, where IAI and IBI are the absolute maximum and minimum amplitudes of the envelope of a modulated acoustical or electrical carrier (first-order quantity), respectively. Amplitude Modulated Waveform: A waveform in which the carrier wave is modified in amplitude by a signal wave as a means of trans­ mitting information. For measurement purposes the AIUM-NEMA 308 GLOSSARY standard defines it as a waveform in which the amplitude modula­ tion factor is greater than 5%. Angle of Incidence: The angle between the axis of an ultrasound beam encountering an interface and the vector normal (perpendicular) to the interface. Attenuation: See Acoustic Attenuation. Attenuation Coefficient: The relative change in the acoustic wave am­ plitude (acoustic attenuation) per unit path length in a medium. Commonly employed units are dB/cm, and Np/cm where Np = Neper. Attenuator: A device that reduces the signal by a specified amount, e.g., 10 dB steps. Average Acoustic Power: The power output from an acoustic trans­ ducer averaged over a period of time that is either long com pared to, or exactly to, the period of pulses or variations in power. Average Intensity: See Intensity. Axial Resolution: The minimum separation of reflectors, required along the direction of sound travel, such that each can be separately distinguished on the display (same as Depth Resolution, Longitudi­ nal Resolution, and Range Resolution). Azimuthal Resolution: The minimum angular separation between ad­ jacent reflectors at the same range such that each can be separately distinguished in the display. This resolution is limited by the beamwidth of the transducer at that range of the targets (see Lateral Resolution). B-Mode (Brightness-Mode): A method of display on an oscilloscope screen in which the intensity of the echo is represented by modula­ tion of the brightness of the spot and in which the position of the echo, displayed in the x-y plane, is determined from the position of the transducer and the transit time of the acoustic pulse. B-Scan: A misnomer for a B-mode scan or image; scanning with B-mode display. Backscattered Energy: The portion of the incident acoustic energy re­ flected from a small (compared to the wavelength) target back to­ ward the reflector source; to be distinguished from specular reflec­ tion, where the reflector dimension may be large compared to the wavelength. Bandwidth: The transmitted bandwidth is the difference in the fre­ quencies, Fr and F2, at which the magnitude in the acoustic pressure spectrum is 71% (-3 dB) of its maximum value. The pulse-echo bandwidth is the difference in frequencies, Fr and F2, at which the magnitude of the pulse-echo response from a planar reflector at a specified range is 50% (-6 dB) of its maximum value.
Recommended publications
  • Glossary Physics (I-Introduction)
    1 Glossary Physics (I-introduction) - Efficiency: The percent of the work put into a machine that is converted into useful work output; = work done / energy used [-]. = eta In machines: The work output of any machine cannot exceed the work input (<=100%); in an ideal machine, where no energy is transformed into heat: work(input) = work(output), =100%. Energy: The property of a system that enables it to do work. Conservation o. E.: Energy cannot be created or destroyed; it may be transformed from one form into another, but the total amount of energy never changes. Equilibrium: The state of an object when not acted upon by a net force or net torque; an object in equilibrium may be at rest or moving at uniform velocity - not accelerating. Mechanical E.: The state of an object or system of objects for which any impressed forces cancels to zero and no acceleration occurs. Dynamic E.: Object is moving without experiencing acceleration. Static E.: Object is at rest.F Force: The influence that can cause an object to be accelerated or retarded; is always in the direction of the net force, hence a vector quantity; the four elementary forces are: Electromagnetic F.: Is an attraction or repulsion G, gravit. const.6.672E-11[Nm2/kg2] between electric charges: d, distance [m] 2 2 2 2 F = 1/(40) (q1q2/d ) [(CC/m )(Nm /C )] = [N] m,M, mass [kg] Gravitational F.: Is a mutual attraction between all masses: q, charge [As] [C] 2 2 2 2 F = GmM/d [Nm /kg kg 1/m ] = [N] 0, dielectric constant Strong F.: (nuclear force) Acts within the nuclei of atoms: 8.854E-12 [C2/Nm2] [F/m] 2 2 2 2 2 F = 1/(40) (e /d ) [(CC/m )(Nm /C )] = [N] , 3.14 [-] Weak F.: Manifests itself in special reactions among elementary e, 1.60210 E-19 [As] [C] particles, such as the reaction that occur in radioactive decay.
