Machine Foundation Analysis VERIFICATION MANUAL REV D

Size: px
Start display at page:

Download "Machine Foundation Analysis VERIFICATION MANUAL REV D"

Transcription

1 Machine Foundation Analysis VERIFICATION MANUAL REV D TM

2 Page:2 COPYRIGHT The computer program CLOCKWORK and all associated documentation are proprietary and copyrighted products. Worldwide rights of ownership rest with NEWTONIAN MACHINES. Unlicensed use of the program or reproduction of the documentation in any form, without prior written authorization from NEWTONIAN MACHINES is explicitly prohibited. NEWTONIAN MACHINES ANDRÉS DE FUENZALIDA 147 PROVIDENCIA, SANTIAGO, CHILE Tel: (+56 2) contact@newtonianmachines.com Web:

3 Page:3 CONTENT I. INTRODUCTION TEST CASE TEST CASE TEST CASE TEST CASE TEST CASE

4 Page:4 I. INTRODUCTION Clockwork is a foundation design and analysis software, based on well-known and internationally accepted theories. This document provides example problems from recognized publications in order to verify the achievement of accuracy and acceptable results. However and by the nature of this software, it is difficult to find suitable examples for this verification manual since most publications are conceived to be a guide for engineers by doing hand calculations, aside from the laborious task that it is for example calculate a structure with six degree of freedom, natural frequencies for a coupled system, intricate periodic loads, etc. The analyzed tests in this manual are just a small part of the rigorous tests that our developers run in the testing stage to ensure the quality of Clockwork.

5 Page:5 1. TEST CASE 1 Dynamic load of single-cylinder compressor. a. Overview Reference: [1] Foundation Vibration Analysis Using Simple Physical Models, John P. Wolf, pg. 56., ISBN: Dynamic Load Type: Periodic Excitation Units: tonnef / m b. Problem Description On a rigid block foundation rests a reciprocating machine composed of a compressor and a driving motor, which generates a vertical unbalanced dynamic load with two components. The first component acts at a frequency of 9Hz and the second component at twice this frequency. The resulting dynamic total load it is represented by P(t) (Fig.1.1). c. Input Parameters Compressor and driving motor mass = Dynamic Load Total load acts vertically on the foundation block. Total Load P(t) = Total Load Operation Frequency = 9 Hz Number of terms used in Fourier Series = 20 Fig. 1.1 Dynamic total load from vertical single-cylinder compressor.

6 Page:6 Rigid Foundation Block Size Length = 2.0 m Width = 1.5 m Height = 1.0 m Soil Poisson s Ratio µ = 0.33 Specific Mass Density ρ = d. Analysis Shear Modulus G = For this analysis the Cone method it is used in Clockwork. e. Results Comparison Measured Value Clockwork Displacement Ref[1] Displacement [mm] [mm] Lower Peak ± * Higher Peak ± * * Displacement value from Fig. XX [1] Fig1.2 - Dynamic vertical displacement from Clockwork results.

7 Page:7 2. TEST CASE 2 Dynamic load of weaver s loom. a. Overview Reference: [1] Foundation Vibration Analysis Using Simple Physical Models, John P. Wolf, pg. 56, ISBN: Dynamic Load Type: Periodic Excitation Units: tonnef / m b. Problem Description On a rigid block foundation rests a weaver s loom operating at 9Hz with a mass of 2750kg. In this case the load is expressed as a Fourier series with 20 terms (Fig 2.1). c. Input Parameters Weaver s loom mass = Dynamic Load Load acts vertically on the foundation block. Vertical Load P(t) Fig 2.1 Dynamic vertical load from weaver s loom. Load Operation Frequency = 9 Hz up to 180 Hz Number of terms used in Fourier Series = 20

8 Page:8 Rigid Foundation Block Size Length = 2.0 m Width = 1.5 m Height = 1.0 m Soil Poisson s Ratio µ = 0.33 Mass Density ρ = d. Analysis Shear Modulus G = For this analysis the Cone method it is used in Clockwork e. Results Comparison Measured Value Clockwork Displacement Ref[1] Displacement [mm] [mm] Lower Peak ± * Higher Peak ± * * Displacement value from Fig [1] Fig 2.2 Dynamic vertical displacement from Clockwork results.

9 Page:9 3. TEST CASE 3 Vertical single-cylinder compressor. a. Overview Reference: [2] Vibration of Soils and Foundations, F. E. Richart, Jr., pg ISBN: Dynamic Load Type: Harmonic Excitation Measured Units: lbf / ft b. Problem Description c. Input Parameters Weight * f compressor = Dynamic Load Load acts vertically on the foundation block. Vertical Load = Fig. 3.1 Dynamic vertical load Load Operation Frequency = 7.5 Hz

10 Page:10 Rigid Foundation Block Size Length = 16 ft Width = 7 ft Height = 3 ft Soil Poisson s Ratio µ = 0.33 Mass Density ρ = d. Analysis Shear Modulus G = For this analysis all available methods were used in Clockwork. e. Results Comparison Measured Clockwork Displacement Displacement Ref[2] Value [in] Zero to Peak [ft] [in]

11 Page:11 4. TEST CASE 4 a. OVERVIEW The Foundation from Fig 4.1 was subjected to six load cases in order to compare results using SAP2000 and Clockwork. Dynamic Load Type: Harmonic Excitation Units: SI Damping and Group Effect were not considered. a. PROBLEM DESCRIPTION A square foundation is loaded on one of its edges and on the geometric center of gravity of the soil contact area. b. PARAMETERS FOUNDATION PARAMETERS Number of Piles 4 Pile Diameter Foundation Height Foundation Length Foundation Width 400 mm 1000 mm 3000 mm 3000 mm Specific Weight 2500 kgf/m 3 Soil Stiffness 80 kgf/cm 2 Foundation Weight kgf PILES LOCATION X - mm Y - mm Pile Pile Pile Pile Fig 4. 1 Pile Foundation on SAP2000 CASE Location Load Location Load X Y Z tonf mm mm mm 1 X Y Z X Y Z

