ORC Speed Guide Explanation
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CHAPTER 20 Wind Turbine Noise Measurements and Abatement
CHAPTER 20 Wind turbine noise measurements and abatement methods Panagiota Pantazopoulou BRE, Watford, UK. This chapter presents an overview of the types, the measurements and the potential acoustic solutions for the noise emitted from wind turbines. It describes the fre- quency and the acoustic signature of the sound waves generated by the rotating blades and explains how they propagate in the atmosphere. In addition, the avail- able noise measurement techniques are being presented with special focus on the technical challenges that may occur in the measurement process. Finally, a discus- sion on the noise treatment methods from wind turbines referring to a range of the existing abatement methods is being presented. 1 Introduction Wind turbines generate two types of noise: aerodynamic and mechanical. A tur- bine’s sound power is the combined power of both. Aerodynamic noise is gener- ated by the blades passing through the air. The power of aerodynamic noise is related to the ratio of the blade tip speed to wind speed. The mechanical noise is associated with the relevant motion between the various parts inside the nacelle. The compartments move or rotate in order to convert kinetic energy to electricity with the expense of generating sound waves and vibration which is transmitted through the structural parts of the turbine. Depending on the turbine model and the wind speed, the aerodynamic noise may seem like buzzing, whooshing, pulsing, and even sizzling. Downwind tur- bines with their blades downwind of the tower cause impulsive noise which can travel far and become very annoying for people. The low frequency noise gener- ated from a wind turbine is primarily the result of the interaction of the aerody- namic lift on the blades and the atmospheric turbulence in the wind. -
An Analytical Approach to the Question of a Clock Change
An Analytical Approach to the Question of a Clock Change by Samuel Halpern One of the ongoing arguments that continues to be brought up is the question of whether or not clocks on Titanic were put back some time before the accident took place Sunday night, April 14, 1912. Some of the deck crew, awakened by the accident at 11:40 p.m. ship’s time, thought that it was close to the time that they were due to take their watch on deck, which would be at 12 o’clock. Despite Boatswain’s Mate Albert Haines, who was awake and on duty at the time, testifying that “The right time, without putting the clock back, was 20 minutes to 12,” there are some that try to argue that a 24 minute clock adjustment had already taken place, and the time of the accident on an unadjusted clock still keeping April 14th time would have been 4 minutes past 12. The underlying question that would resolve this issue is the run time from noon Sunday to the time of the accident. If the run time from noon to the time of the accident was 11 hours 40 minutes, then no clock change had yet taken place, and the time of collision was 11:40 p.m. in unadjusted hours. If the run time was more than 12 hours, then there was a clock change of some 23 or 24 minutes, and the time of collision was 11:40 p.m. in adjusted hours. It really is that simple. So how do we determine the actual run time from the available evidence that does not have to rely on subjective estimates such as time intervals or other measures that people may have perceived? The answer is to take an analytical approach to the problem using the taffrail log mileage data offered by quartermasters George Rowe and Robert Hichens at the inquiries. -
Atmospheric Effects on Traffic Noise Propagation
TRANSPORTATION RESEARCH RECORD 1255 59 Atmospheric Effects on Traffic Noise Propagation ROGER L. WAYSON AND WILLIAM BOWLBY Atmospheric effects on traffic noise propagation have largely L 0 sound level at a reference distance, been ignored during measurements and modeling, even though Ageo attenuation due to geometric spreading, it has generally been accepted that the effects may produce large Ab insertion loss due to diffraction, changes in receiver noise levels. Measurement of traffic noise at L, level increases due to reflection, and multiple locations concurrently with measurement of meteoro Ac attenuation due to ground characteristics and envi logical data is described. Statistical methods were used to evaluate the data. Atmospheric effects on traffic noise levels were shown ronmental effects. to be significant, even at very short distances; parallel components It should be noted that all levels in dB in this paper are of the wind (which are usually ignored) were important at second 2 row receivers; turbulent scattering increased noise levels near the referenced to 2 x 10-s N/m • ground more than refractive ray bending for short-distance prop The last term on the right side of Equation 1, A,, consists agation; and temperature lapse rates were not as important as of three parameters: ground attenuation, attenuation due to wind shear very near the highway. A statistical model was devel atmospheric absorption, and attenuation due to atmospheric oped to predict excess attenuations due to atmospheric effects. refraction. (2) Outdoor noise propagation has been studied since the time of the Greek philosopher Chrysippus (240 B. C.). Modern where prediction models have become accurate, and the advent of computers has increased the capabilities of models. -
