International Journal of Innovative Research in Science, Engineering and Technology Vol. 2, Issue 5, May 2013



Similar documents
CHAPTER 4 4 NUMERICAL ANALYSIS

132 A. A. HASSAN AND L. N. SANKAR J. AIRCRAFT

Ravi Kumar Singh*, K. B. Sahu**, Thakur Debasis Mishra***

Manufacturing Equipment Modeling

CFD Analysis of Swept and Leaned Transonic Compressor Rotor

Unit 4 Practice Test: Rotational Motion

NUMERICAL ANALYSIS OF THE EFFECTS OF WIND ON BUILDING STRUCTURES

Copyright 2013 wolfssl Inc. All rights reserved. 2

SEISMIC RETROFITTING OF STRUCTURES

VISCOSITY OF A LIQUID. To determine the viscosity of a lubricating oil. Time permitting, the temperature variation of viscosity can also be studied.

Modeling Mechanical Systems

PHYS 101-4M, Fall 2005 Exam #3. MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

Simulation of Offshore Structures in Virtual Ocean Basin (VOB)

Numerical Modelling of Regular Waves Propagation and Breaking Using Waves2Foam

Aeroacoustic simulation based on linearized Euler equations and stochastic sound source modelling

NUMERICAL SIMULATION OF REGULAR WAVES RUN-UP OVER SLOPPING BEACH BY OPEN FOAM

Keywords: CFD, heat turbomachinery, Compound Lean Nozzle, Controlled Flow Nozzle, efficiency.

Proceedings of OMAE'01 20 th International Conference on Offshore Mechanics and Arctic Engineering June 3-8, 2001, Rio de Janeiro, Brazil

ENS 07 Paris, France, 3-4 December 2007

Precise Modelling of a Gantry Crane System Including Friction, 3D Angular Swing and Hoisting Cable Flexibility

Damage Evaluation of 500 MWe Indian Pressurized Heavy Water Reactor Nuclear Containment for Air Craft Impact

Rotation: Moment of Inertia and Torque

ENGINEERING COUNCIL DYNAMICS OF MECHANICAL SYSTEMS D225 TUTORIAL 1 LINEAR AND ANGULAR DISPLACEMENT, VELOCITY AND ACCELERATION

Dynamics of Offshore Wind Turbines

EFFECTS ON NUMBER OF CABLES FOR MODAL ANALYSIS OF CABLE-STAYED BRIDGES

Numerical Investigation of Heat Transfer Characteristics in A Square Duct with Internal RIBS

TWO-DIMENSIONAL FINITE ELEMENT ANALYSIS OF FORCED CONVECTION FLOW AND HEAT TRANSFER IN A LAMINAR CHANNEL FLOW

Harmonic oscillations of spiral springs Springs linked in parallel and in series

How To Run A Cdef Simulation

Frequency-domain and stochastic model for an articulated wave power device

DEVELOPMENT AND APPLICATIONS OF TUNED/HYBRID MASS DAMPERS USING MULTI-STAGE RUBBER BEARINGS FOR VIBRATION CONTROL OF STRUCTURES

SLANGTNG - SOFTWARE FOR STOCHASTIC STRUCTURAL ANALYSIS MADE EASY

CASE HISTORY #2. APPLICATION: Piping Movement Survey using Permalign Laser Measurement System

How to compute Random acceleration, velocity, and displacement values from a breakpoint table.

First Power Production figures from the Wave Star Roshage Wave Energy Converter

Magnetic / Gravity Loading Analysis

Dynamic Stability of Flared and Tumblehome Hull Forms in Waves

Bandwidth-dependent transformation of noise data from frequency into time domain and vice versa

CALCULATING THE RESPONSE OF AN OSCILLATOR TO ARBITRARY GROUND MOTION* By G~ORGE W. I-IouSl~ER

The Viscosity of Fluids

Numerical modeling of dam-reservoir interaction seismic response using the Hybrid Frequency Time Domain (HFTD) method

Development of New Inkjet Head Applying MEMS Technology and Thin Film Actuator

State Newton's second law of motion for a particle, defining carefully each term used.

Springs and Dampers. MCE371: Vibrations. Prof. Richter. Department of Mechanical Engineering. Handout 2 Fall 2011

Unit 3 Work and Energy Suggested Time: 25 Hours

A. Hyll and V. Horák * Department of Mechanical Engineering, Faculty of Military Technology, University of Defence, Brno, Czech Republic

Asphalt Institute Technical Bulletin. Laboratory Mixing and Compaction Temperatures

AP1 Waves. (A) frequency (B) wavelength (C) speed (D) intensity. Answer: (A) and (D) frequency and intensity.