12 Page:12 c. RESULTS - SAP2000 v15 Measured Points Displacements Angular Displacements CASE X Y Z u1 u2 u3 θ1 θ2 θ3 mm mm mm m m m rad rad rad ,77E-04 2,29E-04 4,00E ,70E-05-1,52E ,29E-04 4,77E-04-4,00E-05-2,70E ,52E ,00E-05 4,00E-05-8,90E-05-2,40E-05-2,40E ,21E ,60E ,10E ,21E-04-1,60E-05-1,10E ,70E ,21E ,70E-05-1,52E ,21E ,70E ,52E ,60E-05 1,60E-05-1,70E-05-2,40E-05-2,40E ,10E ,10E ,10E ,10E ,70E RESULTS - CLOCKWORK v12 Measured Points Displacements Angular Displacements CASE X Y Z u1 u2 u3 θ1 θ2 θ3 mm mm mm m m m rad rad rad ,76E-04 2,28E-04 4,01E ,67E-05-1,52E ,28E-04 4,76E-04-4,01E-05-2,67E ,52E ,01E-05 4,01E-05-8,85E-05-2,39E-05-2,39E ,21E ,61E ,07E ,21E-04-1,61E-05-1,07E ,65E ,21E ,67E-05-1,52E ,21E ,67E ,52E ,61E-05 1,61E-05-1,65E-05-2,39E-05-2,39E ,10E ,07E ,10E ,07E ,65E Fig 4.2 Pile Foundation on Clockwork 12

13 Page:13 Porcentual Difference of Results between SAP2000 and Clockwork Measured Point Location Displacements Angular Displacements CASE X Y Z u1 u2 u3 θ1 θ2 θ3 mm mm mm m m m rad rad rad ,21% 0,44% 0,25% 0,00% 1,11% 0,00% ,44% 0,21% 0,25% 1,11% 0,00% 0,00% ,25% 0,25% 0,56% 0,42% 0,42% 0,00% ,00% 0,00% 0,62% 0,00% 2,73% 0,00% ,00% 0,00% 0,62% 2,73% 0,00% 0,00% ,00% 0,00% 2,94% 0,00% 0,00% 0,00% ,00% 0,00% 0,00% 0,00% 1,11% 0,00% ,00% 0,00% 0,00% 1,11% 0,00% 0,00% ,62% 0,62% 2,94% 0,42% 0,42% 0,00% ,00% 0,00% 0,00% 0,00% 2,73% 0,00% ,00% 0,00% 0,00% 2,73% 0,00% 0,00% ,00% 0,00% 2,94% 0,00% 0,00% 0,00%

14 Page:14 5. TEST CASE 5 a. OVERVIEW The Foundation from Fig 5.1 was subjected to six load cases in order to compare results using SAP2000 and Clockwork. Dynamic Load Type: Harmonic Excitation Units: SI Damping and Group Effect were not considered b. PROBLEM DESCRIPTION A square foundation is loaded on one of its edges and on the geometric center of gravity of the soil contact area. c. PARAMETERS FOUNDATION PARAMETERS Piles: 6 Pile Diameter: 400 mm Block 1 - Height: 1500 mm Block 1 - Length: 2000 mm Block 1 - Width: 3000 mm Block 2 - Height: 2500 mm Block 2 - Length: 3000 mm Block 2 - Width: 3000 mm Reinf. Concrete Specific Weight 2500 kgf/m 3 Peso fundación : 78,75 kgf Soil Stiffness 80 kgf/cm 2 Fig 5. 1 Pile Foundation on SAP2000 Fig 5. 2 Pile Foundation on Clockwork 12

15 Page:15 PILES LOCATION X mm Y mm CASE Location Load tonf X mm Y mm Pile 1 : Pile 2 : Pile 3 : Pile 4 : Pile 5 : Pile 6 : X Y Z X Y Z RESULTS SAP2000 v15 Measured Points Displacements Angular Displacements Caso X Y Z u1 u2 u3 θ1 θ2 θ3 mm mm mm m m m rad rad rad ,49E-04 1,57E-04 2,20E ,87E-06-6,30E ,57E-04 4,84E-04-6,00E-05-4,00E ,05E ,20E-05 6,00E-05-7,80E-05-2,80E-05-1,00E ,41E ,84E ,73E ,62E-04-1,80E-05-1,20E ,10E ,41E ,87E-06-6,30E ,62E ,00E ,05E ,84E-06 1,80E-05-1,10E-05-2,80E-05-1,00E ,37E ,73E ,44E ,20E ,10E RESULTS - CLOCKWORK v12 Measured Points Displacements Angular Displacements Caso X Y Z u1 u2 u3 θ1 θ2 θ3 mm mm mm m m m rad rad rad ,49E-04 1,57E-04 2,22E ,88E-06-6,29E ,57E-04 4,84E-04-6,01E-05-4,00E ,04E ,22E-05 6,00E-05-7,80E-05-2,76E-05-1,02E ,41E ,87E ,75E ,62E-04-1,86E-05-1,24E ,10E ,41E ,88E-06-6,29E ,62E ,00E ,04E ,87E-06 1,86E-05-1,10E-05-2,76E-05-1,02E ,37E ,75E ,43E ,24E ,10E

16 Page:16

Prob. 1 SDOF Structure subjected to Ground Shaking

Prob. 1 SDOF Structure subjected to Ground Shaking Prob. 1 SDOF Structure subjected to Ground Shaking What is the maximum relative displacement and the amplitude of the total displacement of a SDOF structure subjected to ground shaking? magnitude of ground

More information

Chapter 2: Rigid Bar Supported by Two Buckled Struts under Axial, Harmonic, Displacement Excitation..14

Chapter 2: Rigid Bar Supported by Two Buckled Struts under Axial, Harmonic, Displacement Excitation..14 Table of Contents Chapter 1: Research Objectives and Literature Review..1 1.1 Introduction...1 1.2 Literature Review......3 1.2.1 Describing Vibration......3 1.2.2 Vibration Isolation.....6 1.2.2.1 Overview.

More information

Chapter a. Spring constant, k : The change in the force per unit length change of the spring. b. Coefficient of subgrade reaction, k:

Chapter a. Spring constant, k : The change in the force per unit length change of the spring. b. Coefficient of subgrade reaction, k: Principles of Soil Dynamics 3rd Edition Das SOLUTIONS MANUAL Full clear download (no formatting errors) at: https://testbankreal.com/download/principles-soil-dynamics-3rd-editiondas-solutions-manual/ Chapter

More information

NUMERICAL MODELLING OF RUBBER VIBRATION ISOLATORS

NUMERICAL MODELLING OF RUBBER VIBRATION ISOLATORS NUMERICAL MODELLING OF RUBBER VIBRATION ISOLATORS Clemens A.J. Beijers and André de Boer University of Twente P.O. Box 7, 75 AE Enschede, The Netherlands email: c.a.j.beijers@utwente.nl Abstract An important

More information

ON THE PREDICTION OF EXPERIMENTAL RESULTS FROM TWO PILE TESTS UNDER FORCED VIBRATIONS

ON THE PREDICTION OF EXPERIMENTAL RESULTS FROM TWO PILE TESTS UNDER FORCED VIBRATIONS Transactions, SMiRT-24 ON THE PREDICTION OF EXPERIMENTAL RESULTS FROM TWO PILE TESTS UNDER FORCED VIBRATIONS 1 Principal Engineer, MTR & Associates, USA INTRODUCTION Mansour Tabatabaie 1 Dynamic response

More information

CIVL 8/7117 Chapter 12 - Structural Dynamics 1/75. To discuss the dynamics of a single-degree-of freedom springmass

CIVL 8/7117 Chapter 12 - Structural Dynamics 1/75. To discuss the dynamics of a single-degree-of freedom springmass CIV 8/77 Chapter - /75 Introduction To discuss the dynamics of a single-degree-of freedom springmass system. To derive the finite element equations for the time-dependent stress analysis of the one-dimensional

More information

Structural Dynamics Lecture 2. Outline of Lecture 2. Single-Degree-of-Freedom Systems (cont.)