Industrial Aerodynamics
INDUSTRIAL AERODYNAMICS Unit I Wind Energy Collectors INTRODUCTION Air Movement Wind Air Current Circulation The horizontal movement of air along the earth’s surface is called a Wind. The vertical movement of the air is known as an air current. Winds and air current together comprise a system of circulation in the atmosphere. TYPES OF WINDS On the earth’s surface, certain winds blow constantly in a particular direction throughout the year. These are known as the ‘Prevailing Winds’. They are also called the Permanent or the Planetary Winds. Certain winds blow in one direction in one season and in the opposite direction in another. They are known as Periodic Winds. Then, there are Local Winds in different parts of the world. 1. Planetary Winds: There are three main planetary winds that constantly blow in the same direction all around the world. They are also called prevailing or permanent winds. 1.Trade Winds: Blow from the subtropical high pressure belt towards the Equator. They are called the north-east trades in the northern hemisphere and south-east trades in the southern hemisphere. 2.Westerly winds: Blow from the same subtropical high pressure belts, towards 60˚ S and 60˚ N latitude. They are called the sought Westerly wind sin the northern hemisphere and North Westerly winds in the southern hemispheres. 3.Polar Winds Blow from the polar high pressure to the sub polar low pressure area. In the northern hemisphere, their direction is from the north-east. In the southern hemisphere, they blow from the south-east. 2. Periodic Winds These winds are known to blow for a certain time in a certain direction - it may be for a part of a day or a particular season of the year. -
Small Lightweight Aircraft Navigation in the Presence of Wind Cornel-Alexandru Brezoescu
Small lightweight aircraft navigation in the presence of wind Cornel-Alexandru Brezoescu To cite this version: Cornel-Alexandru Brezoescu. Small lightweight aircraft navigation in the presence of wind. Other. Université de Technologie de Compiègne, 2013. English. NNT : 2013COMP2105. tel-01060415 HAL Id: tel-01060415 https://tel.archives-ouvertes.fr/tel-01060415 Submitted on 3 Sep 2014 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. Par Cornel-Alexandru BREZOESCU Navigation d’un avion miniature de surveillance aérienne en présence de vent Thèse présentée pour l’obtention du grade de Docteur de l’UTC Soutenue le 28 octobre 2013 Spécialité : Laboratoire HEUDIASYC D2105 Navigation d'un avion miniature de surveillance a´erienneen pr´esencede vent Student: BREZOESCU Cornel Alexandru PHD advisors : LOZANO Rogelio CASTILLO Pedro i ii Contents 1 Introduction 1 1.1 Motivation and objectives . .1 1.2 Challenges . .2 1.3 Approach . .3 1.4 Thesis outline . .4 2 Modeling for control 5 2.1 Basic principles of flight . .5 2.1.1 The forces of flight . .6 2.1.2 Parts of an airplane . .7 2.1.3 Misleading lift theories . 10 2.1.4 Lift generated by airflow deflection . -
Gunwale (Canoe Rails) Repair Guide Wood Gunwale Repair
Gunwale (Canoe Rails) Repair Guide Wood Gunwale Repair Canoes with fine woodwork are a tradition at Mad River Canoe. The rails, seats and thwarts on your Mad River Canoe are native Vermont straight-grained ash, chosen for its resiliency, strength and aesthetic appearance. Unlike aluminum or plastic materials, white ash will not kink upon impact and cause undue damage to the canoe hull. There are more options involved in repair of wood gunwales than with vinyl or aluminum, making this section a bit longer than the corresponding instructions for other types of rails. Don't let the length of this document intimidate you - here's an overview of this section to help you plan your repair strategy: General Information - Everyone should read this section. Pre-installation preparation - Everyone should read this section. Gunwale replacement instructions - How to replace both rails of your canoe. Replacing Gunwales with inset decks (including complete deck replacement) - If your canoe has inset decks you will likely have to replace them when you replace your rails. The other option is: Short-splicing method to preserve original inset decks when rerailing - You may cut the existing inwales of your canoe to avoid replacing your existing deck. The new inwale must be carefully spliced to the section of existing inwale. Installation of a 4' splicing section - If you have damage to a small section of gunwale, you can splice in a replacement section on the inside, outside or both. General Information Ordering replacement ash gunwales Rails can be ordered from an authorized Mad River dealer. Replacement ash rails are available for all Mad River Canoes. -
