10 Engineering Noise Control
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EN 300 676 V1.2.1 (1999-12) European Standard (Telecommunications Series)
Draft ETSI EN 300 676 V1.2.1 (1999-12) European Standard (Telecommunications series) Electromagnetic compatibility and Radio spectrum Matters (ERM); Ground-based VHF hand-held, mobile and fixed radio transmitters, receivers and transceivers for the VHF aeronautical mobile service using amplitude modulation; Technical characteristics and methods of measurement 2 Draft ETSI EN 300 676 V1.2.1 (1999-12) Reference REN/ERM-RP05-014 Keywords Aeronautical, AM, DSB, radio, testing, VHF ETSI Postal address F-06921 Sophia Antipolis Cedex - FRANCE Office address 650 Route des Lucioles - Sophia Antipolis Valbonne - FRANCE Tel.:+33492944200 Fax:+33493654716 Siret N° 348 623 562 00017 - NAF 742 C Association à but non lucratif enregistrée à la Sous-Préfecture de Grasse (06) N° 7803/88 Internet [email protected] Individual copies of this ETSI deliverable can be downloaded from http://www.etsi.org If you find errors in the present document, send your comment to: [email protected] Important notice This ETSI deliverable may be made available in more than one electronic version or in print. In any case of existing or perceived difference in contents between such versions, the reference version is the Portable Document Format (PDF). In case of dispute, the reference shall be the printing on ETSI printers of the PDF version kept on a specific network drive within ETSI Secretariat. Copyright Notification No part may be reproduced except as authorized by written permission. The copyright and the foregoing restriction extend to reproduction in all media. © European -
Air Compressor Noise Control Air Compressor Noise Control
AIR COMPRESSOR BY NOISE CONTROL USA AIR COMPRESSOR NOISE CONTROL AIR COMPRESSOR NOISE CONTROL Compressor are often noisy an effective solution is often required to suppress the noise emitted from them. Compressor noise is usually a nuisance because they are sitting on comparatively lightweight structures. The best way to soundproof and to reduce any noise from a compressor regardless of size is to enclose it within a Floor Mounted 4-Sided Soundproofing Acoustic blanket Enclosure. For best results the enclosure should be as large as possible to allow less heat buildup and also to be more effective at reducing the noise output from reaching other areas and acoustically isolating the Compressor to contain structure borne sound being transmitted from where it is mounted. Depending on the current sound levels of the Compressor and your noise reduction goals, an abatement solution can be determined. In most applications a soundproofing blanket enclosure will meet your sound reduction needs. This is a two to four sided soundproofing enclosure with or without a roof. Typically a frame and track is constructed to suspend the soundproofing curtain panels. The soundproofing blankets material is a composite material bonding mass loaded vinyl with an acoustical absorber and faced with a vinyl diamond stitched facing. Using our Soundproofing Acoustic Blankets to construct a 4-sided noise control solution will significantly reduce sound. The noise reduction to be expected is a range of 20 to 40 decibels. The better the construction, weight of blankets and amount of soundproofing acoustic blankets used (the surface area) all factor into your sound reduction numbers. -
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. -
Suburban Noise Control with Plant Materials and Solid Barriers
Suburban Noise Control with Plant Materials and Solid Barriers by DAVID I. COOK and DAVID F. Van HAVERBEKE, respectively professor of engineering mechanics, University of Nebraska, Lin- coln; and silviculturist, USDA Forest Service, Rocky Mountain Forest and Range Experiment Station, Fort Collins, Colo. ABSTRACT.