Structural Dynamics Lecture 2. Outline of Lecture 2. Single-Degree-of-Freedom Systems (cont.) Outline of Single-Degree-of-Freedom Systems (cont.) Linear Viscous Damped Eigenvibrations. Logarithmic decrement. Response to Harmonic and Periodic Loads. 1 Single-Degreee-of-Freedom Systems (cont.). Linear

More information

Active Impact Sound Isolation with Floating Floors. Gonçalo Fernandes Lopes

Active Impact Sound Isolation with Floating Floors. Gonçalo Fernandes Lopes Active Impact Sound Isolation with Floating Floors Gonçalo Fernandes Lopes Outubro 009 Active impact sound isolation with floating floors Abstract The users of buildings are, nowadays, highly demanding

More information

Chapter 14 Oscillations. Copyright 2009 Pearson Education, Inc.

Chapter 14 Oscillations. Copyright 2009 Pearson Education, Inc. Chapter 14 Oscillations 14-1 Oscillations of a Spring If an object vibrates or oscillates back and forth over the same path, each cycle taking the same amount of time, the motion is called periodic. The

More information

Dynamics of structures

Dynamics of structures Dynamics of structures 2.Vibrations: single degree of freedom system Arnaud Deraemaeker (aderaema@ulb.ac.be) 1 Outline of the chapter *One degree of freedom systems in real life Hypothesis Examples *Response

More information

Vibrations Qualifying Exam Study Material

Vibrations Qualifying Exam Study Material Vibrations Qualifying Exam Study Material The candidate is expected to have a thorough understanding of engineering vibrations topics. These topics are listed below for clarification. Not all instructors

More information

Structural System, Machines and Load Cases

Structural System, Machines and Load Cases Machine-Induced Vibrations Machine-Induced Vibrations In the following example the dynamic excitation of two rotating machines is analyzed. A time history analysis in the add-on module RF-DYNAM Pro - Forced

More information

Computational Simulation of Dynamic Response of Vehicle Tatra T815 and the Ground

Computational Simulation of Dynamic Response of Vehicle Tatra T815 and the Ground IOP Conference Series: Earth and Environmental Science PAPER OPEN ACCESS Computational Simulation of Dynamic Response of Vehicle Tatra T815 and the Ground To cite this article: Jozef Vlek and Veronika

More information

Chapter 14 Oscillations

Chapter 14 Oscillations Chapter 14 Oscillations If an object vibrates or oscillates back and forth over the same path, each cycle taking the same amount of time, the motion is called periodic. The mass and spring system is a

More information

Varuvan Vadivelan. Institute of Technology LAB MANUAL. : 2013 : B.E. MECHANICAL ENGINEERING : III Year / V Semester. Regulation Branch Year & Semester

Varuvan Vadivelan. Institute of Technology LAB MANUAL. : 2013 : B.E. MECHANICAL ENGINEERING : III Year / V Semester. Regulation Branch Year & Semester Varuvan Vadivelan Institute of Technology Dharmapuri 636 703 LAB MANUAL Regulation Branch Year & Semester : 2013 : B.E. MECHANICAL ENGINEERING : III Year / V Semester ME 6511 - DYNAMICS LABORATORY GENERAL

More information

Influence of the Soil Structure Interaction on the Fundamental Period of Large Dynamic Machine Foundation

Influence of the Soil Structure Interaction on the Fundamental Period of Large Dynamic Machine Foundation Influence of the Soil Structure Interaction on the Fundamental Period of Large Dynamic Machine Foundation Jingbo Liu, Wenhui Wang, Xiaobo Zhang, Dongdong Zhao Department of Civil Engineering, Tsinghua

More information

Dynamic Soil Structure Interaction

Dynamic Soil Structure Interaction Dynamic Soil Structure Interaction Kenji MIURA, Dr. Eng. Professor Graduate School of Engineering Hiroshima University Dynamic Soil Structure Interaction Chapter 1 : Introduction Kenji MIURA, Dr. Eng.

More information

Mechatronics. MANE 4490 Fall 2002 Assignment # 1

Mechatronics. MANE 4490 Fall 2002 Assignment # 1 Mechatronics MANE 4490 Fall 2002 Assignment # 1 1. For each of the physical models shown in Figure 1, derive the mathematical model (equation of motion). All displacements are measured from the static

More information

APPROXIMATE DYNAMIC MODEL SENSITIVITY ANALYSIS FOR LARGE, COMPLEX SPACE STRUCTURES. Timothy S. West, Senior Engineer

APPROXIMATE DYNAMIC MODEL SENSITIVITY ANALYSIS FOR LARGE, COMPLEX SPACE STRUCTURES. Timothy S. West, Senior Engineer APPROXIMATE DYNAMIC MODEL SENSITIVITY ANALYSIS FOR LARGE, COMPLEX SPACE STRUCTURES Timothy S. West, Senior Engineer McDonnell Douglas Aerospace Space Station Division, Houston, Texas ABSTRACT During the

More information

Chapter 14 Oscillations. Copyright 2009 Pearson Education, Inc.

Chapter 14 Oscillations. Copyright 2009 Pearson Education, Inc. Chapter 14 Oscillations Oscillations of a Spring Simple Harmonic Motion Energy in the Simple Harmonic Oscillator Simple Harmonic Motion Related to Uniform Circular Motion The Simple Pendulum The Physical

More information

COMPLEX MODULUS AND DAMPING MEASUREMENTS USING RESONANT AND NON-RESONANT METHODS

COMPLEX MODULUS AND DAMPING MEASUREMENTS USING RESONANT AND NON-RESONANT METHODS COMPLEX MODULUS AND DAMPING MEASUREMENTS USING RESONANT AND NON-RESONANT METHODS S. Gade, K. Zaveri, H. Konstantin-Hansen and H. Herlufsen Briiel & Kjaer, Skodsborgvej 307,285O Naerum, Denmark ABSTRACT

More information

Structural Dynamics. Spring mass system. The spring force is given by and F(t) is the driving force. Start by applying Newton s second law (F=ma).

