Dynamic Stability of Periodically Stiffened Pipes Conveying Fluid Dr. Osama J. Aldraihem Dept. of Mechanical Engineering King Saud University, Saudi Arabia.

Slides:



Advertisements
Similar presentations
Application of the Root-Locus Method to the Design and Sensitivity Analysis of Closed-Loop Thermoacoustic Engines C Mark Johnson.
Advertisements

MEG 361 CAD Finite Element Method Dr. Mostafa S. Hbib.
Finite element method Among the up-to-date methods of stress state analysis, the finite element method (abbreviated as FEM below, or often as FEA for analyses.
1 Department of Civil and Environmental Engineering Sungkyunkwan University 비대칭 박벽보의 개선된 해석이론 및 방법 An Improved Theory and Analysis Procedures of Nonsymmetric.
Spring 2007 Dr. D. M. McStravick Rice University
TRC Project: Predictions of Force Coefficients in Off-Centered Grooved Oil Seals A novel FE Bulk-Flow Model for Improved Predictions of Force Coefficients.
10 Columns.
APPLIED MECHANICS Lecture 10 Slovak University of Technology
Introduction to Statics
1 MECH 221 FLUID MECHANICS (Fall 06/07) Tutorial 7.
Column Design ( ) MAE 316 – Strength of Mechanical Components
Smart Materials in System Sensing and Control Dr. M. Sunar Mechanical Engineering Department King Fahd University of Petroleum & Minerals.
Technical University of Łódź Department of Strength of Material and Structures M.Kotelko, Z. Kołakowski, R.J. Mania LOAD-BEARING CAPACITY OF THIN-WALLED.
Review (2 nd order tensors): Tensor – Linear mapping of a vector onto another vector Tensor components in a Cartesian basis (3x3 matrix): Basis change.
Dynamic Analysis-A Finite –Element Approach
© 2011 Autodesk Freely licensed for use by educational institutions. Reuse and changes require a note indicating that content has been modified from the.
In Engineering --- Designing a Pneumatic Pump Introduction System characterization Model development –Models 1, 2, 3, 4, 5 & 6 Model analysis –Time domain.
Proceedings of the 18 th International Conference on Nuclear Engineering ICONE18 May , 2010, Xi’an, China Hannam University Fluid-elastic Instability.
The Finite Element Method
Ken YoussefiMechanical Engineering Dept. 1 Design Optimization Optimization is a component of design process The design of systems can be formulated as.
Chapter 10 Columns .
BY Prof. Zeinab S. Abdel Rehim & M. A. Ziada and Salwa El-Deeb H Mechanical Engineering Department National Research Centre Egypt Prof. Zeinab S. Abdel.
Contact Line Instability in Driven Films
FINITE ELEMENT ANALYSIS CONVERSION FACTORS FOR NATURAL VIBRATIONS OF BEAMS Austin Cosby and Ernesto Gutierrez-Miravete Rensselaer at Hartford.
MECN 4600 Inter - Bayamon Lecture Mechanical Measurement and Instrumentation MECN 4600 Professor: Dr. Omar E. Meza Castillo
Ken YoussefiMechanical Engineering Dept. 1 Design Optimization Optimization is a component of design process The design of systems can be formulated as.
One of the most important fields in engineering Mechanics.
A PPLIED M ECHANICS Lecture 01 Slovak University of Technology Faculty of Material Science and Technology in Trnava.
3. Stresses in Machine Elements Lecture Number – 3.1 Prof. Dr. C. S. Pathak Department of Mechanical Engineering Sinhgad College of Engineering, Pune Strength.
Buckling of Slender Columns ( )
Characteristics of Two-phase Flows in Vertical Pipe
Aerospace Engineering Laboratory II Vibration of Beam
Order of Magnitude Scaling of Complex Engineering Problems Patricio F. Mendez Thomas W. Eagar May 14 th, 1999.
