The Impact of Seasonal Changes in Stratification on the Dynamics of Internal Waves in the Sea of Okhotsk
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Regional Climatology East Asian Seas: an Introduction
NOAA Atlas NESDIS 79 doi:10.7289/V5D21VM9 REGIONAL CLIMATOLOGY OF THE EAST ASIAN SEAS: AN INTRODUCTION National Centers for Environmental Information Silver Spring, Maryland December 2015 U.S. DEPARTMENT OF COMMERCE National Oceanic and Atmospheric Administration National Environmental Satellite, Data, and Information Service National Centers for Environmental Information Additional copies of this publication, as well as information about National Centers for Environmental Information (formerly the National Oceanographic Data Center) data holdings and services, are available upon request directly from the National Centers for Environmental Information. National Centers for Environmental Information User Services Team NOAA/NESDIS/NCEI SSMC III, 4th floor 1315 East-West Highway Silver Spring, MD 20910-3282 Telephone: (301) 713-3277 E-mail: [email protected] NCEI Oceans Home Page: http://www.ncei.noaa.gov/ This document should be cited as: Johnson, D.R., Boyer, T.P., 2015: Regional Climatology of the East Asian Seas: An Introduction. NOAA Atlas NESDIS 79, Silver Spring, MD, 37 pp. doi:10.7289/V5D21VM9. This document is available at http://data.nodc.noaa.gov/woa/REGCLIM/EAS/DOC/nesdis79-doi107289V5D21VM9.pdf. Editor: Dan Seidov, National Centers for Environmental Information Technical Editor: Alexey Mishonov, National Centers for Environmental Information NOAA Atlas NESDIS 79 doi:10.7289/V5D21VM9 REGIONAL CLIMATOLOGY OF THE EAST ASIAN SEAS: AN INTRODUCTION Daphne R. Johnson and Tim P. Boyer National Centers for Environmental Information Silver Spring, Maryland December 2015 U.S. DEPARTMENT OF COMMERCE Penny Pritzker, Secretary National Oceanic and Atmospheric Administration Kathryn Sullivan Under Secretary of Commerce for Oceans and Atmosphere and NOAA Administrator National Environmental Satellite, Data, and Information Service Stephen Volz, Assistant Administrator This page intentionally left blank Table of Contents ABSTRACT ...................................................................................................................................... -
Waves on Deep Water, I
Lecture 14: Waves on deep water, I Lecturer: Harvey Segur. Write-up: Adrienne Traxler June 23, 2009 1 Introduction In this lecture we address the question of whether there are stable wave patterns that propagate with permanent (or nearly permanent) form on deep water. The primary tool for this investigation is the nonlinear Schr¨odinger equation (NLS). Below we sketch the derivation of the NLS for deep water waves, and review earlier work on the existence and stability of 1D surface patterns for these waves. The next lecture continues to more recent work on 2D surface patterns and the effect of adding small damping. 2 Derivation of NLS for deep water waves The nonlinear Schr¨odinger equation (NLS) describes the slow evolution of a train or packet of waves with the following assumptions: • the system is conservative (no dissipation) • then the waves are dispersive (wave speed depends on wavenumber) Now examine the subset of these waves with • only small or moderate amplitudes • traveling in nearly the same direction • with nearly the same frequency The derivation sketch follows the by now normal procedure of beginning with the water wave equations, identifying the limit of interest, rescaling the equations to better show that limit, then solving order-by-order. We begin by considering the case of only gravity waves (neglecting surface tension), in the deep water limit (kh → ∞). Here h is the distance between the equilibrium surface height and the (flat) bottom; a is the wave amplitude; η is the displacement of the water surface from the equilibrium level; and φ is the velocity potential, u = ∇φ. -
21 Non-Linear Wave Equations and Solitons