Structural Dynamics. Spring mass system. The spring force is given by and F(t) is the driving force. Start by applying Newton s second law (F=ma). Structural Dynamics Spring mass system. The spring force is given by and F(t) is the driving force. Start by applying Newton s second law (F=ma). We will now look at free vibrations. Considering the free

More information

Vibrations of Machine Foundations

Vibrations of Machine Foundations Vibrations of Machine Foundations Richard P. Ray, Ph.D., P.E. Civil and Environmental Engineering University of South Carolina Thanks To: Prof. Richard D. Woods, Notre Dame Univ. Prof. F.E. Richart, Jr.

More information

UNITS AND DEFINITIONS RELATED TO BIOMECHANICAL AND ELECTROMYOGRAPHICAL MEASUREMENTS

UNITS AND DEFINITIONS RELATED TO BIOMECHANICAL AND ELECTROMYOGRAPHICAL MEASUREMENTS APPENDIX B UNITS AND DEFINITIONS RELATED TO BIOMECHANICAL AND ELECTROMYOGRAPHICAL MEASUREMENTS All units used are SI (Système International d Unités). The system is based on seven well-defined base units

More information

Advanced Vibrations. Elements of Analytical Dynamics. By: H. Ahmadian Lecture One

Advanced Vibrations. Elements of Analytical Dynamics. By: H. Ahmadian Lecture One Advanced Vibrations Lecture One Elements of Analytical Dynamics By: H. Ahmadian ahmadian@iust.ac.ir Elements of Analytical Dynamics Newton's laws were formulated for a single particle Can be extended to

More information

k 21 k 22 k 23 k 24 k 31 k 32 k 33 k 34 k 41 k 42 k 43 k 44

k 21 k 22 k 23 k 24 k 31 k 32 k 33 k 34 k 41 k 42 k 43 k 44 CE 6 ab Beam Analysis by the Direct Stiffness Method Beam Element Stiffness Matrix in ocal Coordinates Consider an inclined bending member of moment of inertia I and modulus of elasticity E subjected shear

More information

Dynamic Analysis Contents - 1

Dynamic Analysis Contents - 1 Dynamic Analysis Contents - 1 TABLE OF CONTENTS 1 DYNAMIC ANALYSIS 1.1 Overview... 1-1 1.2 Relation to Equivalent-Linear Methods... 1-2 1.2.1 Characteristics of the Equivalent-Linear Method... 1-2 1.2.2

More information

Foundation Engineering Dr. Priti Maheshwari Department Of Civil Engineering Indian Institute Of Technology, Roorkee

Foundation Engineering Dr. Priti Maheshwari Department Of Civil Engineering Indian Institute Of Technology, Roorkee Foundation Engineering Dr. Priti Maheshwari Department Of Civil Engineering Indian Institute Of Technology, Roorkee Module - 02 Lecture - 15 Machine Foundations - 3 Hello viewers, In the last class we

More information

This equation of motion may be solved either by differential equation method or by graphical method as discussed below:

This equation of motion may be solved either by differential equation method or by graphical method as discussed below: 2.15. Frequency of Under Damped Forced Vibrations Consider a system consisting of spring, mass and damper as shown in Fig. 22. Let the system is acted upon by an external periodic (i.e. simple harmonic)

More information

EXPERIMENTAL DETERMINATION OF DYNAMIC CHARACTERISTICS OF STRUCTURES

EXPERIMENTAL DETERMINATION OF DYNAMIC CHARACTERISTICS OF STRUCTURES EXPERIMENTAL DETERMINATION OF DYNAMIC CHARACTERISTICS OF STRUCTURES RADU CRUCIAT, Assistant Professor, Technical University of Civil Engineering, Faculty of Railways, Roads and Bridges, e-mail: rcruciat@utcb.ro

More information

NONLINEAR CHARACTERISTICS OF THE PILE-SOIL SYSTEM UNDER VERTICAL VIBRATION

NONLINEAR CHARACTERISTICS OF THE PILE-SOIL SYSTEM UNDER VERTICAL VIBRATION IGC 2009, Guntur, INDIA NONLINEAR CHARACTERISTICS OF THE PILE-SOIL SYSTEM UNDER VERTICAL VIBRATION B. Manna Lecturer, Civil Engineering Department, National Institute of Technology, Rourkela 769008, India.

More information

A Circular Cavity Embedded in a Full-Plane Under Impulse Pressure

A Circular Cavity Embedded in a Full-Plane Under Impulse Pressure Benchmark Example No. 50 A Circular Cavity Embedded in a Full-Plane Under Impulse Pressure SOFiSTiK 2018 VERiFiCATiON MANUAL BE50: A Circular Cavity Embedded in a Full-Plane Under Impulse Pressure VERiFiCATiON

More information

Oscillations. Phys101 Lectures 28, 29. Key points: Simple Harmonic Motion (SHM) SHM Related to Uniform Circular Motion The Simple Pendulum

Oscillations. Phys101 Lectures 28, 29. Key points: Simple Harmonic Motion (SHM) SHM Related to Uniform Circular Motion The Simple Pendulum Phys101 Lectures 8, 9 Oscillations Key points: Simple Harmonic Motion (SHM) SHM Related to Uniform Circular Motion The Simple Pendulum Ref: 11-1,,3,4. Page 1 Oscillations of a Spring If an object oscillates

More information

Codal Provisions IS 1893 (Part 1) 2002

Codal Provisions IS 1893 (Part 1) 2002 Abstract Codal Provisions IS 1893 (Part 1) 00 Paresh V. Patel Assistant Professor, Civil Engineering Department, Nirma Institute of Technology, Ahmedabad 38481 In this article codal provisions of IS 1893

More information

Dynamic Analysis of Pile Foundations: Effects of Material Nonlinearity of Soil

Dynamic Analysis of Pile Foundations: Effects of Material Nonlinearity of Soil Dynamic Analysis of Pile Foundations: Effects of Material Nonlinearity of Soil Bal Krishna Maheshwari Asst. Professor, Department of Earthquake Engineering, IIT Roorkee, Roorkee, U.A. 247 667, India (Formerly

More information

Introduction to Geotechnical Earthquake Engineering

Introduction to Geotechnical Earthquake Engineering Module 1 Introduction to Geotechnical Earthquake Engineering by Dr. Deepankar Choudhury Professor Department of Civil Engineering IIT Bombay, Powai, Mumbai 400 076, India. Email: dc@civil.iitb.ac.in URL:

More information

*Definition of Mechanics *Basic Concepts *Newton s Laws *Units

*Definition of Mechanics *Basic Concepts *Newton s Laws *Units INTRODUCTION *Definition of Mechanics *Basic Concepts *Newton s Laws *Units Mechanics may be defined as the physical science which describes and predicts the conditions of rest or motion of bodies under