Illustration of FE algorithm on the example of 1D problem Problem: Stress and displacement analysis of a one-dimensional bar, loaded only by its own weight,
Convective Heat Transfer in Porous Media filled with Compressible Fluid subjected to Magnetic Field Watit Pakdee* and Bawonsak Yuwaganit Center R & D on.
1 Aerospace & Mechanical Engineering Department Continuum Mechanics & Thermomechanics Tel: +32-(0) Chemin des chevreuils 1 Fax: +32-(0)
HEAT TRANSFER FINITE ELEMENT FORMULATION
HCMUT 2004 Faculty of Applied Sciences Hochiminh City University of Technology The Finite Element Method PhD. TRUONG Tich Thien Department of Engineering.
On Describing Mean Flow Dynamics in Wall Turbulence J. Klewicki Department of Mechanical Engineering University of New Hampshire Durham, NH
ENERGY CONVERSION MME 9617A Eric Savory Lecture 10 – Analyzing a complete plant: Energy conversion cycles Department.
The Stability of Laminar Flows - 2
© 2011 Autodesk Freely licensed for use by educational institutions. Reuse and changes require a note indicating that content has been modified from the.
Buckling Capacity of Pretwisted Steel Columns: Experiments and Finite Element Simulation Farid Abed & Mai Megahed Department of Civil Engineering American.
STATIC ANALYSIS OF UNCERTAIN STRUCTURES USING INTERVAL EIGENVALUE DECOMPOSITION Mehdi Modares Tufts University Robert L. Mullen Case Western Reserve University.
F. Fairag, H Tawfiq and M. Al-Shahrani Department of Math & Stat Department of Mathematics and Statistics, KFUPM. Nov 6, 2013 Preconditioning Technique.
RELIABLE DYNAMIC ANALYSIS OF TRANSPORTATION SYSTEMS Mehdi Modares, Robert L. Mullen and Dario A. Gasparini Department of Civil Engineering Case Western.
☻ ☻ ☻ ☻ 2.0 Bending of Beams sx 2.1 Revision – Bending Moments
EGM 5653 Advanced Mechanics of Materials
1 FEMCI Workshop 2002 May 23, NASA Goddard Space Flight Center, Greenbelt, MD. PASSIVE CONTROL OF VIBRATION AND WAVE PROPAGATION WAVE PROPAGATION.
ME 160 Introduction to Finite Element Method-Spring 2016 Topics for Term Projects by Teams of 2 Students Instructor: Tai-Ran Hsu, Professor, Dept. of Mechanical.
Fundamental (First) Principles of Fluid Mechanics
ERT 146 Engineering Mechanics Ms Siti Kamariah Md Sa’at School of Bioprocess Engineering, UniMAP
1 Dept. of Agricultural & Biological Engineering University of Illinois TSM 363 Fluid Power Systems TSM 363 Fluid Power Systems Bernoulli’s Law and Applications.
Finite element method for structural dynamic and stability analyses
Linear Buckling Analysis
Finite Element Method Weak form Monday, 11/4/2002.
By Dr. A. Ranjbaran, Associate Professor
ABE 223 ABE Principles – Machine systems Bernoulli’s Law Tony Grift
AAE 556 Aeroelasticity Lectures 22, 23
Performance Evaluation of Wood and Aluminum Baseball Bats Using Finite Element Analysis James Cain 12/4/14.
Multi-physics Simulation of a Wind Piezoelectric Energy Harvester Validated by Experimental Results Giuseppe Acciani, Filomena Di Modugno, Ernesto Mininno,
10 Columns.
Effective bending moment method
1C9 Design for seismic and climate changes
Implementation of 2D stress-strain Finite Element Modeling on MATLAB
Chapter 3 Buckling of Column SAIFULNIZAN JAMIAN.
By Heather Huenison and Allan Dolovich University of Saskatchewan
10 Columns.
Subject Name: FLUID MECHANICS
Introduction to Strength of Materials Lecturer; MOHD FIRASATH ALI.
Presentation transcript:

Dynamic Stability of Periodically Stiffened Pipes Conveying Fluid Dr. Osama J. Aldraihem Dept. of Mechanical Engineering King Saud University, Saudi Arabia INES 2003

