Wave Hydrodynamics Dr. R N Sankhua Prologue Wind Blowing
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Downloaded 09/24/21 11:26 AM UTC 966 JOURNAL of PHYSICAL OCEANOGRAPHY VOLUME 46
MARCH 2016 G R I M S H A W E T A L . 965 Modelling of Polarity Change in a Nonlinear Internal Wave Train in Laoshan Bay ROGER GRIMSHAW Department of Mathematical Sciences, Loughborough University, Loughborough, United Kingdom CAIXIA WANG AND LAN LI Physical Oceanography Laboratory, Ocean University of China, Qingdao, China (Manuscript received 23 July 2015, in final form 29 December 2015) ABSTRACT There are now several observations of internal solitary waves passing through a critical point where the coefficient of the quadratic nonlinear term in the variable coefficient Korteweg–de Vries equation changes sign, typically from negative to positive as the wave propagates shoreward. This causes a solitary wave of depression to transform into a train of solitary waves of elevation riding on a negative pedestal. However, recently a polarity change of a different kind was observed in Laoshan Bay, China, where a periodic wave train of elevation waves converted to a periodic wave train of depression waves as the thermocline rose on a rising tide. This paper describes the application of a newly developed theory for this phenomenon. The theory is based on the variable coefficient Korteweg–de Vries equation for the case when the coefficient of the quadratic nonlinear term undergoes a change of sign and predicts that a periodic wave train will pass through this critical point as a linear wave, where a phase change occurs that induces a change in the polarity of the wave, as observed. A two-layer model of the density stratification and background current shear is developed to make the theoretical predictions specific and quantitative. -
Part II-1 Water Wave Mechanics
Chapter 1 EM 1110-2-1100 WATER WAVE MECHANICS (Part II) 1 August 2008 (Change 2) Table of Contents Page II-1-1. Introduction ............................................................II-1-1 II-1-2. Regular Waves .........................................................II-1-3 a. Introduction ...........................................................II-1-3 b. Definition of wave parameters .............................................II-1-4 c. Linear wave theory ......................................................II-1-5 (1) Introduction .......................................................II-1-5 (2) Wave celerity, length, and period.......................................II-1-6 (3) The sinusoidal wave profile...........................................II-1-9 (4) Some useful functions ...............................................II-1-9 (5) Local fluid velocities and accelerations .................................II-1-12 (6) Water particle displacements .........................................II-1-13 (7) Subsurface pressure ................................................II-1-21 (8) Group velocity ....................................................II-1-22 (9) Wave energy and power.............................................II-1-26 (10)Summary of linear wave theory.......................................II-1-29 d. Nonlinear wave theories .................................................II-1-30 (1) Introduction ......................................................II-1-30 (2) Stokes finite-amplitude wave theory ...................................II-1-32 -
Title Relation Between Wave Characteristics of Cnoidal Wave
Relation between Wave Characteristics of Cnoidal Wave Title Theory Derived by Laitone and by Chappelear Author(s) YAMAGUCHI, Masataka; TSUCHIYA, Yoshito Bulletin of the Disaster Prevention Research Institute (1974), Citation 24(3): 217-231 Issue Date 1974-09 URL http://hdl.handle.net/2433/124843 Right Type Departmental Bulletin Paper Textversion publisher Kyoto University Bull. Disas. Prey. Res. Inst., Kyoto Univ., Vol. 24, Part 3, No. 225,September, 1974 217 Relation between Wave Characteristics of Cnoidal Wave Theory Derived by Laitone and by Chappelear By Masataka YAMAGUCHIand Yoshito TSUCHIYA (Manuscriptreceived October5, 1974) Abstract This paper presents the relation between wave characteristicsof the secondorder approxi- mate solutionof the cnoidal wave theory derived by Laitone and by Chappelear. If the expansionparameters Lo and L3in the Chappeleartheory are expanded in a series of the ratio of wave height to water depth and the expressionsfor wave characteristics of the secondorder approximatesolution of the cnoidalwave theory by Chappelearare rewritten in a series form to the second order of the ratio, the expressions for wave characteristics of the cnoidalwave theory derived by Chappelearagree exactly with the ones by Laitone, whichare convertedfrom the depth below the wave trough to the mean water depth. The limitingarea betweenthese theories for practical applicationis proposed,based on numerical comparison. In addition, somewave characteristicssuch as wave energy, energy flux in the cnoidal waves and so on are calculated. 