More information

557. Radial correction controllers of gyroscopic stabilizer

557. Radial correction controllers of gyroscopic stabilizer 557. Radial correction controllers of gyroscopic stabilizer M. Sivčák 1, J. Škoda, Technical University in Liberec, Studentská, Liberec, Czech Republic e-mail: 1 michal.sivcak@tul.cz; jan.skoda@pevnosti.cz

More information

Analyses of Soil-Structure Systems

Analyses of Soil-Structure Systems Analyses of Soil-Structure Systems Julio García Paul C. Rizzo Associates, Inc., 105 Mall Blvd. Suite 270E, Monroeville, PA 15146, USA Phone: +1 (412)856-9700, Fax: +1 (412)856-9749, Email: julio.garcia@rizzoassoc.com

More information

Sound radiation and sound insulation

Sound radiation and sound insulation 11.1 Sound radiation and sound insulation We actually do not need this chapter You have learned everything you need to know: When waves propagating from one medium to the next it is the change of impedance

More information

DYNAMIC ANALYSIS OF PILES IN SAND BASED ON SOIL-PILE INTERACTION

DYNAMIC ANALYSIS OF PILES IN SAND BASED ON SOIL-PILE INTERACTION October 1-17,, Beijing, China DYNAMIC ANALYSIS OF PILES IN SAND BASED ON SOIL-PILE INTERACTION Mohammad M. Ahmadi 1 and Mahdi Ehsani 1 Assistant Professor, Dept. of Civil Engineering, Geotechnical Group,

More information

NONLINEAR STRUCTURAL DYNAMICS USING FE METHODS

NONLINEAR STRUCTURAL DYNAMICS USING FE METHODS NONLINEAR STRUCTURAL DYNAMICS USING FE METHODS Nonlinear Structural Dynamics Using FE Methods emphasizes fundamental mechanics principles and outlines a modern approach to understanding structural dynamics.

More information

Modal analysis of shear buildings

Modal analysis of shear buildings Modal analysis of shear buildings A comprehensive modal analysis of an arbitrary multistory shear building having rigid beams and lumped masses at floor levels is obtained. Angular frequencies (rad/sec),

More information

Structural Dynamics Lecture 4. Outline of Lecture 4. Multi-Degree-of-Freedom Systems. Formulation of Equations of Motions. Undamped Eigenvibrations.

Structural Dynamics Lecture 4. Outline of Lecture 4. Multi-Degree-of-Freedom Systems. Formulation of Equations of Motions. Undamped Eigenvibrations. Outline of Multi-Degree-of-Freedom Systems Formulation of Equations of Motions. Newton s 2 nd Law Applied to Free Masses. D Alembert s Principle. Basic Equations of Motion for Forced Vibrations of Linear

More information

Response Spectrum Analysis Shock and Seismic. FEMAP & NX Nastran

Response Spectrum Analysis Shock and Seismic. FEMAP & NX Nastran Response Spectrum Analysis Shock and Seismic FEMAP & NX Nastran Table of Contents 1. INTRODUCTION... 3 2. THE ACCELEROGRAM... 4 3. CREATING A RESPONSE SPECTRUM... 5 4. NX NASTRAN METHOD... 8 5. RESPONSE

More information

WORK SHEET FOR MEP311

WORK SHEET FOR MEP311 EXPERIMENT II-1A STUDY OF PRESSURE DISTRIBUTIONS IN LUBRICATING OIL FILMS USING MICHELL TILTING PAD APPARATUS OBJECTIVE To study generation of pressure profile along and across the thick fluid film (converging,

More information

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each.

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each. GTE 2016 Q. 1 Q. 9 carry one mark each. D : SOLID MECHNICS Q.1 single degree of freedom vibrating system has mass of 5 kg, stiffness of 500 N/m and damping coefficient of 100 N-s/m. To make the system

More information

Vibration analysis of compressor piping system with fluid pulsation

Vibration analysis of compressor piping system with fluid pulsation Journal of Mechanical Science and Technology 6 () () 393~399 www.springerlink.com/content/738-494x DOI.7/s6--89-8 Vibration analysis of compressor piping system with fluid pulsation Seong-Hyeon Lee, Sang-Mo

More information

Design Procedures For Dynamically Loaded Foundations

Design Procedures For Dynamically Loaded Foundations Design Procedures For Dynamically Loaded Foundations 1/11 Choice of parameters for equivalent lumped systems Lumped mass : the mass of the foundation and supported machinery Damping : 1 Geometrical(or

More information

SHOCK RESPONSE SPECTRUM ANALYSIS VIA THE FINITE ELEMENT METHOD Revision C

SHOCK RESPONSE SPECTRUM ANALYSIS VIA THE FINITE ELEMENT METHOD Revision C SHOCK RESPONSE SPECTRUM ANALYSIS VIA THE FINITE ELEMENT METHOD Revision C By Tom Irvine Email: tomirvine@aol.com November 19, 2010 Introduction This report gives a method for determining the response of

More information

ME 563 HOMEWORK # 5 SOLUTIONS Fall 2010

ME 563 HOMEWORK # 5 SOLUTIONS Fall 2010 ME 563 HOMEWORK # 5 SOLUTIONS Fall 2010 PROBLEM 1: You are given the lumped parameter dynamic differential equations of motion for a two degree-offreedom model of an automobile suspension system for small

More information

Effect of Soil-Foundation Interaction on the Dynamic Response of a Four-Cylinder Compressor Foundation

Effect of Soil-Foundation Interaction on the Dynamic Response of a Four-Cylinder Compressor Foundation Case Study Effect of Soil-Foundation Interaction on the Dynamic Response of a Four-Cylinder Compressor Foundation O. S. Ali, Ph.D., P.E., M.ASCE 1 ; and Mustafa Mahamid, Ph.D., P.E., S.E., F.ASCE 2 Abstract:

More information

Chap. 15: Simple Harmonic Motion

Chap. 15: Simple Harmonic Motion Chap. 15: Simple Harmonic Motion Announcements: CAPA is due next Tuesday and next Friday. Web page: http://www.colorado.edu/physics/phys1110/phys1110_sp12/ Examples of periodic motion vibrating guitar

More information

T1 T e c h n i c a l S e c t i o n

T1 T e c h n i c a l S e c t i o n 1.5 Principles of Noise Reduction A good vibration isolation system is reducing vibration transmission through structures and thus, radiation of these vibration into air, thereby reducing noise. There

More information

DEVELOPMENT OF ACTIVELY TUNED VIBRATION ABSORBER FOR WASHING MACHINE

DEVELOPMENT OF ACTIVELY TUNED VIBRATION ABSORBER FOR WASHING MACHINE DEVELOPMENT OF ACTIVELY TUNED VIBRATION ABSORBER FOR WASHING MACHINE Mr.G.M.ABHISHEK 1, Mr. K. S. MANOBALA 2 1M.E.product design and commerce, psg college of technology, Coimbatore, Tamilnadu, India 2Assistant