    [Show full text]
  • Acoustical Engineering
    National Aeronautics and Space Administration Engineering is Out of This World! Acoustical Engineering NASA is developing a new rocket called the Space Launch System, or SLS. The SLS will be able to carry astronauts and materials, known as payloads. Acoustical engineers are helping to build the SLS. Sound is a vibration. A vibration is a rapid motion of an object back and forth. Hold a piece of paper up right in front of your lips. Talk or sing into the paper. What do you feel? What do you think is causing the vibration? If too much noise, or acoustical loading, is ! caused by air passing over the SLS rocket, the vehicle could be damaged by the vibration! NAME: (Continued from front) Typical Sound Levels in Decibels (dB) Experiment with the paper. 130 — Jet takeoff Does talking louder or softer change the vibration? 120 — Pain threshold 110 — Car horn 100 — Motorcycle Is the vibration affected by the pitch of your voice? (Hint: Pitch is how deep or 90 — Power lawn mower ! high the sound is.) 80 — Vacuum cleaner 70 — Street traffic —Working area on ISS (65 db) Change the angle of the paper. What 60 — Normal conversation happens? 50 — Rain 40 — Library noise Why do you think NASA hires acoustical 30 — Purring cat engineers? (Hint: Think about how loud 20 — Rustling leaves rockets are!) 10 — Breathing 0 — Hearing Threshold How do you think the noise on an airplane compares to the noise on a rocket? Hearing protection is recommended at ! 85 decibels. NASA is currently researching ways to reduce the noise made by airplanes.
    [Show full text]
  • A GUIDE to USING FETS for SENSOR APPLICATIONS by Ron Quan
    Three Decades of Quality Through Innovation A GUIDE TO USING FETS FOR SENSOR APPLICATIONS By Ron Quan Linear Integrated Systems • 4042 Clipper Court • Fremont, CA 94538 • Tel: 510 490-9160 • Fax: 510 353-0261 • Email: [email protected] A GUIDE TO USING FETS FOR SENSOR APPLICATIONS many discrete FETs have input capacitances of less than 5 pF. Also, there are few low noise FET input op amps Linear Systems that have equivalent input noise voltages density of less provides a variety of FETs (Field Effect Transistors) than 4 nV/ 퐻푧. However, there are a number of suitable for use in low noise amplifier applications for discrete FETs rated at ≤ 2 nV/ 퐻푧 in terms of equivalent photo diodes, accelerometers, transducers, and other Input noise voltage density. types of sensors. For those op amps that are rated as low noise, normally In particular, low noise JFETs exhibit low input gate the input stages use bipolar transistors that generate currents that are desirable when working with high much greater noise currents at the input terminals than impedance devices at the input or with high value FETs. These noise currents flowing into high impedances feedback resistors (e.g., ≥1MΩ). Operational amplifiers form added (random) noise voltages that are often (op amps) with bipolar transistor input stages have much greater than the equivalent input noise. much higher input noise currents than FETs. One advantage of using discrete FETs is that an op amp In general, many op amps have a combination of higher that is not rated as low noise in terms of input current noise and input capacitance when compared to some can be converted into an amplifier with low input discrete FETs.
    [Show full text]
  • Standing Waves and Sound
    Standing Waves and Sound Waves are vibrations (jiggles) that move through a material Frequency: how often a piece of material in the wave moves back and forth. Waves can be longitudinal (back-and- forth motion) or transverse (up-and- down motion). When a wave is caught in between walls, it will bounce back and forth to create a standing wave, but only if its frequency is just right! Sound is a longitudinal wave that moves through air and other materials. In a sound wave the molecules jiggle back and forth, getting closer together and further apart. Work with a partner! Take turns being the “wall” (hold end steady) and the slinky mover. Making Waves with a Slinky 1. Each of you should hold one end of the slinky. Stand far enough apart that the slinky is stretched. 2. Try making a transverse wave pulse by having one partner move a slinky end up and down while the other holds their end fixed. What happens to the wave pulse when it reaches the fixed end of the slinky? Does it return upside down or the same way up? Try moving the end up and down faster: Does the wave pulse get narrower or wider? Does the wave pulse reach the other partner noticeably faster? 3. Without moving further apart, pull the slinky tighter, so it is more stretched (scrunch up some of the slinky in your hand). Make a transverse wave pulse again. Does the wave pulse reach the end faster or slower if the slinky is more stretched? 4. Try making a longitudinal wave pulse by folding some of the slinky into your hand and then letting go.
