Two- and Three-Dimensional Stress Analysis

Similar documents
= ρ. Since this equation is applied to an arbitrary point in space, we can use it to determine the charge density once we know the field.

Coordinate Geometry. = k2 e 2. 1 e + x. 1 e. ke ) 2. We now write = a, and shift the origin to the point (a, 0). Referred to

FACTORS EFFECTING ELASTICITY

2 Governing Equations

Cylindrical and Spherical Coordinate Systems

PHYS 705: Classical Mechanics. Central Force Problems I

PHYS 705: Classical Mechanics. Central Force Problems II

Skps Media

LINEAR PLATE BENDING

7.2.1 Basic relations for Torsion of Circular Members

γ b =2 γ e In case there is no infiltration under the dam, the angle α is given by In case with infiltration under the dam, the angle a is given by

Chapter 12: Kinematics of a Particle 12.8 CURVILINEAR MOTION: CYLINDRICAL COMPONENTS. u of the polar coordinate system are also shown in

TRANSILVANIA UNIVERSITY OF BRASOV MECHANICAL ENGINEERING FACULTY DEPARTMENT OF MECHANICAL ENGINEERING ONLY FOR STUDENTS

Stress, Cauchy s equation and the Navier-Stokes equations

r cos, and y r sin with the origin of coordinate system located at

B l 4 P A 1 DYNAMICS OF RECIPROCATING ENGINES

However, because the center-of-mass is at the co-ordinate origin, r1 and r2 are not independent, but are related by

Physics 505 Electricity and Magnetism Fall 2003 Prof. G. Raithel. Problem Set 7 Maximal score: 25 Points. 1. Jackson, Problem Points.

As is natural, our Aerospace Structures will be described in a Euclidean three-dimensional space R 3.

ELECTROSTATICS::BHSEC MCQ 1. A. B. C. D.

5.8 Trigonometric Equations

AE301 Aerodynamics I UNIT B: Theory of Aerodynamics

In many engineering and other applications, the. variable) will often depend on several other quantities (independent variables).

A Tutorial on Multiple Integrals (for Natural Sciences / Computer Sciences Tripos Part IA Maths)

P-2: The screw eye is subjected to two forces, ԦF 1 and ԦF 2. Determine the magnitude and direction of the resultant force.

EM 388F Fracture Mechanics, Spring Introduction

ANTENNAS. Vector and Scalar Potentials. Maxwell's Equations. D = εe. For a linear, homogeneous, isotropic medium µ and ε are contant.

Physics Tutorial V1 2D Vectors

Chapter 5 Force and Motion

Course Updates. Reminders: 1) Assignment #10 due next Wednesday. 2) Midterm #2 take-home Friday. 3) Quiz # 5 next week. 4) Inductance, Inductors, RLC

Chapter 5 Force and Motion

Introduction to Vectors and Frames

3-7 FLUIDS IN RIGID-BODY MOTION

Class #16 Monday, March 20, 2017

Article : 8 Article : 8 Stress Field. and. Singularity Problem

Radian Measure CHAPTER 5 MODELLING PERIODIC FUNCTIONS

J. N. R E DDY ENERGY PRINCIPLES AND VARIATIONAL METHODS APPLIED MECHANICS

Chapter 1: Introduction to Polar Coordinates

Cartesian Coordinate System and Vectors

Lecture Principles of scattering and main concepts.

Mechanics Physics 151

Mechanics Physics 151

Momentum Heat Mass Transfer

Discretizing the 3-D Schrödinger equation for a Central Potential

Jackson 4.7 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell

Strain Energy in Linear Elastic Solids

Right-handed screw dislocation in an isotropic solid

Physics 122, Fall October 2012

Mutual Inductance. If current i 1 is time varying, then the Φ B2 flux is varying and this induces an emf ε 2 in coil 2, the emf is

1) Consider an object of a parabolic shape with rotational symmetry z

Physics 111 Lecture 5 (Walker: 3.3-6) Vectors & Vector Math Motion Vectors Sept. 11, 2009

An Application of Bessel Functions: Study of Transient Flow in a Cylindrical Pipe

Vectors Serway and Jewett Chapter 3

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS

Sides and Angles of Right Triangles 6. Find the indicated side length in each triangle. Round your answers to one decimal place.