More information

Theoretical Manual Theoretical background to the Strand7 finite element analysis system

Theoretical Manual Theoretical background to the Strand7 finite element analysis system Theoretical Manual Theoretical background to the Strand7 finite element analysis system Edition 1 January 2005 Strand7 Release 2.3 2004-2005 Strand7 Pty Limited All rights reserved Contents Preface Chapter

More information

Explosion Protection of Buildings

Explosion Protection of Buildings Explosion Protection of Buildings Author: Miroslav Mynarz Explosion Protection of Buildings Introduction to the Problems of Determination of Building Structure's Response 3 Classification of actions According

More information

18.12 FORCED-DAMPED VIBRATIONS

18.12 FORCED-DAMPED VIBRATIONS 8. ORCED-DAMPED VIBRATIONS Vibrations A mass m is attached to a helical spring and is suspended from a fixed support as before. Damping is also provided in the system ith a dashpot (ig. 8.). Before the

More information

TWO-STAGE ISOLATION FOR HARMONIC BASE EXCITATION Revision A. By Tom Irvine February 25, 2008

TWO-STAGE ISOLATION FOR HARMONIC BASE EXCITATION Revision A. By Tom Irvine   February 25, 2008 TWO-STAGE ISOLATION FOR HARMONIC BASE EXCITATION Revision A By Tom Irvine Email: tomirvine@aol.com February 5, 008 Introduction Consider a base plate mass m and an avionics mass m modeled as two-degree-of-freedom.

More information

NON-LINEAR VISCOELASTIC MODEL OF STRUCTURAL POUNDING

NON-LINEAR VISCOELASTIC MODEL OF STRUCTURAL POUNDING 3 th World Conference on Earthquake Engineering Vancouver, B.C., Canada August -6, 004 Paper No. 308 NON-LINEAR VISCOELASTIC MODEL OF STRUCTURAL POUNDING Robert JANKOWSKI SUMMARY Pounding between structures

More information

PLANAR KINETICS OF A RIGID BODY: WORK AND ENERGY Today s Objectives: Students will be able to: 1. Define the various ways a force and couple do work.

PLANAR KINETICS OF A RIGID BODY: WORK AND ENERGY Today s Objectives: Students will be able to: 1. Define the various ways a force and couple do work. PLANAR KINETICS OF A RIGID BODY: WORK AND ENERGY Today s Objectives: Students will be able to: 1. Define the various ways a force and couple do work. In-Class Activities: 2. Apply the principle of work

More information

Final Exam December 13, 2016

Final Exam December 13, 2016 Final Exam Instructions: You have 120 minutes to complete this exam. This is a closed-boo, closed-notes exam. You are allowed to use a calculator during the exam. Do NOT unstaple your exam. Do NOT write

More information

SHAKE TABLE STUDY OF SOIL STRUCTURE INTERACTION EFFECTS ON SEISMIC RESPONSE OF SINGLE AND ADJACENT BUILDINGS

SHAKE TABLE STUDY OF SOIL STRUCTURE INTERACTION EFFECTS ON SEISMIC RESPONSE OF SINGLE AND ADJACENT BUILDINGS 13 th World Conference on Earthquake Engineering Vancouver, B.C., Canada August 1-6, 2004 Paper No. 1918 SHAKE TABLE STUDY OF SOIL STRUCTURE INTERACTION EFFECTS ON SEISMIC RESPONSE OF SINGLE AND ADJACENT

More information

Strength Study of Spiral Flexure Spring of Stirling Cryocooler

Strength Study of Spiral Flexure Spring of Stirling Cryocooler Sensors & Transducers 2013 by IFSA http://www.sensorsportal.com Strength Study of Spiral of Stirling Cryocooler WANG Wen-Rui, NIE Shuai, ZHANG Jia-Ming School of Mechanical Engineering, University of Science

More information

Dynamics Manual. Version 7

Dynamics Manual. Version 7 Dynamics Manual Version 7 DYNAMICS MANUAL TABLE OF CONTENTS 1 Introduction...1-1 1.1 About this manual...1-1 2 Tutorial...2-1 2.1 Dynamic analysis of a generator on an elastic foundation...2-1 2.1.1 Input...2-1

More information

MODELLING OF VIBRATION WITH ABSORBER

MODELLING OF VIBRATION WITH ABSORBER Journal of Machine Engineering, Vol. 10, No.4, 2010 mumerical modelling, Simulink, vibration, machine, absorber Jiří VONDŘICH 1 Evžen THÖNDE 1 Slavomír JIRKŮ 1 MODEING OF VIBRATION WITH ABSORBER Machine

More information

Structure Design and Modal Analysis for a New Type of Cycloidal Drives

Structure Design and Modal Analysis for a New Type of Cycloidal Drives Structure Design and Modal nalysis for a New Type of Cycloidal Drives Yiqiang Jiang, Li Hou, Yunxia You, Jingyu Zhang School of Manufacturing Science and Engineering Sichuan University Chengdu, Sichuan,China

More information

SEISMIC RESPONSE OF INDUSTRIAL STRUCTURES CONSIDERING SOIL-PILE-STRUCTURE INTERACTION

SEISMIC RESPONSE OF INDUSTRIAL STRUCTURES CONSIDERING SOIL-PILE-STRUCTURE INTERACTION 13 th World Conference on Earthquake Engineering Vancouver, B.C., Canada August 1-6, 2004 Paper No. 3129 SEISMIC RESPONSE OF INDUSTRIAL STRUCTURES CONSIDERING SOIL-PILE-STRUCTURE INTERACTION Yingcai Han

More information

Engineering Science OUTCOME 2 - TUTORIAL 3 FREE VIBRATIONS

Engineering Science OUTCOME 2 - TUTORIAL 3 FREE VIBRATIONS Unit 2: Unit code: QCF Level: 4 Credit value: 5 Engineering Science L/60/404 OUTCOME 2 - TUTORIAL 3 FREE VIBRATIONS UNIT CONTENT OUTCOME 2 Be able to determine the behavioural characteristics of elements

More information

1. Multiple Degree-of-Freedom (MDOF) Systems: Introduction

1. Multiple Degree-of-Freedom (MDOF) Systems: Introduction 1. Multiple Degree-of-Freedom (MDOF) Systems: Introduction Lesson Objectives: 1) List examples of MDOF structural systems and state assumptions of the idealizations. 2) Formulate the equation of motion

More information

LANMARK UNIVERSITY OMU-ARAN, KWARA STATE DEPARTMENT OF MECHANICAL ENGINEERING COURSE: MECHANICS OF MACHINE (MCE 322). LECTURER: ENGR.