Simulation of Trajectories and Comparison of Joint Variables for Robotic Manipulator Using Multibody Dynamics (MBD)

Waves-Wave Characteristics

Finite Element Simulation of Simple Bending Problem and Code Development in C++

FLow pattern around cable and its aerodynamic characteristics in critical Reynolds number range

Structural Axial, Shear and Bending Moments

HOOKE S LAW AND OSCILLATIONS

ANALYTICAL METHODS FOR ENGINEERS

TRAVELING WAVE EFFECTS ON NONLINEAR SEISMIC BEHAVIOR OF CONCRETE GRAVITY DAMS

Centripetal force, rotary motion, angular velocity, apparent force.

THE DETERMINATION OF DELAMINATION STRAIN ENERGY RELEASE RATE OF COMPOSITE BI-MATERIAL INTERFACE

SOLUTIONS TO CONCEPTS CHAPTER 15

Introduction to Engineering System Dynamics

Aeroelastic models for wind turbines

Soil Dynamics Prof. Deepankar Choudhury Department of Civil Engineering Indian Institute of Technology, Bombay

A Cost- Effective Computational Tool for Offshore Floater Design

Automatic Detection of Emergency Vehicles for Hearing Impaired Drivers

Overset Grids Technology in STAR-CCM+: Methodology and Applications

The Viscosity of Fluids

Solved with COMSOL Multiphysics 4.3

Lab 8: DC generators: shunt, series, and compounded.

Application of the Pareto Principle in Rapid Application Development Model

HW Set VI page 1 of 9 PHYSICS 1401 (1) homework solutions

Simulation of Flow Field and Particle Trajectories in Hard Disk Drive Enclosures

Detection of Heart Diseases by Mathematical Artificial Intelligence Algorithm Using Phonocardiogram Signals

Performance Analysis of AQM Schemes in Wired and Wireless Networks based on TCP flow

AP1 Oscillations. 1. Which of the following statements about a spring-block oscillator in simple harmonic motion about its equilibrium point is false?

DESIGN AND ANALYSIS OF KINETIC ENERGY RECOVERY SYSTEM IN BICYCLES

MATERIALS. Multisim screen shots sent to TA.

State Newton's second law of motion for a particle, defining carefully each term used.

Lab 1: Introduction to PSpice

Study of the Stability of Turret moored Floating Body

Design and Analysis of Engine Cooling Fan

Experiment 4 ~ Newton s Second Law: The Atwood Machine

CFD SUPPORTED EXAMINATION OF BUOY DESIGN FOR WAVE ENERGY CONVERSION

. Address the following issues in your solution:

Navier-Stokes Equation Solved in Comsol 4.1. Copyright Bruce A. Finlayson, 2010 See also Introduction to Chemical Engineering Computing, Wiley (2006).

Master s Program Requirements. Industrial & Systems Engineering at Texas A&M University. Since Fall 2014.

Analysis of the Response Under Live Loads of Two New Cable Stayed Bridges Built in Mexico

Face detection is a process of localizing and extracting the face region from the

both double. A. T and v max B. T remains the same and v max doubles. both remain the same. C. T and v max

Designer-Oriented Electric Field Analysis System for Power Cable Accessories

Using CFD to improve the design of a circulating water channel

FRENIC5000MS5 for Machine Tool Spindle Drives

Application of CFD Simulation in the Design of a Parabolic Winglet on NACA 2412

Vibrations of a Free-Free Beam

Analysis of Wing Leading Edge Data. Upender K. Kaul Intelligent Systems Division NASA Ames Research Center Moffett Field, CA 94035

Transcription:

ISSN: 2319-8753 International Journal of Innovative Research in Science, Engineering and Technology Vol. 2, Issue 5, May 2013 of vibration are 0.14 rad/s and 0.42 rad/s respectively. The dynamic response of double hinged articulated loading platform is obtained under regular wave without current forces with the use of Airy linear wave theory as well as the Stokes nonlinear wave theory. Two sea states are hereby considered for (H = 10m, T = 10s) and (H = 15m, T = 15s). The sea is simulated for the duration of one hour. It is important to mention here that simulated length excludes the initial transient non stationary phase of the responses due to initial conditions. V. SIMULATION RESULTS The response of deck displacement, lower and upper hinge rotation, base and upper hinge shear for ALP under 10 m/10 s waves without current velocity is plotted. Fig. 2 show the response of deck displacement; Figs. 3-4 show the response of lower and upper hinge rotation; Figs. 5-6 show the response of base and upper hinge shear. Deck displacement (m) 0.6 0.4 0.2 1E-15-0.2-0.4-0.6-0.8 Fig. 2. Deck displacement response of ALP (10 m/10 s) Bottom hinge rotation (rad) It is seen from the plotted graphs that the maximum positive response obtained using Stokes fifth order nonlinear wave theory is less than those obtained from Airy s linear wave theory with the Chakrabarti s modification. 1.50E-03 1.00E-03 5.00E-04 1.00E-17-5.00E-04-1.00E-03-1.50E-03-2.00E-03 Upper hinge rotation (rad) Fig. 3. Bottom hinge rotation response of ALP (10 m/10 s) 1.00E-03 5.00E-04-5.00E-04-1.00E-03-1.50E-03 Fig. 4. Upper hinge rotation response of ALP (10 m/10 s) The Table 1 shows the comparative statistical response obtained by both the theories in terms of mean, standard deviation, maximum and minimum values for 10m/10s waves without current forces. Copyright to IJIRSET www.ijirset.com 1536

ISSN: 2319-8753 International Journal of Innovative Research in Science, Engineering and Technology Vol. 2, Issue 5, May 2013 Base hinge shear (N) 1.50E+07 1.00E+07 5.00E+06-5.00E+06-1.00E+07-1.50E+07 Fig. 5. Base hinge shear response of ALP (10 m/10 s) Upper hinge shear (N) 1.50E+07 1.00E+07 5.00E+06-5.00E+06-1.00E+07-1.50E+07 Fig. 6. Upper hinge shear response of ALP (10 m/10 s) The response of deck displacement, lower hinge rotation, upper hinge rotation, base hinge shear and upper hinge shear for ALP under 15 m/15 s waves without current velocity is plotted. Fig. 7 show the response of deck displacement; Figs. 8-9 show the response of lower and upper hinge rotation; Figs. 10-11 show the response of base and upper hinge shear. Deck displacement (m) 3 2 1 0-1 -2 Bottom hinge rotation (rad) Fig. 7. Deck displacement response of ALP (15 m/15 s) 8.00E-03 4.00E-03-4.00E-03-8.00E-03 Fig. 8. Bottom hinge rotation response of ALP (15 m/15 s) Copyright to IJIRSET www.ijirset.com 1537

ISSN: 2319-8753 International Journal of Innovative Research in Science, Engineering and Technology Upper hinge rotation (rad) Vol. 2, Issue 5, May 2013 2.00E-02 1.50E-02 1.00E-02 5.00E-03 1.00E-17-5.00E-03-1.00E-02-1.50E-02 Fig. 9. Upper hinge rotation response of ALP (15 m/15 s) Base hinge shear (N) 4.00E+07 2.00E+07-2.00E+07-4.00E+07 Fig. 10. Base hinge shear response of ALP (15 m/15 s) Upper hinge shear (N) 4.00E+07 2.00E+07-2.00E+07-4.00E+07 Fig. 11. Upper hinge shear response of ALP (15 m/15 s) The Table 2 shows the comparative statistical response obtained by both the theories in terms of mean, standard deviation, maximum and minimum values for 15m/15s waves without current forces. VI. CONCLUSIONS Based on the performed analytical studies, the following conclusions are drawn: 1. The response obtained using Stokes s nonlinear wave theory for the hydrodynamic case of 10m/10s waves without current forces are lesser by 57.7%, 46.8%, 65.6%, 50% and 47.5% for deck displacement, bottom hinge rotation, upper hinge rotation, base hinge shear and upper hinge shear respectively in comparision to that obtained by using Airy s linear wave theory with Chakrabarti s modifications. 2. The response obtained using Stokes s nonlinear wave theory for the hydrodynamic case of 15m/15s waves without current forces are lesser by 20.9%, 13.2%, 16.4%, 22.2% and 22.2% for deck displacement, bottom hinge rotation, upper hinge rotation, base hinge shear and upper hinge shear respectively in comparision to that obtained by using Airy s linear wave theory with Chakrabarti s modifications. Copyright to IJIRSET www.ijirset.com 1538