Mechanics Physics 151

Static equilibrium requires a balance of forces and a balance of moments.

radians). Figure 2.1 Figure 2.2 (a) quadrant I angle (b) quadrant II angle is in standard position Terminal side Terminal side Terminal side

UCSD Phys 4A Intro Mechanics Winter 2016 Ch 5 Solutions

3D INTERACTION DOMAINS FOR UNREINFORCED MASONRY PANELS SUBJECTED TO ECCENTRIC COMPRESSION AND SHEAR

Understanding the Concepts

Conducting fuzzy division by using linear programming

New Newton Mechanics Taking Law of Conservation of Energy as Unique Source Law

PHYS 1444 Section 501 Lecture #7

Kepler's 1 st Law by Newton

FI 2201 Electromagnetism

Objectives. We will also get to know about the wavefunction and its use in developing the concept of the structure of atoms.

A dual-reciprocity boundary element method for axisymmetric thermoelastodynamic deformations in functionally graded solids

COORDINATE TRANSFORMATIONS - THE JACOBIAN DETERMINANT

PDF Created with deskpdf PDF Writer - Trial ::

Jackson 3.3 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell

Numerical Integration

Cartesian Control. Analytical inverse kinematics can be difficult to derive Inverse kinematics are not as well suited for small differential motions

BENDING OF BEAM. Compressed layer. Elongated. layer. Un-strained. layer. NA= Neutral Axis. Compression. Unchanged. Elongation. Two Dimensional View

Three-dimensional systems with spherical symmetry

Capacitance Extraction. Classification (orthogonal to 3D/2D)

7.2. Coulomb s Law. The Electric Force

Ch 8 Alg 2 Note Sheet Key

A moving charged particle creates a magnetic field vector at every point in space except at its position.

dx dt V x V t V y a Dt Acceleration field z dz dt V dt V v y V u t a Dt

FE FORMULATIONS FOR PLASTICITY

Physics Spring 2012 Announcements: Mar 07, 2012

Vectors, Vector Calculus, and Coordinate Systems

Physics for Scientists and Engineers

ENGI 4430 Non-Cartesian Coordinates Page xi Fy j Fzk from Cartesian coordinates z to another orthonormal coordinate system u, v, ˆ i ˆ ˆi

Tutorial Exercises: Central Forces

Physics 235 Chapter 5. Chapter 5 Gravitation

On a particular class of elastic coaction that one encounters in the study of the resistance of artillery.

Electric Charge and Field

The Strain Compatibility Equations in Polar Coordinates RAWB, Last Update 27/12/07

SPH3UW/SPH4U Unit 3.2 Forces in Cetripetal Motion Page 1 of 6. Notes Physics Tool Box

Fields. Coulomb s Law

is the instantaneous position vector of any grid point or fluid

Relative motion (Translating axes)

2. Plane Elasticity Problems

Central Force Motion

Vectors, Vector Calculus, and Coordinate Systems

ESCI 342 Atmospheric Dynamics I Lesson 3 Fundamental Forces II

Voltage-Induced Wrinkling in a Constrained Annular Dielectric Elastomer Film

Physics 181. Assignment 4

Transcription:

Two- and Thee-Dimensiona Stess Anasis Stesses, w d, d d Components of Catesian stess acting at an infinitesima ome st inde = diection of pane noma nd inde = stess diection Fom otationa eqiibim abot the thee coodinate aes in tn: = = =, The state of stess at a point is compete descibed b the si components of qiibim eqations, R R R,R,R bod foce components d d d d, d d, w qiibim of an infinitesima ome R Fom eqiibim in a thee othogona diections: R R R qiibim of foces in -diection: ddd d dd d dd dd dd dd R Stains and dispacements w w w These stain dispacement eations ae aid fo sma stains i.e. sma defomations