Leopard 58' Catamaran – RABBLE ROUSER
Leopard 58' Catamaran – RABBLE ROUSER Make: Leopard Boat Name: RABBLE ROUSER Model: 58' Catamaran Hull Material: Fiberglass Length: 58 ft Draft: 5 ft 7 in Price: $ 1,550,000 Builder: Robertson & Caine Year: 2014 Designer: Simonis Voogd Location: Ft. Lauderdale, FL, United States RABBLE ROUSER RABBLE ROUSER is an exceptional Owner’s version of the Leopard 58 with 4 cabin layout. Built and launched as a Leopard 58 but that’s where it starts and ends. In the hands of her current and original owner she was transformed into one of the most customized, highly detailed, well equipped and unique Leopard 58’s in existence. From her Carbon fiber roller furling boom to make sailing easy, to the custom cabinetry to enhance the already generous storage space, and a custom electrical system, where there was an opportunity to improve or make better, it was done. With low hours on both her engines and generators, this boat has East Coast Yacht Sales - Allen Schiller, CPYB at Dion's Yacht Yard, 23 Glendale Street, Salem, MA 01970, United States Tel: 617-529-5553 cell Tel: 707-414-0414 Fax: 978-744-7071 [email protected] seen very light use. You owe it to yourself to at least get onboard and see if RABBLE ROUSER is the boat for you. An Addendum section captures many of the changes and the thought process behind them. Measurements Cruising Speed: 9.5 kn Displacement: 61730 Cruising Speed RPM: 2200 lb LOA: 57 ft 7 in Fuel Tanks #: 4 LWL: 54 ft 2 in Fuel Tanks Capacity: 394 gal Beam: 27 ft 9 in Fresh Water Tanks #: 2 Max Bridge Clearance: 90 ft 3 in Fresh Water -
Olympic Broach: E No Good Very Bad Windiest Day Two Races in Athens Shatter an Olympic Medal Dream
November 30th 2014 by Lenny Rudow Olympic Broach: e No Good Very Bad Windiest Day Two races in Athens shatter an Olympic medal dream. Day two of sailing at the 2004 Olympics started out just like day one: sunny and gaspingly hot, with only about three knots of wind. And just like the day before, I called up to the committee boat, “Good morning—USA.” At this regatta, I checked in not as myself or as the skipper of a three-person team, but as an entire country. What a rush. I remember that moment perfectly, but it’s taken me 10 years to swallow my pride enough to write about what followed. And I’m only going to do it once, so listen up. Day two started out very light and ended up very windy. Fortunately our Olympic branding held up to the change in conditions better than we did. Photo: ©DanielForster STARTING STRONG Th e Saronic Gulf rippled and heat-shimmered beneath the light easterly, which we hoped would build to meet the fi ve-knot minimum in time for racing. In similar conditions the day before, we’d fi nished second in the very fi rst race of our week-long event. So I’d chosen the same clothing: white long-sleeved shirt, light-colored leggings, white USA hat. Liz had gone with short sleeves and Nancy sported a tank top, but we were unifi ed by our Team USA regatta pinnies. And in case we forgot our last names, all we had to do was look up—they’d been stuck on the mainsail in bold letters, just below a large American fl ag. -
In Wind and Ocean Currents
PAPERS IN PHYSICAL OCEANOGRAPHY AND METEOROLOGY PUBLISHED BY MASSACHUSETTS INSTITUTE OF TECHNOLOGY AND WOODS HOLE OCEANOGRAPHIC INSTITUTION (In continuation of Massachusetts Institute of Technology Meteorological Papers) VOL. III, NO.3 THE LAYER OF FRICTIONAL INFLUENCE IN WIND AND OCEAN CURRENTS BY c.-G. ROSSBY AND R. B. MONTGOMERY Contribution No. 71 from the Woods Hole Oceanographic Institution .~ J~\ CAMBRIDGE, MASSACHUSETTS Ap~il, 1935 CONTENTS i. INTRODUCTION 3 II. ADIABATIC ATMOSPHERE. 4 1. Completion of Solution for Adiabatic Atmosphere 4 2. Light Winds and Residual Turbulence 22 3. A Study of the Homogeneous Layer at Boston 25 4. Second Approximation 4° III. INFLUENCE OF STABILITY 44 I. Review 44 2. Stability in the Boundary Layer 47 3. Stability within Entire Frictional Layer 56 IV. ApPLICATION TO DRIFT CURRENTS. 64 I. General Commen ts . 64 2. The Homogeneous Layer 66 3. Analysis of Material 67 4. Results of Analysis . 69 5. Scattering of the Observations and Advection 72 6. Oceanograph Observations 73 7. Wind Drift of the Ice 75 V. LENGTHRELATION BETWEEN THE VELOCITY PROFILE AND THE VALUE OF THE85 MIXING ApPENDIX2.1. StirringTheoretical in Shallow Comments . Water 92. 8885 REFERENCESSUMMARYModified Computation of the Boundary Layer in Drift Currents 9899 92 1. INTRODUCTION The purpose of the present paper is to analyze, in a reasonably comprehensive fash- ion, the principal factors controlling the mean state of turbulence and hence the mean velocity distribution in wind and ocean currents near the surface. The plan of the in- vestigation is theoretical but efforts have been made to check each major step or result through an analysis of available measurements. -