Utah State University DigitalCommons@USU Foundations of Wave Phenomena Open Textbooks 8-2014 21 Non-Linear Wave Equations and Solitons Charles G. Torre Department of Physics, Utah State University, [email protected] Follow this and additional works at: https://digitalcommons.usu.edu/foundation_wave Part of the Physics Commons To read user comments about this document and to leave your own comment, go to https://digitalcommons.usu.edu/foundation_wave/2 Recommended Citation Torre, Charles G., "21 Non-Linear Wave Equations and Solitons" (2014). Foundations of Wave Phenomena. 2. https://digitalcommons.usu.edu/foundation_wave/2 This Book is brought to you for free and open access by the Open Textbooks at DigitalCommons@USU. It has been accepted for inclusion in Foundations of Wave Phenomena by an authorized administrator of DigitalCommons@USU. For more information, please contact [email protected]. Foundations of Wave Phenomena, Version 8.2 21. Non-linear Wave Equations and Solitons. In 1834 the Scottish engineer John Scott Russell observed at the Union Canal at Hermiston a well-localized* and unusually stable disturbance in the water that propagated for miles virtually unchanged. The disturbance was stimulated by the sudden stopping of a boat on the canal. He called it a “wave of translation”; we call it a solitary wave. As it happens, a number of relatively complicated – indeed, non-linear – wave equations can exhibit such a phenomenon. Moreover, these solitary wave disturbances will often be stable in the sense that if two or more solitary waves collide then after the collision they will separate and take their original shape. -
Shallow Water Waves and Solitary Waves Article Outline Glossary
Shallow Water Waves and Solitary Waves Willy Hereman Department of Mathematical and Computer Sciences, Colorado School of Mines, Golden, Colorado, USA Article Outline Glossary I. Definition of the Subject II. Introduction{Historical Perspective III. Completely Integrable Shallow Water Wave Equations IV. Shallow Water Wave Equations of Geophysical Fluid Dynamics V. Computation of Solitary Wave Solutions VI. Water Wave Experiments and Observations VII. Future Directions VIII. Bibliography Glossary Deep water A surface wave is said to be in deep water if its wavelength is much shorter than the local water depth. Internal wave A internal wave travels within the interior of a fluid. The maximum velocity and maximum amplitude occur within the fluid or at an internal boundary (interface). Internal waves depend on the density-stratification of the fluid. Shallow water A surface wave is said to be in shallow water if its wavelength is much larger than the local water depth. Shallow water waves Shallow water waves correspond to the flow at the free surface of a body of shallow water under the force of gravity, or to the flow below a horizontal pressure surface in a fluid. Shallow water wave equations Shallow water wave equations are a set of partial differential equations that describe shallow water waves. 1 Solitary wave A solitary wave is a localized gravity wave that maintains its coherence and, hence, its visi- bility through properties of nonlinear hydrodynamics. Solitary waves have finite amplitude and propagate with constant speed and constant shape. Soliton Solitons are solitary waves that have an elastic scattering property: they retain their shape and speed after colliding with each other. -
Joint Industry Programme
CETACEAN STOCK ASSESSMENT IN RELATION TO EXPLORATION AND PRODUCTION INDUSTRY SOUND by Prepared for Joint Industry Programme 30 September 2009 LGL Report TA4582-1 CETACEAN STOCK ASSESSMENT IN RELATION TO EXPLORATION AND PRODUCTION INDUSTRY SOUND by LGL Limited, environmental research associates 22 Fisher Street, POB 280 King City, Ontario, Canada L7B 1A6 9768 Second Street Sidney, British Columbia, Canada V8L 3Y8 and LGL Alaska Research Associates Inc. 1101 East 76th Avenue, Suite B Anchorage, Alaska, United States 99518 Prepared for Joint Industry Programme 30 September 2009 LGL Report TA4582-1 Executive Summary Purpose and Objectives This project investigated the relationship between the oil industry‘s offshore E&P activities and trends in the distribution, abundance and rates of increase of key cetacean stocks found in three areas where E&P activities are intensive. The approach taken was to compare the status and population trends of stocks of key cetacean species in three areas with E&P activities―Alaska (subdivided into three regions, the Beaufort, Bering and Chukchi seas), Australia (Western and southeast regions), and Sakhalin Island, Russia―with corresponding parameters for stocks of the same species (where possible) in areas where E&P activities were absent or greatly reduced. The project involved a critical review of existing and historical data on cetacean stocks, and a compilation of data on E&P activities and non-industry factors that may have influenced stocks, in the areas of interest. Data were assessed in terms of quality, quantity, and temporal and spatial coverage to determine whether sufficient data were available for a reasonable assessment of correlations between cetacean populations and E&P activities. -