    [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]
  • Transducers and Sensors
    3/7/2017 TRANSDUCERS AND SENSORS Dr. Ibrahim Al-Naimi Closed‐loop Control System 1 3/7/2017 CHAPTER ONE Introduction Functional Elements of a Measurement System • Basic Functional Elements 1‐Transducer Element 2‐ Signal Conditioning Element 3‐ Data Presentation Element • Auxiliary Functional Elements A‐ Calibration Element B‐ External Power supply 2 3/7/2017 Functional Elements of a Measurement System Transducer and Signal Conditioning 3 3/7/2017 Transducer Element • The Transducer is defined as a device, which when actuated by one form of energy, is capable of converting it to another form of energy. The transduction may be from mechanical, electrical, or optical to any other related form. • The term transducer is used to describe any item which changes information from one form to another. Transducer Element • The Transducer element normally senses the desired input in one physical form and convert it to an output in another physical form. For example, the input variable to the transducer could be pressure, acceleration, or temperature and the output of transducer may be disp lacemen t, voltage, or resitistance change depending on the type of transducer element. 4 3/7/2017 Transducer Element • Single stage • Double stage Single Stage Transducer 5 3/7/2017 Double Stage Transducer Typical Examples of Transducer Elements 6 3/7/2017 Typical Examples of Transducer Elements Typical Examples of Transducer Elements 7 3/7/2017 Transducers classification • Based on power type classification ‐ Active transducer (Diaphragms, Bourdon Tubes, tachometers, piezoelectric, etc…) ‐ Passive transducer (Capacitive, inductive, photo, LVDT, etc…) Transducers classification • Based on the type of output signal ‐ Analogue Transducers (stain gauges, LVDT, etc…) ‐ Digital Transducers (Absolute and incremental encoders) 8 3/7/2017 Transducers classification • Based on the electrical phenomenon or parameter tha t may be chdhanged due to the whole process.
    [Show full text]
  • M204; the Doppler Effect
    MISN-0-204 THE DOPPLER EFFECT by Mary Lu Larsen THE DOPPLER EFFECT Towson State University 1. Introduction a. The E®ect . .1 b. Questions to be Answered . 1 2. The Doppler E®ect for Sound a. Wave Source and Receiver Both Stationary . 2 Source Ear b. Wave Source Approaching Stationary Receiver . .2 Stationary c. Receiver Approaching Stationary Source . 4 d. Source and Receiver Approaching Each Other . 5 e. Relative Linear Motion: Three Cases . 6 f. Moving Source Not Equivalent to Moving Receiver . 6 g. The Medium is the Preferred Reference Frame . 7 Moving Ear Away 3. The Doppler E®ect for Light a. Introduction . .7 b. Doppler Broadening of Spectral Lines . 7 c. Receding Galaxies Emit Doppler Shifted Light . 8 4. Limitations of the Results . 9 Moving Ear Toward Acknowledgments. .9 Glossary . 9 Project PHYSNET·Physics Bldg.·Michigan State University·East Lansing, MI 1 2 ID Sheet: MISN-0-204 THIS IS A DEVELOPMENTAL-STAGE PUBLICATION Title: The Doppler E®ect OF PROJECT PHYSNET Author: Mary Lu Larsen, Dept. of Physics, Towson State University The goal of our project is to assist a network of educators and scientists in Version: 4/17/2002 Evaluation: Stage 0 transferring physics from one person to another. We support manuscript processing and distribution, along with communication and information Length: 1 hr; 24 pages systems. We also work with employers to identify basic scienti¯c skills Input Skills: as well as physics topics that are needed in science and technology. A number of our publications are aimed at assisting users in acquiring such 1.