Wells/Kern Take Down Southern CC Regatta
Wells/Kern Take Down Southern CC Regatta Above: Wells/Kern (#1130) make a close cross as Hennon/Wallace tack away from the shore at the SCC. The 6th Southern Comfort Classic regatta kicked suited up five boats for the event, including one off Friday night with ASC members Lenny Wells helmed by Nicky Einthoven with crew Teri and Teri Fosmire sharing some alone time at the Fosmire, still glowing from her date with Lenny local pizza joint. We are still investigating the lack of enthusiasm for the annual darts and beer IN THIS ISSUE extravaganza, but preliminary indications point towards the absence of Dave “Plywood” Michos Southern Comfort Classic Pictures.……..…… 3 and Brent “It’s only a 5 hour drive to NC” Restoring a Classic (Part II) ………………4 Barbehenn as primary factors. Upcoming Regattas………………….…….…6 Classifieds…………………………..………… 6 The weather forecast was very promising for the President’s Corner……..…………………….7 entire weekend and did not disappoint. ASC Jet-14 Connect!.............……….……………...7 2 the previous evening. Lenny was joined by his ultimately could not recover and had to retire for rising junior star, Caswell Kern, while new Jet the day. Wells/Kern went on to take the next member Curtis Boyd was ready to give #203 its two races and secure the lead. first action of the year. Joining the ASC boats That night, the fleet enjoyed a wonderful was our regular traveler, Tom Grace and Paula evening at the local restaurant on the lake. They Pacheco (Lake Norman YC) in Wren, last were joined by several ASC club members for a renovated during the Eisenhower BBQ meal. -
Parts of a Ship: the Basics
Parts of a Ship: The Basics PORT SIDE MAIN FORE MAIN WINDLASS STERN AFT BOW TILLER MAST MAST HATCH HATCH STARBOARD SIDE Overhead view of the schooner Sultana he front of a ship is called the bow, and the back is called the stern. If you were standing T on the ship’s deck looking forward (towards the bow), the left side would be the port side and the right side would be the starboard side. Close to Sultana’s stern is the tiller, a long stick attached to a device called a rudder used for steering the ship. Other important items include the main mast, the fore mast and the windlass (a large simple machine used for pulling up the anchor). POOP DECK QUARTER DECK MIDDLE DECK FORE DECK MAIN TILLER HATCH ultana’s deck is divided into four sections. At the front of the ship is the fore deck, where S the anchors are stored and the fore mast is located. The largest section of the ship is the middle deck where the main hatch is located. Historically, this is where cargo would have been loaded and unloaded. Towards the ship’s stern is the quarter deck. On larger ships, only the high ranking officers were allowed to stand in this area. Sultana’s smallest deck is the poop deck, where sailors steered with the tiller. Parts of a Ship: The Basics NAME: ____________________________________________ DATE: ____________ DIRECTIONS: Use information from the reading to answer each of the following questions in a complete sentence. 1. What is the front of a ship called? What do you call the back end of a ship? 2. -
The Evolution of Decorative Work on English Men-Of-War from the 16
THE EVOLUTION OF DECORATIVE WORK ON ENGLISH MEN-OF-WAR FROM THE 16th TO THE 19th CENTURIES A Thesis by ALISA MICHELE STEERE Submitted to the Office of Graduate Studies of Texas A&M University in partial fulfillment of the requirements for the degree of MASTER OF ARTS May 2005 Major Subject: Anthropology THE EVOLUTION OF DECORATIVE WORK ON ENGLISH MEN-OF-WAR FROM THE 16th TO THE 19th CENTURIES A Thesis by ALISA MICHELE STEERE Submitted to the Office of Graduate Studies of Texas A&M University in partial fulfillment of the requirements for the degree of MASTER OF ARTS Approved as to style and content by: C. Wayne Smith James M. Rosenheim (Chair of Committee) (Member) Luis Filipe Vieira de Castro David L. Carlson (Member) (Head of Department) May 2005 Major Subject: Anthropology iii ABSTRACT The Evolution of Decorative Work on English Men-of-War from the 16th to the 19th Centuries. (May 2005) Alisa Michele Steere, B.A., Texas A&M University Chair of Advisory Committee: Dr. C. Wayne Smith A mixture of shipbuilding, architecture, and art went into producing the wooden decorative work aboard ships of all nations from around the late 1500s until the advent of steam and the steel ship in the late 19th century. The leading humanists and artists in each country were called upon to draw up the iconographic plan for a ship’s ornamentation and to ensure that the work was done according to the ruler’s instructions. By looking through previous research, admiralty records, archaeological examples, and contemporary ship models, the progression of this maritime art form can be followed.