1. Introduction In recent years, the various higher order solutions of finite amplitude waves based on the perturbation method have been extended with the progress of wave theories. For example, systematic deviations of the cnoidal wave theory, which is a nonlinear shallow water wave theory, have been made by Kellern, Laitone2), and Chappelears> respectively. -
Spectral Analysis
Ocean Environment Sep. 2014 Kwang Hyo Jung, Ph.D Assistant Professor Dept. of Naval Architecture & Ocean Engineering Pusan National University Introduction Project Phase and Functions Appraise Screen new development development Identify Commence basic Complete detail development options options & define Design & define design & opportunity & Data acquisition base case equipment & material place order LLE Final Investment Field Feasibility Decision Const. and Development Pre-FEED FEED Detail Eng. Procurement Study Installation Planning (3 - 5 M) (6 - 8 M) (33 - 36 M) 1st Production 45/40 Tendering for FEED Tendering for EPCI Single Source 30/25 (4 - 6 M) (11 - 15 M) Design Competition 20/15 15/10 0 - 10/- 5 - 15/-10 - 25/-15 Cost Estimate Accuracy (%) EstimateAccuracy Cost - 40/- 25 Equipment Bills of Material & Concept options Process systems & Material Purchase order & Process blocks defined Definition information Ocean Water Properties Density, Viscosity, Salinity and Temperature Temperature • The largest thermocline occurs near the water surface. • The temperature of water is the highest at the surface and decays down to nearly constant value just above 0 at a depth below 1000 m. • This decay is much faster in the colder polar region compared to the tropical region and varies between the winter and summer seasons. Salinity • The variation of salinity is less profound, except near the coastal region. • The river run-off introduces enough fresh water in circulation near the coast producing a variable horizontal as well as vertical salinity. • In the open sea. the salinity is less variable having an average value of about 35 ‰ (permille, parts per thousand). Viscosity • The dynamic viscosity may be obtained by multiplying the viscosity with mass density. -
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. -
Variational of Surface Gravity Waves Over Bathymetry BOUSSINESQ
Gert Klopman Variational BOUSSINESQ modelling of surface gravity waves over bathymetry VARIATIONAL BOUSSINESQ MODELLING OF SURFACE GRAVITY WAVES OVER BATHYMETRY Gert Klopman The research presented in this thesis has been performed within the group of Applied Analysis and Mathematical Physics (AAMP), Department of Applied Mathematics, Uni- versity of Twente, PO Box 217, 7500 AE Enschede, The Netherlands. Copyright c 2010 by Gert Klopman, Zwolle, The Netherlands. Cover design by Esther Ris, www.e-riswerk.nl Printed by W¨ohrmann Print Service, Zutphen, The Netherlands. ISBN 978-90-365-3037-8 DOI 10.3990/1.9789036530378 VARIATIONAL BOUSSINESQ MODELLING OF SURFACE GRAVITY WAVES OVER BATHYMETRY PROEFSCHRIFT ter verkrijging van de graad van doctor aan de Universiteit Twente, op gezag van de rector magnificus, prof. dr. H. Brinksma, volgens besluit van het College voor Promoties in het openbaar te verdedigen op donderdag 27 mei 2010 om 13.15 uur door Gerrit Klopman geboren op 25 februari 1957 te Winschoten Dit proefschrift is goedgekeurd door de promotor prof. dr. ir. E.W.C. van Groesen Aan mijn moeder Contents Samenvatting vii Summary ix Acknowledgements x 1 Introduction 1 1.1 General .................................. 1 1.2 Variational principles for water waves . ... 4 1.3 Presentcontributions........................... 6 1.3.1 Motivation ............................ 6 1.3.2 Variational Boussinesq-type model for one shape function .. 7 1.3.3 Dispersionrelationforlinearwaves . 10 1.3.4 Linearwaveshoaling. 11 1.3.5 Linearwavereflectionbybathymetry . 12 1.3.6 Numerical modelling and verification . 14 1.4 Context .................................. 16 1.4.1 Exactlinearfrequencydispersion . 17 1.4.2 Frequency dispersion approximations . 18 1.5 Outline ................................. -
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. -
Comparison of Various Spectral Models for the Prediction of the 100-Year Design Wave Height