Soliton and Some of Its Geophysical/Oceanographic Applications
Introduction Historical KdV equation Other equations Theory Applications Higher dimensions Problems Soliton and Some of its Geophysical/Oceanographic Applications M. Lakshmanan Centre for Nonlinear Dynamics Bharathidasan University Tiruchirappalli – 620024 India Discussion Meeting, ICTS-TIFR 21 July 2016 M. Lakshmanan Soliton and Some of its Geophysical Introduction Historical KdV equation Other equations Theory Applications Higher dimensions Problems Theme Soliton is a counter-intuitive wave entity arising because of a delicate balance between dispersion and nonlinearity. Its major attraction is its localized nature, finite energy and preservation of shape under collision = a remark- ably stable structure. Consequently, it has⇒ ramifications in as wider areas as hydrodynamics, tsunami dynamics, condensed matter, magnetism, particle physics, nonlin- ear optics, cosmology and so on. A brief overview will be presented with emphasis on oceanographic applications and potential problems will be indicated. M. Lakshmanan Soliton and Some of its Geophysical Introduction Historical KdV equation Other equations Theory Applications Higher dimensions Problems Plan 1 Introduction 2 Historical: (i) Scott-Russel (ii) Zabusky/Kruskal 3 Korteweg-de Vries equation and solitary wave/soliton 4 Other ubiquitous equations 5 Mathematical theory of solitons 6 Geophysical/Oceanographic applications 7 Solitons in higher dimensions 8 Problems and potentialities M. Lakshmanan Soliton and Some of its Geophysical Introduction Historical KdV equation Other equations Theory -
Sakhalin-1 Project Report on Environmental Protection Activities
SAKHALIN-1 PROJECT REPORT ON ENVIRONMENTAL PROTECTION ACTIVITIES EXXON NEFTEGAS LIMITED 2017 Report on ENL Environmental Protection Activities in 2017 Sakhalin-1 Project Table of Contents 1. Health, Safety, and Environmental Protection in 2017 .………………………………………3 2. 2017 Environmental Performance………...…………………………………..………………..3 2.1 Waste management ….………………………………………………………………..3 2.2 Water use, water consumption, and wastewater disposal …………………………8 2.3 Air emissions ……………………………………………………………………………9 2.4 Oil/Products spill response activities ….…………………………………………….11 2.5 Purchasing emergency response equipment (OSR, fire and rescue equipment) 14 2.6 Expenditures for environmental protection ……………… …………………….…..15 2.7 Payments for the use of natural resources ……………..……………………….…...15 3. Key Environmental Protection and Environmental Monitoring Programs …...…………….16 3.1 Pipeline right-of-way repair and maintenance ……………………………………....16 3.2 Environmental monitoring and in-process oversight ………………………………16 3.3 Environmental monitoring and in-process oversight results in 2017 .……………19 3.4 Key environmental protection programs ……………………………………………25 3.5 Compensation for damage to aquatic biological resources ….……………………28 Attachment: ENL’s SSHE performance in 2014-2017. 2 Report on ENL Environmental Protection Activities in 2017 Sakhalin-1 Project 1. HEALTH, SAFETY, AND ENVIRONMENTAL PROTECTION IN 2017. In 2017 Exxon Neftegas Limited conducted the following major activities to develop a culture of safety, health, and environmental protection: ♦ Promotion of safety -
Dissipative Cnoidal Waves (Turing Rolls) and the Soliton Limit in Microring Resonators