Stains and dispacements in mati notation w The si components of stain ae obtained fom jst the thee dispacement components thogh the mati of diffeentia opeatos: Stess-stain eations (constittie eqations and C ae 6 6 matices, hence 36 eastic constants Since smmetic, thee ae independent eastic constants astic constants ae detemined thogh aboato testing. Fo homogeneos, isotopic mateias, we edce to constants, and homogeneos phsica popeties of continm ae the same at a points isotopic eastic popeties ae the same in a diections The si components of stess ae eated to the si components of stain thogh a set of constittie eqations: C o Stess-stain eations fo homogeneos, isotopic mateia Appication of positie noma stess in one diection cases positie stain (etension in the same diection, and negatie stain (contaction in the othe two othogona diections. The amont of contaction is popotiona to the Poisson s atio,. If a thee noma stesses ae acting the noma stain noma stess eations become: Noma stains ae independent of an sheaing behaio. The sheaing stain sheaing stess eations ae: whee Stess-stain eations fo homogeneos, isotopic mateia ( ( Mati fom of the stain-stess eations: Mati fom of the stess-stain eations: C

Stain compatibiit conditions The si components of stain ae epessed in tems of on thee dispacement components: Thee mst be some conditions imposed on the stain components in ode that the si stain-dispacement eqations gie a set of singeaed continos sotions fo the thee dispacement components thoghot the inteio of the bod. Ths the components of stain cannot be compete independent of one anothe. Two Dimensions Withot oss of geneait, conside the pane. Shea stesses on the othe panes wi be eo. = = = = We wi conside thee ideaiations in two dimensions.. Pane stess: =. Pane stain: = 3. Aismmetic: thee-dimensiona bod deeoped b otation of a pana section Pane stess = Thickness is sma with espect to ength and width. No oading is appied in the thickness diection. ε Pane stain = eomet and oading ae constant in ongitdina diection. ampes: stip footing, ong cinde, etaining wa, eath dam Usa conside a section of nit thickness in the diection. Incompessibe mateia: =.5 Can case tobe with nmeica anasis of pane stain conditions. Stcta eampe: wide one-wa sab ε

Othotopic mateias Othe tpes of mateias othe than isotopic can be deat with. We wi on discss pane stess othotopic mateias in the and ais. Define as the stain in the diection de to stain in the diection. ( In genea fo independent constants Can be edced to thee with the foowing appoimation Pobem with othotopic mateias: detemination of mateia constants Pincipa Stesses Use Moh s cice to find pincipa stesses., p tan Maimm sheaing stess: ma Stess Inaiants Same nmeica ae in an coodinate sstem Stess Intensit 3 SI on Mises stess 3 3 e (effectie, eqiaent Usef in faie theoies, which state that ieding begins when cetain stess inaiant eaches a imiting ae. Aismmet Thee-dimensiona bod that is deeoped b otation of a pana section. (,,w, Aismmet ( ( Note that this is e simia to pane stain, ecept thee is an.

Stess and Stain Definitions Stains: ngineeing, o nomina stain: een-lagange stain: Logaithmic, o te stain: d n Stetch: Used in age stain and age dispacement anasis. Stesses: ngineeing stess: diide b oigina aea Cach (te stess: diide b defomed aea Smma A phsica pobems ae thee-dimensiona. Using a two-dimensiona anasis impies that at east a sma amont of ideaiation has taken pace. Two-dimension simpifications Tsses and fames Pates (mats and sabs and shes Pane defomations (pane stess, pane stain, aismmetic Stains, and hence stesses, ae obtained fom deiaties (o gadients of dispacements, and hence ae ess accate. Vaios constittie modes othe than isotopic can be sed. Detemination of mateia constants is not awas eas.