    [Show full text]
  • Transducers in Audio ● Transducer: Any Mechanism That Transforms One Form of Energy Into Another Form of Energy
    Transducers in Audio ● Transducer: Any mechanism that transforms one form of energy into another form of energy. ○ Physical energy into mechanical energy ○ Physical energy into electrical energy ○ Mechanical energy into electrical energy ○ Vice versa Audio is primarily concerned with turning physical acoustic energy into electrical energy and back again. What are our two most basic audio transducers? scienceaid.net https://socratic.org/questions/what-part-of-the-ear-contains-the-sensory-receptors-for-hearing From Acoustic to Electric Energy First...a short trip into basic electrical theory... Michael Faraday http://www.rigb.org/our-history/michael-faraday Electro-magnetism Faraday’s Law of Induction: Basically, any change in the magnetic field of a coil of wire will cause a voltage to be induced in a wire. Conversely, any change in the voltage on a coil of wire will cause the magnetic field to change. This is called electromagnetism, and the field created is called an electro-magnetic field. Capacitance When two conductors are given an opposite charge, an electric or more specifically a capacitive field is generated around them. When the relationship between the two conductors (for example the distance between them) changes it causes measurable effects on the charges. http://hyperphysics.phy-astr.gsu.edu/hbase/electric/imgele/cap.png Capacitance When two conductors are given an opposite charge, a electric or more specifically a capacitive field is generated around them. When the relationship between the two conductors, for example the distance between them, changes is causes measurable effects on the charges. http://hyperphysics.phy-astr.gsu.edu/hbase/electric/imgele/cap.png ● Alternating Current (AC) vs Direct Current (DC) ○ AC charge changes from positive to negative across the zero axis.
    [Show full text]
  • AIUM Practice Parameter for the Performance of an Ultrasound Examination of the Abdomen And/Or Retroperitoneum
    1 AIUM Practice Parameter for the Performance of an Ultrasound Examination of the Abdomen and/or Retroperitoneum Parameter developed in conjunction with the American College of Radiology (ACR), the Society for Pediatric Radiology (SPR), and the Society of Radiologists in Ultrasound (SRU). The American Institute of Ultrasound in Medicine (AIUM) is a multidisciplinary association dedicated to advancing the safe and effective use of ultrasound in medicine through professional and public education, research, development of parameters, and accreditation. To promote this mission, the AIUM is pleased to publish, in conjunction with the American College of Radiology (ACR), the Society for Pediatric Radiology (SPR), and the Society of Radiologists in Ultrasound (SRU), this AIUM Practice Parameter for the Performance of an Ultrasound Examination of the Abdomen and/or Retroperitoneum. We are indebted to the many volunteers who contributed their time, knowledge, and energy to bringing this document to completion. The AIUM represents the entire range of clinical and basic science interests in medical diagnostic ultrasound, and, with hundreds of volunteers, the AIUM has promoted the safe and effective use of ultrasound in clinical medicine for more than 65 years. This document and others like it will continue to advance this mission. © 2017 American Institute of Ultrasound in Medicine 14750 Sweitzer Ln, Suite 100 Laurel, MD 20707-5906 USA www.aium.org 2 Practice parameters of the AIUM are intended to provide the medical ultrasound community with parameters for the performance and recording of high-quality ultrasound examinations. The parameters reflect what the AIUM considers the minimum criteria for a complete examination in each area but are not intended to establish a legal standard of care.