-Studies were conducted in suburban settings with specially designed noise screens consisting of combinations of plant inaterials and solid barriers. The amount of reduction in sound level due to the presence of the plant materials and barriers is re- ported. Observations and conclusions for the measured phenomenae are offered, as well as tentative recommendations for the use of plant materials and solid barriers as noise screens. YOUR$50,000 HOME IN THE SUB- relocated truck routes, and improved URBS may be the object of an in- engine muffling can be helpful. An al- vasion more insidious than termites, and ternative solution is to create some sort fully as damaging. The culprit is noise, of barrier between the noise source and especially traffic noise; and although it the property to be protected. In the will not structurally damage your house, Twin Cities, for instance, wooden walls it will cause value depreciation and dis- up to 16 feet tall have been built along comfort for you. The recent expansion Interstate Highways 35 and 94. Al- of our national highway systems, and though not esthetically pleasing, they the upgrading of arterial streets within have effectively reduced traffic noise, the city, have caused widespread traffic- and the response from property owners noise problems at residential properties. has been generally favorable. -
Acoustical and Optical Radiation Pressures and the Development of Single Beam Acoustical Tweezers Jean-Louis Thomas, Régis Marchiano, Diego Baresch
Acoustical and optical radiation pressures and the development of single beam acoustical tweezers Jean-Louis Thomas, Régis Marchiano, Diego Baresch To cite this version: Jean-Louis Thomas, Régis Marchiano, Diego Baresch. Acoustical and optical radiation pressures and the development of single beam acoustical tweezers. Journal of Quantitative Spectroscopy and Radiative Transfer, Elsevier, 2017, 195, pp.55-65. 10.1016/j.jqsrt.2017.01.012. hal-01438774 HAL Id: hal-01438774 https://hal.archives-ouvertes.fr/hal-01438774 Submitted on 18 Jan 2017 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. Acoustical and optical radiation pressures and the development of single beam acoustical tweezers Jean-Louis Thomasa,∗, R´egisMarchianob, Diego Barescha,b aSorbonne Universit´es,UPMC Univ Paris 06, CNRS UMR 7588, Institut des NanoSciences de Paris, 4 place Jussieu, Paris, France bSorbonne Universit´es,UPMC Univ Paris 06, CNRS UMR 7190, Institut Jean le Rond d'Alembert, 4 place Jussieu, Paris, France Abstract Studies on radiation pressure in acoustics and optics have enriched one an- other and have a long common history. Acoustic radiation pressure is used for metrology, levitation, particle trapping and actuation. However, the dexter- ity and selectivity of single-beam optical tweezers are still to be matched with acoustical devices. -
Realisation of the First Sub Shot Noise Wide Field Microscope
Realisation of the first sub shot noise wide field microscope Nigam Samantaray1,2, Ivano Ruo-Berchera1, Alice Meda1, , Marco Genovese1,3 1 INRIM, Strada delle Cacce 91, I-10135 Torino, ∗Italy 2 Politecnico di Torino, Corso Duca degli Abruzzi, 24 - I-10129 Torino, Italy and 3 INFN, Via P. Giuria 1, I-10125 Torino, Italy ∗ ∗ Correspondence: Alice Meda, Email: [email protected], Tel: +390113919245 In the last years several proof of principle experiments have demonstrated the advantages of quantum technologies respect to classical schemes. The present challenge is to overpass the limits of proof of principle demonstrations to approach real applications. This letter presents such an achievement in the field of quantum enhanced imaging. In particular, we describe the realization of a sub-shot noise wide field microscope based on spatially multi-mode non-classical photon number correlations in twin beams. The microscope produces real time images of 8000 pixels at full resolution, for (500µm)2 field-of-view, with noise reduced to the 80% of the shot noise level (for each pixel), suitable for absorption imaging of complex structures. By fast post-elaboration, specifically applying a quantum enhanced median filter, the noise can be further reduced (less than 30% of the shot noise level) by setting a trade-off with the resolution, demonstrating the best sensitivity per incident photon ever achieved in absorption microscopy. Keywords: imaging, sub shot noise, microscopy, parametric down conversion 1 INTRODUCTION Sensitivity in standard optical imaging and sensing, the ones exploiting classical illuminating fields, is fundamentally lower bounded by the shot noise, the inverse square root of the number of photons used. -
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. -
Low Power Energy Harvesting and Storage Techniques from Ambient Human Powered Energy Sources