Research Article Vol. X, No. X / Febrary 1046 B.C. / OSA Journal 1 Dissipative cnoidal waves (Turing rolls) and the soliton limit in microring resonators ZHEN QI1,*,S HAOKANG WANG1,J OSÉ JARAMILLO-VILLEGAS2,M INGHAO QI3, ANDREW M. WEINER3,G IUSEPPE D’AGUANNO1,T HOMAS F. CARRUTHERS1, AND CURTIS R. MENYUK1 1University of Maryland at Baltimore County, 1000 Hilltop Circle, Baltimore, MD 21250, USA 2Technological University of Pereira, Cra. 27 10-02, Pereira, Risaralda 660003, Colombia 3Purdue University, 610 Purdue Mall, West Lafayette, IN 47907, USA *Corresponding author: [email protected] Compiled May 27, 2019 Single solitons are a special limit of more general waveforms commonly referred to as cnoidal waves or Turing rolls. We theoretically and computationally investigate the stability and acces- sibility of cnoidal waves in microresonators. We show that they are robust and, in contrast to single solitons, can be easily and deterministically accessed in most cases. Their bandwidth can be comparable to single solitons, in which limit they are effectively a periodic train of solitons and correspond to a frequency comb with increased power. We comprehensively explore the three-dimensional parameter space that consists of detuning, pump amplitude, and mode cir- cumference in order to determine where stable solutions exist. To carry out this task, we use a unique set of computational tools based on dynamical system theory that allow us to rapidly and accurately determine the stable region for each cnoidal wave periodicity and to find the instabil- ity mechanisms and their time scales. Finally, we focus on the soliton limit, and we show that the stable region for single solitons almost completely overlaps the stable region for both con- tinuous waves and several higher-periodicity cnoidal waves that are effectively multiple soliton trains. -
Routes and Intensity of Geese Migration Over Northern Sakhalin and the Mainland Part of Tatar Strait I
ISSN 10674136, Russian Journal of Ecology, 2011, Vol. 42, No. 2, pp. 151–160. © Pleiades Publishing, Ltd., 2011. Original Russian Text © I. M. Tiunov, A. Yu. Blokhin, P. A. Faiman, 2011, published in Ekologiya, 2011, No. 2, pp. 134–143. Routes and Intensity of Geese Migration over Northern Sakhalin and the Mainland Part of Tatar Strait I. M. Tiunova, A. Yu. Blokhinb, and P. A. Faimanc aInstitute of Biology and Soil Sciences, Far East Branch, Russian Academy of Sciences, pr. Stoletiya Vladivostoka 159, Vladivostok, 690022 Russia; email: [email protected] bSakhalin Ecological Company, ul. Rozhdestvenskaya 63, YuzhnoSakhalinsk, 693007 Russia cResearch Institute for Applied Mechanics, 61 Kasuga, Fukuoka, 8168580 Japan Received March 26, 2010 Abstract—The intensity of geese migration has increased since 2005, and its routes have shifted eastward. The main migration route of the geese previously passed over the northwestern Sea of Okhotsk, far from the coast; since 2005, however, a major migration flow has been recorded over northern Sakhalin and the main land part of Tatar Strait. A probable factor accounting for this shift is a change in weather conditions and, in particular, in the circulation of air masses over the northwestern Sea of Okhotsk. Keywords: geese, migration, flight dates, numbers, northern Sakhalin, Tatar Strait. DOI: 10.1134/S1067413611010139 Sakhalin Island is located on the East Asian–Aus and on the mainland coast of Nevelskoy Strait tralasian flyway. Its diverse and extensive wetlands and between the village of DeKastri to the Tymi River on coastal biotopes offer a major resting and feeding stop the north, mainly in autumn, in 2001–1008 (Fig. -
Three-Dimensional Dynamics of Baroclinic Tides Over a Seamount
University of Plymouth PEARL https://pearl.plymouth.ac.uk Faculty of Science and Engineering School of Biological and Marine Sciences 2018-02 Three-dimensional dynamics of baroclinic tides over a seamount Vlasenko, V http://hdl.handle.net/10026.1/10845 10.1002/2017JC013287 Journal of Geophysical Research: Oceans American Geophysical Union All content in PEARL is protected by copyright law. Author manuscripts are made available in accordance with publisher policies. Please cite only the published version using the details provided on the item record or document. In the absence of an open licence (e.g. Creative Commons), permissions for further reuse of content should be sought from the publisher or author. JOURNAL OF GEOPHYSICAL RESEARCH, VOL. ???, XXXX, DOI:10.1002/, Three-dimensional dynamics of baroclinic tides over a seamount 1 1 1 Vasiliy Vlasenko , Nataliya Stashchuk , and W. Alex M. Nimmo-Smith Vasiliy Vlasenko, School of Biological and Marine Sciences, Plymouth University, Plymouth, PL4 8AA, UK ([email protected]) 1School of Biological and Marine Sciences, Plymouth University, Plymouth, PL4 8AA, UK. D R A F T January 17, 2018, 10:45am D R A F T X-2 VLASENKO ET AL.: BAROCLINIC TIDES OVER A SEAMOUNT 1 Abstract. 