    [Show full text]
  • Training in Diagnostic Ultrasound: Essentials, Principles and Standards
    This report contains the collective views of on international group of experts and does not necessarily represent the decisions or the stated policy offe World Health Organization TRAINING IN DIAGNOSTIC ULTRASOUND: ESSENTIALS, PRINCIPLES AND STANDARDS Report of a WHO Study Group Geneva 1998 WHO L~braryCataloguing In Publ~catlonData Training in diagnostic ultrasound : essentials, principles and standards : report of a WHO study group (WHO technical report series ; 875) 1 .Ultrasonography 2.Diagnostic imag~ng- standards 3.Guidelines 4.Health per- sonnel - education I Title II.Series (NLM Classification: WN 200) The World Health Organization welcomes requests for permission to reproduce or translate its publications, in part or in full Applications and enquiries should be addressed to the Office of Publications, World Health Organization, Geneva, Switzerland, which will be glad to prov~dethe latest information on any changes made to the text, plans for new editions, and reprlnts and translations already available. O World Health Organization 1998 Publications of the World Health Organization enjoy copyright protect~onin accordance with the provisions of Protocol 2 of the Universal Copyright Convention. All rights reserved. The designations employed and the presentation of the material in this publication do not imply the expression of any opnlon whatsoever on the part of the Secretariat of the World Health Organization concerning the legal status of any country, territory, city or area or of its authorities, or concerning the delimitation of its frontiers or boundaries. The mention of specific companies or of certain manufacturers' products does not imply that they are endorsed or recommended by the World Health Organ~zat~onin preference to others of a simllar nature that are not mentioned.
    [Show full text]
  • Recent Advances in the Sound Insulation Properties of Bio-Based Materials
    PEER-REVIEWED REVIEW ARTICLE bioresources.com Recent Advances in the Sound Insulation Properties of Bio-based Materials Xiaodong Zhu,a,b Birm-June Kim,c Qingwen Wang,a and Qinglin Wu b,* Many bio-based materials, which have lower environmental impact than traditional synthetic materials, show good sound absorbing and sound insulation performances. This review highlights progress in sound transmission properties of bio-based materials and provides a comprehensive account of various multiporous bio-based materials and multilayered structures used in sound absorption and insulation products. Furthermore, principal models of sound transmission are discussed in order to aid in an understanding of sound transmission properties of bio-based materials. In addition, the review presents discussions on the composite structure optimization and future research in using co-extruded wood plastic composite for sound insulation control. This review contributes to the body of knowledge on the sound transmission properties of bio-based materials, provides a better understanding of the models of some multiporous bio-based materials and multilayered structures, and contributes to the wider adoption of bio-based materials as sound absorbers. Keywords: Bio-based material; Acoustic properties; Sound transmission; Transmission loss; Sound absorbing; Sound insulation Contact information: a: Key Laboratory of Bio-based Material Science and Technology (Ministry of Education), Northeast Forestry University, Harbin 150040, China; b: School of Renewable Natural Resources, LSU AgCenter, Baton Rouge, Louisiana; c: Department of Forest Products and Biotechnology, Kookmin University, Seoul 136-702, Korea. * Corresponding author: [email protected] (Qinglin Wu) INTRODUCTION Noise reduction is a must, as noise has negative effects on physiological processes and human psychological health.
    [Show full text]
  • Determining the Motion of Galaxies Using Doppler Redshift
    Determining the Motion of Galaxies Using Doppler Redshift Caitlin M. Matyas The Arts Academy at Benjamin Rush Overview Rationale Objective Strategies Classroom Activities Annotated Bibliography / Resources Standards Appendices Overview The Doppler effect of sound is a method used to determine the relative speeds of an object emitting a sound and an observer. Depending on whether the source and/or observer are moving towards or away from each other, the frequency of the wave will change. This in turn creates a change in pitch perceived by the observer. The relative speeds can easily be calculated using the following formula: � ± �′ = �( ), � ± where f’ represents the shifted frequency, f represents the frequency of the source, v is the speed of sound, vo is the speed of the observer, and vs is the speed of the source. Vo is added if moving towards and subtracted if moving away from the source. vs is added if moving away and subtracted if moving towards the observer. The figures below help to demonstrate the perceived change in frequency. The source is located at the center of the smallest circle. The picture shows waves expanding as they move outwards away from the source, so the earliest emitted waves create the biggest circles. If both the source and observer were stationary, the waves appear to pass at equal periods of time, as seen in figure IA. However, if the source is moving, the frequency appears to change. Figure IB shows what would happen if the source moves towards the right. Although the waves are emitted at a constant frequency, they seem closer together on the right side and farther spaced on the left.
    [Show full text]