University of Northern Iowa UNI ScholarWorks Dissertations and Theses @ UNI Student Work 2008 Low power energy harvesting and storage techniques from ambient human powered energy sources Faruk Yildiz University of Northern Iowa Copyright ©2008 Faruk Yildiz Follow this and additional works at: https://scholarworks.uni.edu/etd Part of the Power and Energy Commons Let us know how access to this document benefits ouy Recommended Citation Yildiz, Faruk, "Low power energy harvesting and storage techniques from ambient human powered energy sources" (2008). Dissertations and Theses @ UNI. 500. https://scholarworks.uni.edu/etd/500 This Open Access Dissertation is brought to you for free and open access by the Student Work at UNI ScholarWorks. It has been accepted for inclusion in Dissertations and Theses @ UNI by an authorized administrator of UNI ScholarWorks. For more information, please contact [email protected]. LOW POWER ENERGY HARVESTING AND STORAGE TECHNIQUES FROM AMBIENT HUMAN POWERED ENERGY SOURCES. A Dissertation Submitted In Partial Fulfillment of the Requirements for the Degree Doctor of Industrial Technology Approved: Dr. Mohammed Fahmy, Chair Dr. Recayi Pecen, Co-Chair Dr. Sue A Joseph, Committee Member Dr. John T. Fecik, Committee Member Dr. Andrew R Gilpin, Committee Member Dr. Ayhan Zora, Committee Member Faruk Yildiz University of Northern Iowa August 2008 UMI Number: 3321009 INFORMATION TO USERS The quality of this reproduction is dependent upon the quality of the copy submitted. Broken or indistinct print, colored or poor quality illustrations and photographs, print bleed-through, substandard margins, and improper alignment can adversely affect reproduction. In the unlikely event that the author did not send a complete manuscript and there are missing pages, these will be noted. -
Bernoulli-Gaussian Distribution with Memory As a Model for Power Line Communication Noise Victor Fernandes, Weiler A
XXXV SIMPOSIO´ BRASILEIRO DE TELECOMUNICAC¸ OES˜ E PROCESSAMENTO DE SINAIS - SBrT2017, 3-6 DE SETEMBRO DE 2017, SAO˜ PEDRO, SP Bernoulli-Gaussian Distribution with Memory as a Model for Power Line Communication Noise Victor Fernandes, Weiler A. Finamore, Mois´es V. Ribeiro, Ninoslav Marina, and Jovan Karamachoski Abstract— The adoption of Additive Bernoulli-Gaussian Noise very useful to come up with a as simple as possible models (ABGN) as an additive noise model for Power Line Commu- of PLC noise, similar to the additive white Gaussian noise nication (PLC) systems is the subject of this paper. ABGN is a (AWGN) model. model that for a fraction of time is a low power noise and for the remaining time is a high power (impulsive) noise. In this context, In this regard, we introduce the definition of a simple and we investigate the usefulness of the ABGN as a model for the useful mathematical model for the noise perturbing the data additive noise in PLC systems, using samples of noise registered transmission over PLC channel that would be a helpful tool. during a measurement campaign. A general procedure to find the With this goal in mind, an investigation of the usefulness of model parameters, namely, the noise power and the impulsiveness what we call additive Bernoulli-Gaussian noise (ABGN) as a factor is presented. A strategy to assess the noise memory, using LDPC codes, is also examined and we came to the conclusion that model for the noise perturbing the digital communication over ABGN with memory is a consistent model that can be used as for PLC channel is discussed. -
In-Situ Attenuation Corrections for Radiation Force Measurements of High Frequency Ultrasound with a Conical Target
Volume 111, Number 6, November-December 2006 Journal of Research of the National Institute of Standards and Technology [J. Res. Natl. Inst. Stand. Technol. 111, 435-442 (2006)] In-situ Attenuation Corrections for Radiation Force Measurements of High Frequency Ultrasound With a Conical Target Volume 111 Number 6 November-December 2006 Steven E. Fick Radiation force balance (RFB) measure- Key words: attenuation correction; coni- ments of time-averaged, spatially-integrat- cal target; in-situ attenuation; power meas- National Institute of Standards ed ultrasound power transmitted into a urement; radiation force balance; radiation and Technology, reflectionless water load are based on pressure; ultrasonic power; ultrasound Gaithersburg, MD 20899 measurements of the power received by power. the RFB target. When conical targets are used to intercept the output of collimated, and circularly symmetric ultrasound sources operating at frequencies above