MATEC Web of Conferences 203, 01020 (2018) https://doi.org/10.1051/matecconf/201820301020 ICCOEE 2018 Comparison of Various Spectral Models for the Prediction of the 100-Year Design Wave Height Sayyid Zainal Abidin Syed Ahmad1, 2,*, Mohd Khairi Abu Husain1, Noor Irza Mohd Zaki1, Mohd Hairil Mohd2 and Gholamhossein Najafian3 1Universiti Teknologi Malaysia, 54100 Kuala Lumpur, Malaysia 2Universiti Malaysia Terengganu, 21030 Kuala Nerus, Malaysia 3School of Engineering, Universiti of Liverpool, Liverpool, United Kingdom Abstract. Offshore structures are exposed to random wave loading in the ocean environment, and hence the probability distribution of the extreme values of their response to wave loading is required for their safe and economical design. In most cases, the dominant load on offshore structures is due to wind-generated random waves where the ocean surface elevation is defined using appropriate ocean wave energy spectra. Several spectral models have been proposed to describe a particular sea state that is used in the design of offshore structures. These models are derived from analysis of observed ocean waves and are thus empirical in nature. The spectral models popular in the offshore industry include Pierson-Moskowitz spectrum and JONSWAP spectrum. While the offshore industry recognizes that different methods of simulating ocean surface elevation lead to different estimation of design wave height, no systematic investigation has been conducted. Hence, the aim of this study is to investigate the effects of predicting the 100-year responses from various wave spectrum models. In this paper, the Monte Carlo time simulation (MCTS) procedure has been used to compare the magnitude of the 100-year extreme responses derived from different spectral models. -
11 Ardhuin CLIVAR Stokesdrift
Stokes drift and vertical shear at the sea surface: upper ocean transport, mixing, remote sensing Fabrice Ardhuin (SIO/MPL) Adapted from Sutherland et al. (JPO 2016) (26 N, 36 W) Stokes drift | CLIVAR surface current workshop | F. Ardhuin | Slide 1 1. Oscillating motions can transport mass… Linear Airy wave theory, monochromatic waves in deep water - Phase speed: C ~ 10 m/s Quadratic quantities: - Orbital velocity: u =(ak) C ~ 1 m/s , Wave energy: E = ⍴g a2/2 [J/m2] 2 - Stokes drift: US =(ak) C ~ 0.1 m/s , Mass transport: Mw = E/C [kg/m/s] (depth integrated. Mw =E/C is very general) linear Eulerian velocity non-linear Eulerian velocity Eulerian mean velocity horizontal displacement vertical displacement Lagragian mean velocity same transport Stokes drift | CLIVAR surface current workshop | F. Ardhuin | Slide 2 2. Beyond simple waves - Non-linear effects: limited for monochromatic waves in deep water - Random waves: Kenyon (1969) ESA (2019, SKIM RfMS) Rascle et al. (JGR 2006) Stokes drift | CLIVAR surface current workshop | F. Ardhuin | Slide 3 2. Beyond simple waves - Random waves (continued): it is not just the wind : average Us for 5 to 10 m/s is 20% higher at PAPA (data courtesy J. Thomson / CDIP) compared to East Atlantic buoy 62069. Up to 0.5 Hz Up to 0.5 Hz Stokes drift | CLIVAR surface current workshop | F. Ardhuin | Slide 4 2. Beyond simple waves … and context Now compared to PAPA currents (courtesy of Cronin et al. PMEL) Stokes drift | CLIVAR surface current workshop | F. Ardhuin | Slide 5 2. Beyond simple waves -Nonlinear random waves …? harmonics, modulation … -Breaking: Pizzo et al. -
Mohammed and Fritz
JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 117, C11015, doi:10.1029/2011JC007850, 2012 Physical modeling of tsunamis generated by three-dimensional deformable granular landslides Fahad Mohammed1,2 and Hermann M. Fritz2 Received 21 December 2011; revised 19 September 2012; accepted 21 September 2012; published 15 November 2012. [1] Tsunamis generated by deformable granular landslides are physically modeled in a three-dimensional tsunami wave basin based on the generalized Froude similarity. The dynamic landslide impact characteristics were controlled by means of a novel pneumatic landslide generator. The wave amplitudes, periods, and wavelengths are related to the landslide parameters at impact with the landslide Froude number being a dominant parameter. Between 1 and 15% of the landslide kinetic energy at impact is converted into the wave train energy. The wave amplitudes decay in radial and angular directions from the landslide axis. The first wave crest mostly travels with speeds close to the theoretical approximation of the solitary wave speed. The measured tsunami wave profiles were either of the nonlinear oscillatory or nonlinear transition type depending primarily on the landslide Froude number and relative slide thickness at impact. The generated waves range from shallow to deep water depth regimes, with the majority being in the intermediate water depth regime. Wave characteristics are compared with other two- and three-dimensional landslide tsunami studies and the results are discussed. Citation: Mohammed, F., and H. M. Fritz (2012), Physical modeling of tsunamis generated by three-dimensional deformable granular landslides, J. Geophys. Res., 117, C11015, doi:10.1029/2011JC007850. 