LANMARK UNIVERSITY OMU-ARAN, KWARA STATE DEPARTMENT OF MECHANICAL ENGINEERING COURSE: MECHANICS OF MACHINE (MCE 322). LECTURER: ENGR. LANMARK UNIVERSITY OMU-ARAN, KWARA STATE DEPARTMENT OF MECHANICAL ENGINEERING COURSE: MECHANICS OF MACHINE (MCE 322). LECTURER: ENGR. IBIKUNLE ROTIMI ADEDAYO SIMPLE HARMONIC MOTION. Introduction Consider

More information

Determination of dynamic soil characteristics and transfer functions to support the evaluation of the efficiency of vibration mitigation measures

Determination of dynamic soil characteristics and transfer functions to support the evaluation of the efficiency of vibration mitigation measures RIVAS Final Conference "Vibrations Ways out of the annoyance" Royal Flemish Academy of Belgium, Brussels, 21 November 213 Determination of dynamic soil characteristics and transfer functions to support

More information

STIFFNESS AND DAMPING OF SOIL-PILE SYSTEM IN LIQUEFACTION PROCESS

STIFFNESS AND DAMPING OF SOIL-PILE SYSTEM IN LIQUEFACTION PROCESS th World Conference on Earthquake Engineering Vancouver, B.C., Canada August -6, 4 Paper No. 8 STIFFNESS AND DAMPING OF SOIL-PILE SYSTEM IN LIQUEFACTION PROCESS Hatsukazu MIZUNO and Tsutomu HIRADE SUMMARY

More information

Introduction to Continuous Systems. Continuous Systems. Strings, Torsional Rods and Beams.

Introduction to Continuous Systems. Continuous Systems. Strings, Torsional Rods and Beams. Outline of Continuous Systems. Introduction to Continuous Systems. Continuous Systems. Strings, Torsional Rods and Beams. Vibrations of Flexible Strings. Torsional Vibration of Rods. Bernoulli-Euler Beams.

More information

MASS LOADING EFFECTS FOR HEAVY EQUIPMENT AND PAYLOADS Revision F

MASS LOADING EFFECTS FOR HEAVY EQUIPMENT AND PAYLOADS Revision F MASS LOADING EFFECTS FOR HEAVY EQUIPMENT AND PAYLOADS Revision F By Tom Irvine Email: tomirvine@aol.com May 19, 2011 Introduction Consider a launch vehicle with a payload. Intuitively, a realistic payload

More information

MODELING AND FEM ANALYSIS OF DYNAMIC PROPERTIES OF THERMALLY OPTIMAL COMPOSITE MATERIALS

MODELING AND FEM ANALYSIS OF DYNAMIC PROPERTIES OF THERMALLY OPTIMAL COMPOSITE MATERIALS 11th World Congress on Computational Mechanics (WCCM XI) 5th European Conference on Computational Mechanics (ECCM V) 6th European Conference on Computational Fluid Dynamics (ECFD VI) E. Oñate, J. Oliver

More information

3. Overview of MSC/NASTRAN

3. Overview of MSC/NASTRAN 3. Overview of MSC/NASTRAN MSC/NASTRAN is a general purpose finite element analysis program used in the field of static, dynamic, nonlinear, thermal, and optimization and is a FORTRAN program containing

More information

Lecture 31. EXAMPLES: EQUATIONS OF MOTION USING NEWTON AND ENERGY APPROACHES

Lecture 31. EXAMPLES: EQUATIONS OF MOTION USING NEWTON AND ENERGY APPROACHES Lecture 31. EXAMPLES: EQUATIONS OF MOTION USING NEWTON AND ENERGY APPROACHES Figure 5.29 (a) Uniform beam moving in frictionless slots and attached to ground via springs at A and B. The vertical force

More information

Final Exam Solution Dynamics :45 12:15. Problem 1 Bateau

Final Exam Solution Dynamics :45 12:15. Problem 1 Bateau Final Exam Solution Dynamics 2 191157140 31-01-2013 8:45 12:15 Problem 1 Bateau Bateau is a trapeze act by Cirque du Soleil in which artists perform aerial maneuvers on a boat shaped structure. The boat

More information

Embedded Foundation with Different Parameters under Dynamic Excitations

Embedded Foundation with Different Parameters under Dynamic Excitations 13 th World Conference on Earthquake Engineering Vancouver, B.C., Canada August 1-6, 2004 Paper No. 2287 Embedded Foundation with Different Parameters under Dynamic Excitations Jaya K P 1 and Meher Prasad

More information

Address for Correspondence

Address for Correspondence Research Article EXPERIMENT STUDY OF DYNAMIC RESPONSE OF SOFT STOREY BUILDING MODEL C. S. Sanghvi 1, H S Patil 2 and B J Shah 3 Address for Correspondence 1 Associate Professor, Applied Mechanics Department,

More information

Modal and Static Structural Analysis of Exhaust Collector Box for Compressor test facility

Modal and Static Structural Analysis of Exhaust Collector Box for Compressor test facility Modal and Static Structural Analysis of Exhaust Collector Box for Compressor test facility Shankar Gouda 1, Praveen M P 2 P G student, Department of Mechanical Engineering, EPCET, Bangalore, Karnataka,

More information

COEFFICIENT OF DYNAMIC HORIZONTAL SUBGRADE REACTION OF PILE FOUNDATIONS ON PROBLEMATIC GROUND IN HOKKAIDO Hirofumi Fukushima 1

COEFFICIENT OF DYNAMIC HORIZONTAL SUBGRADE REACTION OF PILE FOUNDATIONS ON PROBLEMATIC GROUND IN HOKKAIDO Hirofumi Fukushima 1 COEFFICIENT OF DYNAMIC HORIZONTAL SUBGRADE REACTION OF PILE FOUNDATIONS ON PROBLEMATIC GROUND IN HOKKAIDO Hirofumi Fukushima 1 Abstract In this study, static loading tests and dynamic shaking tests of

More information

ROTATING RING. Volume of small element = Rdθbt if weight density of ring = ρ weight of small element = ρrbtdθ. Figure 1 Rotating ring

ROTATING RING. Volume of small element = Rdθbt if weight density of ring = ρ weight of small element = ρrbtdθ. Figure 1 Rotating ring ROTATIONAL STRESSES INTRODUCTION High centrifugal forces are developed in machine components rotating at a high angular speed of the order of 100 to 500 revolutions per second (rps). High centrifugal force

More information

Rigid Part Mating. Goals of this class

Rigid Part Mating. Goals of this class Rigid Part Mating Goals of this class understand the phases of a typical part mate determine the basic scaling laws understand basic physics of part mating for simple geometries relate forces and motions