a few Dorea Ruggles megahertz, the correction for in-situ atten- uation is significant, and differs signifi- cantly from predictions for idealized cir- School of Architecture, Accepted: November 7, 2006 cumstances. Empirical attenuation correc- Program in Architectural tion factors for a 45° (half-angle) absorp- Acoustics, tive conical RFB target have been deter- Rensselaer Polytechnic Institute, mined for 24 frequencies covering the 5 Troy, NY 12180 MHz to 30 MHz range. They agree well with previously unpublished attenuation calibration factors determined in 1994 for [email protected] a similar target. Available online: http://www.nist.gov/jres 1. Introduction stances, the inertia of the target causes it to effectively integrate pulses into the corresponding steady-state Radiation pressure [1-13] has been employed in a force. -
EP Signal to Noise in Emp 2
TN0000909 – Former Doc. No. TECN1852625 – New Doc. No. Rev. 02 Page 1 of 5 Understanding the EP Signal-to-Noise Calculation in Empower 2 This document: • Provides a definition of the 2005 European Pharmacopeia (EP) signal-to-noise ratio • Describes the built-in EP S/N calculation in Empower™ 2 • Describes the custom field necessary to determine EP S/N using noise from a blank injection. 2005 European Pharmacopeia (EP) Definition: Signal-to-Noise Ratio The signal-to-noise ratio (S/N) influences the precision of quantification and is calculated by the equation: 2H S/N = λ where: H = Height of the peak (Figure 1) corresponding to the component concerned, in the chromatogram obtained with the prescribed reference solution, measured from the maximum of the peak to the extrapolated baseline of the signal observed over a distance equal to 20 times the width at half-height. λ = Range of the background noise in a chromatogram obtained after injection or application of a blank, observed over a distance equal to 20 times the width at half- height of the peak in the chromatogram obtained with the prescribed reference solution and, if possible, situated equally around the place where this peak would be found. Figure 1 – Peak Height Measurement TN0000909 – Former Doc. No. TECN1852625 – New Doc. No. Rev. 02 Page 2 of 5 In Empower 2 software, the EP Signal-to-Noise (EP S/N) is determined in an automated fashion and does not require a blank injection. The intention of this calculation is to preserve the sense of the EP calculation without requiring a separate blank injection. -
Measurement and Estimation of the Mode Partition Coefficient K
Measurement and Estimation of the Mode Partition Coefficient k Rick Pimpinella and Jose Castro IEEE P802.3bm 40 Gb/s and 100 Gb/s Fiber Optic Task Force November 2012, San Antonio, TX Background & Objective Background: Mode Partition Noise in MMF channel links is caused by pulse-to-pulse power fluctuations among VCSEL modes and differential delay due to dispersion in the fiber (Power independent penalty) “k” is an index used to describe the degree of mode fluctuations and takes on a value between 0 and 1, called the mode partition coefficient [1,2] Currently the IEEE link model assumes k = 0.3 It has been discussed that a new link model requires validation of k The measurement & estimation of k is challenging due to several conditions: Low sensitivity of detectors at 850nm The presence of additional noise components in VCSEL-MMF channels (RIN, MN, Jitter – intensity fluctuations, reflection noise, thermal noise, …) Differences in VCSEL designs Objective: Provide an experimental estimate of the value of k for VCSELs Additional work in progress 2 MPN Theory Originally derived for Fabry-Perot lasers and SMF [3] Assumptions: Total power of all modes carried by each pulse is constant Power fluctuations among modes are anti-correlated Mechanism: When modes (different wavelengths) travel at the same speed their fluctuations remain anti-correlated and the resultant pulse-to-pulse noise is zero. When modes travel in a dispersive medium the modes undergo different delays resulting in pulse distortions and a noise penalty. Example: Two VCSEL modes transmitted in a SMF undergoing chromatic dispersion: START END Optical Waveform @ Detector START t END With mode power fluctuations Decision Region Shorter Wavelength Time (arrival) t slope DL Time (arrival) Longer Wavelength Time (arrival) 3 Example of Intensity Fluctuation among VCSEL modes MPN can be observed using an Optical Spectrum Analyzer (OSA).