 Motivation and Objectives  Previous Works  Modeling  Stability Analysis and Dynamic Response  Results and Discussions  Conclusions  Work in Progress/ Future Research Presentation Outline

Motivation Engineering Examples: Trans-Arabian pipeline “TAPLINE”

Motivation Heat exchanger tubesCoriolis mass flow meter

 Objectives  To present a general model for periodically stiffened pipes  To evaluate the stability of stiffened pipes  To investigate the stability for clamped-free periodic pipes of various design parameters  Pipe Construction Pipes Conveying Fluid

 Housner [1952] was the first to investigate the dynamic stability of uniform pipes supported at both ends and conveying fluids.  Benjamin [1961] was the first to correctly derive the Hamilton’s principle of continuous flexible pipes.  Païdoussis [1997] has presented a comprehensive survey of the dynamics and stability of slender structures subjected to moving fluid.  Maalawi and Ziada [2002] is focused on the static instability of stepped pipes conveying fluid.  Aldraihem and Baz [2002] studied the dynamic stability of stepped beams under the action of moving loads. Previous Works

 Main assumptions: (1) the pipe is symmetric and obeys the Euler-Bernoulli theory; (2) the fluid is incompressible and of mass m f per unit length; (3) the pipe’s cells are identical and made of isotropic materials. Modeling

 An approach that accounts for the out-release energy of a flowing fluid in a pipe should be used.  The approach is essentially the Hamilton’s principle with some modification to encompass the fluid out- flow energy(was first devised by Benjamin [1961] and then elaborated by McIver [1973]). Traditional Hamilton’s Principle New terms Formulation

 Kinetic Energy  Strain Energy  Work by Non-Conservative Forces Pipe System Energies

with boundary conditions pairs At x = 0 W = 0 or W’ = 0 or At x = L W = 0 or W’ = 0 or Inertia Force Flexural Restoring Force Internal Damping Force Coriolis Effect term Centrifugal Force Gravitational Force Distributed-Parameter Model

 Buckling of Column COMPARING TERMS  Pipe Conveying Fluid Source of Instability in Pipe Conveying Fluid

 Using a one-dimensional beam element, yields  Cast in a first order form Where Finite Element Model

 The stability of the pipe system in the neighborhood of the equilibrium depends upon the eigenvalues of the matrix [A].  If the real parts of the eigenvalues are negative, the pipe is asymptotically stable;  If at least one of the eigenvalues has a positive real part, the pipe is unstable;  If at least one of the eigenvalues has no real part, the pipe is marginally stable. Stability Analysis

 The pipe response is obtained by where Dynamic Response

Results and Discussions Material Properties Aluminum: E = 76 GPa  = 2840 kg/m 3  Control Parameters: m f,  A, EI, U and L Mass ratio Speed ratio Using Dimensionless quantities:

Results and Discussions Geometrical Properties Cantilever pipes Inner diameter: D i = 14 mm Outer diameter: D o = 16 mm Length: L = mm Fixed at the left end (x = 0) Free at the other end (x = L) Pipes are exposed to flowing fluids traveling at constant speed U form the fixed end toward the free end

Performance of Periodic Pipes

Effect of Cell Length Ratio Ls/Lu on Stability

Effect of Step Factor f on the Stability

Conclusions  Pipes stability is predicted by FEM that accounts for periodic cells and the interaction between the flowing fluid and pipe vibration.  The effect of the number of cells, cell length ratio and step factor on the stability characteristics are examined.  Results demonstrated that periodically stiffened pipes exhibit significantly improved stability characteristics.  The stability characteristics of stiffened pipes with four and more cells are comparable.  The effect of the cell length ratio on the stability appears to be important for large values of mass ratio.  Increasing the step factor enlarges the stable region of the pipe.

Work in Progress/ Future Work  Work in Progress : Dynamic analyses of pipes with periodic rings made of piezoelectric and viscoelastic materials.  Future Work: The present numerical results will be verified experimentally.