More information

3-D FINITE ELEMENT NONLINEAR DYNAMIC ANALYSIS FOR SOIL-PILE-STRUCTURE INTERACTION

3-D FINITE ELEMENT NONLINEAR DYNAMIC ANALYSIS FOR SOIL-PILE-STRUCTURE INTERACTION 13 th World Conference on Earthquake Engineering Vancouver, B.C., Canada August 1-, 4 Paper No. 157 3-D FINITE ELEMENT NONLINEAR DYNAMIC ANALYSIS FOR SOIL-PILE-STRUCTURE INTERACTION B.K. MAHESHWARI 1,

More information

MEC3403. Dynamics II. Introductory book. Faculty of Engineering and Surveying

MEC3403. Dynamics II. Introductory book. Faculty of Engineering and Surveying MEC3403 Dynamics II Faculty of Engineering and Surveying Introductory book Semester 2 2010 Published by University of Southern Queensland Toowoomba Queensland 4350 Australia http://www.usq.edu.au University

More information

RESPONSE SPECTRUM METHOD FOR ESTIMATION OF PEAK FLOOR ACCELERATION DEMAND

RESPONSE SPECTRUM METHOD FOR ESTIMATION OF PEAK FLOOR ACCELERATION DEMAND RESPONSE SPECTRUM METHOD FOR ESTIMATION OF PEAK FLOOR ACCELERATION DEMAND Shahram Taghavi 1 and Eduardo Miranda 2 1 Senior catastrophe risk modeler, Risk Management Solutions, CA, USA 2 Associate Professor,

More information

Integration simulation method concerning speed control of ultrasonic motor

Integration simulation method concerning speed control of ultrasonic motor Integration simulation method concerning speed control of ultrasonic motor R Miyauchi 1, B Yue 2, N Matsunaga 1 and S Ishizuka 1 1 Cybernet Systems Co., Ltd. 3 Kanda-neribeicho,Chiyoda-ku, Tokyo,101-0022,Japan

More information

Introduction to Mechanical Vibration

Introduction to Mechanical Vibration 2103433 Introduction to Mechanical Vibration Nopdanai Ajavakom (NAV) 1 Course Topics Introduction to Vibration What is vibration? Basic concepts of vibration Modeling Linearization Single-Degree-of-Freedom

More information

Chapter 5. Vibration Analysis. Workbench - Mechanical Introduction ANSYS, Inc. Proprietary 2009 ANSYS, Inc. All rights reserved.

Chapter 5. Vibration Analysis. Workbench - Mechanical Introduction ANSYS, Inc. Proprietary 2009 ANSYS, Inc. All rights reserved. Workbench - Mechanical Introduction 12.0 Chapter 5 Vibration Analysis 5-1 Chapter Overview In this chapter, performing free vibration analyses in Simulation will be covered. In Simulation, performing a

More information

A Guide to linear dynamic analysis with Damping

A Guide to linear dynamic analysis with Damping A Guide to linear dynamic analysis with Damping This guide starts from the applications of linear dynamic response and its role in FEA simulation. Fundamental concepts and principles will be introduced

More information

Software Verification

Software Verification SAP000 EXAMPLE 6-00 LINK LINEAR LINK WITH RAMP LOADING PROBLEM DESCRIPTION In this example a ramp load is applied to an undamped single degree of freedom structure. The ramp loading has a finite rise time

More information

ABSTRACT. Ossama Salem Ali Ahmed, Ph.D., interaction of the pile with the surrounding soils under vibratory loading will modify

ABSTRACT. Ossama Salem Ali Ahmed, Ph.D., interaction of the pile with the surrounding soils under vibratory loading will modify ABSTRACT Title of Document: VERTICAL DYNAMIC SOIL-PILE INTERACTION FOR MACHINE FOUNDATIONS Ossama Salem Ali Ahmed, Ph.D., 2015 Directed By: Professor, M. Sherif Aggour, Department of Civil and Environmental

More information

Experimental Study of Seismic Soil-Structure Interaction by using Large Geotechnical Centrifuge System

Experimental Study of Seismic Soil-Structure Interaction by using Large Geotechnical Centrifuge System October 12-17, 28, Beijing, China Experimental Study of Seismic Soil-Structure Interaction by using Large Geotechnical Centrifuge System T. Kawasato 1, T. Okutani 1, T. Ishikawa 1, T. Fujimori 2, and M.

More information

On The Finite Element Modeling Of Turbo Machinery Rotors In Rotor Dynamic Analysis

On The Finite Element Modeling Of Turbo Machinery Rotors In Rotor Dynamic Analysis Proceedings of The Canadian Society for Mechanical Engineering International Congress 2018 CSME International Congress 2018 May 27-30, 2018, Toronto, On, Canada On The Finite Element Modeling Of Turbo

More information

Geotechnical Earthquake Engineering

Geotechnical Earthquake Engineering Geotechnical Earthquake Engineering by Dr. Deepankar Choudhury Professor Department of Civil Engineering IIT Bombay, Powai, Mumbai 400 076, India. Email: dc@civil.iitb.ac.in URL: http://www.civil.iitb.ac.in/~dc/

More information

Research on Optimization of Bearing Span of Main Reducer Gear System Based on the Transfer Matrix

Research on Optimization of Bearing Span of Main Reducer Gear System Based on the Transfer Matrix MATEC Web of Conferences 3, () DOI:.5/ matecconf/3 MMME Research on Optimization of Bearing Span of Main Reducer Gear System Based on the Transfer Matrix Feng Yun HUANG, Li TIAN a, Ding WEI and Huan Huan

More information

Graphical User Interface (GUI) for Torsional Vibration Analysis of Rotor Systems Using Holzer and MatLab Techniques

Graphical User Interface (GUI) for Torsional Vibration Analysis of Rotor Systems Using Holzer and MatLab Techniques Basrah Journal for Engineering Sciences, vol. 14, no. 2, 2014 255 Graphical User Interface (GUI) for Torsional Vibration Analysis of Rotor Systems Using Holzer and MatLab Techniques Dr. Ameen Ahmed Nassar

More information

EQUIVALENT FRACTURE ENERGY CONCEPT FOR DYNAMIC RESPONSE ANALYSIS OF PROTOTYPE RC GIRDERS

EQUIVALENT FRACTURE ENERGY CONCEPT FOR DYNAMIC RESPONSE ANALYSIS OF PROTOTYPE RC GIRDERS EQUIVALENT FRACTURE ENERGY CONCEPT FOR DYNAMIC RESPONSE ANALYSIS OF PROTOTYPE RC GIRDERS Abdul Qadir Bhatti 1, Norimitsu Kishi 2 and Khaliq U Rehman Shad 3 1 Assistant Professor, Dept. of Structural Engineering,

More information