1. Introduction tsunami was generated by a coastal landslide triggered by the 2010 Haiti earthquake [Fritz et al., 2012]. -
Analysis of Different Methods for Wave Generation and Absorption in a CFD-Based Numerical Wave Tank
Journal of Marine Science and Engineering Article Analysis of Different Methods for Wave Generation and Absorption in a CFD-Based Numerical Wave Tank Adria Moreno Miquel 1 ID , Arun Kamath 2,* ID , Mayilvahanan Alagan Chella 3 ID , Renata Archetti 1 ID and Hans Bihs 2 ID 1 Department of Civil, Chemical, Environmental and Materials Engineering, University of Bologna, Via Terracini 28, 40131 Bologna, Italy; [email protected] (A.M.M.); [email protected] (R.A.) 2 Department of Civil and Environmental Engineering, NTNU Trondheim, 7491 Trondheim, Norway; [email protected] 3 Department of Civil & Environmental Engineering & Earth Sciences, University of Notre Dame, Notre Dame, IN 46556, USA; [email protected] * Correspondence: [email protected] Received: 30 April 2018; Accepted: 10 June 2018; Published: 14 June 2018 Abstract: In this paper, the performance of different wave generation and absorption methods in computational fluid dynamics (CFD)-based numerical wave tanks (NWTs) is analyzed. The open-source CFD code REEF3D is used, which solves the Reynolds-averaged Navier–Stokes (RANS) equations to simulate two-phase flow problems. The water surface is computed with the level set method (LSM), and turbulence is modeled with the k-w model. The NWT includes different methods to generate and absorb waves: the relaxation method, the Dirichlet-type method and active wave absorption. A sensitivity analysis has been conducted in order to quantify and compare the differences in terms of absorption quality between these methods. A reflection analysis based on an arbitrary number of wave gauges has been adopted to conduct the study. Tests include reflection analysis of linear, second- and fifth-order Stokes waves, solitary waves, cnoidal waves and irregular waves generated in an NWT. -
Title a New Approach to Stokes Wave Theory Author(S) TSUCHIYA
Title A New Approach to Stokes Wave Theory Author(s) TSUCHIYA, Yoshito; YASUDA, Takashi Bulletin of the Disaster Prevention Research Institute (1981), Citation 31(1): 17-34 Issue Date 1981-03 URL http://hdl.handle.net/2433/124895 Right Type Departmental Bulletin Paper Textversion publisher Kyoto University Bull. Disas. Prey. Res. Inst., Kyoto Univ., Vol. 31, Part 1, No. 276, 1981 17 A New Approach to Stokes Wave Theory By Yoshito TSUCHIYA and Takashi YASUDA (Manuscript received November 28, 1980) Abstract Stokes wave theories to third-order approximation have widely been employed to calculate wave properties for waves propagating over finite depths of water in most engineering appli- cations. However, different and often inconsistent expressions of wave variables can be observed from the numerous theories available. Examinations of the usual Stokes wave theories are on the so-called Stokes definitions of wave celerity and Bernoulli constant, as well as on the physical explanations of some theo- retical problems involved. A new Stokes wave theory to third order approximation is derived by applying only necessary conditions and assumptions, without using the definitions of wave celerity. The resulting mathematical formulations for some pertinent wave variables are presented. Comparison is made between the new third-order approximation and the usual ones derived from using the Stokes definitions of wave celerity, showing different expressions of wave celerity, horizontal water particle velocity, and mass transport velocities. It is found that the mass transport velocity exists in the Eulerian description as well as the usual Stokes drift in the Lagrangian description. 1. Introductionintrodurtinn A thorough understanding of wave characteristics in shallow water is essential in estimating wave forces on structures, as well as investigating various mechanisms of wave-induced transport phenomenon, such as nearshore currents and sand drift.