2 The Massachusetts Institute of Technology general circulation model is used 3 for the analysis of baroclinic tides over Anton Dohrn Seamount (ADS), in 4 the North Atlantic. The model output is validated against in-situ data col- 5 lected during the 136-th cruise of the RRS “James Cook” in May-June 2016. 6 The observational data set includes velocity time series recorded at two moor- 7 ings as well as temperature, salinity and velocity profiles collected at 22 hy- 8 drological stations. -
Plasmon-Soliton
Plasmon-Soliton Eyal Feigenbaum and Meir Orenstein Department of Electrical Engineering, Technion, Haifa 32000, Israel [email protected] Abstract : Formation of a novel hybrid-vector spatial plasmon-soliton in a Kerr slab embedded in-between metal plates is predicted and analyzed with a modified NLSE, encompassing hybrid vector field characteristics. Assisted by the transverse plasmonic effect, the self trapping dimension of the plasmon-soliton was substantially compressed (compared to the dielectrically cladded slab case) when reducing the slab width. The practical limitation of the Plasmon-soliton size reduction is determined by available nonlinear materials and metal loss. For the extreme reported values of nonlinear index change, we predict soliton with a cross section of 300nm×30nm (average dimension of 100nm). 1 The downscaling of conventional photonics is halted when approaching a transverse dimension of ~ λ/2 ( λ is the wavelength). This limitation can be alleviated by the incorporation of metals, giving rise to surface plasmon polaritons (SPP) [1,2]. Here we analyze a novel configuration where light is transversely tightly guided between two metal layers, and laterally self trapped by a nonlinear Kerr effect to yield a plasmon-soliton. The tight field confinement of this scheme is important for potential excitation of plasmon-solitons by a low power continuous wave optical source, which is further assisted by the expected small group velocity of the plasmon-soliton. In this letter we present for the first time both an analysis of TM spatial solitons, using the Non- linear Schrödinger Equation (NLSE), where the full vectorial field is considered, as well as the prediction and characteristics of SPP based solitons. -
Environmental Management and Environmental Protection Policy
ENVIRONMENTAL MANAGEMENT AND ENVIRONMENTAL PROTECTION POLICY EXXON NEFTEGAS LIMITED SAKHALIN-1 PROJECT OPERATOR ExxonMobil Corporation Subsidiary 2019 Environmental Management and Sakhalin-1 Project Environmental Protection Policy. Contents 1 Introduction .................................................................................................................. 1-3 2 Operations Integrity Management System .................................................................... 2-4 3 Environmental management ......................................................................................... 3-6 4 ENL environmental protection policy ............................................................................ 4-8 5 Comprehensive assessment of Sakhalin-1 Project potential environmental, socioeconomic, and public health impact ................................................................... 5-10 6 Potential environmental impact prevention and mitigation .......................................... 6-12 6.1 Air Quality Protection ...................................................................................... 6-12 6.2 Protection of Surface Water ............................................................................ 6-13 6.3 Protection Against Physical Factors ................................................................ 6-14 6.4 Protection of the Geological Environment ....................................................... 6-14 6.5 Reducing Natural Landscape Fragmentation, Soil Protection, and Land Remediation ..................................................................................................