In general stress in a material can be defined by three normal stresses and three shear stresses. For many cases we can simplify to three stress components.

Slides:



Advertisements
Similar presentations
Mechanics of Materials – MAE 243 (Section 002) Spring 2008
Advertisements

Chapter Outline Shigley’s Mechanical Engineering Design.
III. Strain and Stress Basics of continuum mechanics, Strain Basics of continuum mechanics, Stress Reading Suppe, Chapter 3 Twiss&Moores, chapter 15 Additional.
Hamrock Fundamentals of Machine Elements Chapter 2: Load, Stress and Strain The careful text-books measure (Let all who build beware!) The load, the shock,
Chapter 3 Rock Mechanics Stress
PLANE STRAIN TRANSFORMATION
PLANE STRESS TRANSFORMATION
CHAPTER OBJECTIVES Apply the stress transformation methods derived in Chapter 9 to similarly transform strain Discuss various ways of measuring strain.
Copyright © 2011 Pearson Education South Asia Pte Ltd
Principle and Maximum Shearing Stresses ( )
Analysis of Stress and Strain
Analysis of Stress and Strain Review: - Axially loaded Bar - Torsional shaft Questions: (1) Is there any general method to determine stresses on any arbitrary.
Mechanics of Materials – MAE 243 (Section 002) Spring 2008
Professor Joe Greene CSU, CHICO
Stress Transformation
ENGR 220 Section
Chapter Outline Shigley’s Mechanical Engineering Design.
Checking Out Stress States With Mohr’s Circle
GLG310 Structural Geology. 16 July 2015GLG310 Structural Geology.
Mechanics of Materials(ME-294)
Distributed Forces: Moments of Inertia
IV. Basics of continuum mechanics, Stress Reading Suppe, Chapter 3 Twiss&Moores, chapter 15 Additional References : Jean Salençon, Handbook of continuum.
7.2 Shear and Moment Equations and Diagrams
Civil Engineering Materials – CIVE 2110
Theories of Stress and Strain
Content Stress Transformation A Mini Quiz Strain Transformation
Transformations of Stress and Strain
APPLICATIONS/ MOHR’S CIRCLE
10.7 Moments of Inertia for an Area about Inclined Axes
Mock Course – Plane Stress Transformation (ref MCHT 213, Hibbeler text) 1 hr 15 min format: –Present Theory/Overview with Power Point, 15 min. –Problem.
Mechanics of Materials – MAE 243 (Section 002) Spring 2008 Dr. Konstantinos A. Sierros.
Introduction Stress: When some external system of forces act on a body, the internal forces are set up at various sections of the body, which resist the.
CHAPTER OBJECTIVES To show how to transform the stress components that are associated with a particular coordinate system into components associated with.
Stress and Strain ( , 3.14) MAE 316 – Strength of Mechanical Components NC State University Department of Mechanical & Aerospace Engineering Stress.
Stress: Stress tensor Principal stresses and directions Maximum shear stresses and directions Failure theories.
Structure Analysis I. Lecture 7 Internal Loading Developed in Structural Members Ch.4 in text book.
BFC (Mechanics of Materials) Chapter 1: Stress & Strain Shahrul Niza Mokhatar
Triaxial State of Stress at any Critical Point in a Loaded Body
Transformations of Stress and Strain
ME16A: CHAPTER FOUR ANALYSIS OF STRESSES IN TWO DIMENSIONS.
1 Structural Geology Force and Stress - Mohr Diagrams, Mean and Deviatoric Stress, and the Stress Tensor Lecture 6 – Spring 2016.
MOHR'S CIRCLE The formulas developed in the preceding article may be used for any case of plane stress. A visual interpretation of them, devised by the.
CHAPTER OBJECTIVES Derive equations for transforming stress components between coordinate systems of different orientation Use derived equations to.
6. Strain Assoc.Prof.Dr. Ahmet Zafer Şenalp Mechanical Engineering Department Gebze Technical University.
GLG310 Structural Geology. 18 March 2016GLG310 Structural Geology.
Transformation methods - Examples
Copyright ©2011 by Pearson Education, Inc. All rights reserved. Mechanics of Materials, Eighth Edition Russell C. Hibbeler General Plane-Strain Transformation.
Principal Stresses and Strain and Theories of Failure
Mohr’s Circles GLE/CEE 330 Lecture Notes Soil Mechanics
1 CHAPTER 2C- Mohr’s Circle Dr. Zuhailawati Hussain EBB 334 Mechanical Metallurgy.
EAG 345 – GEOTECHNICAL ANALYSIS
1. PLANE–STRESS TRANSFORMATION
DEPARTMENT OF MECHANICAL AND MANUFACTURING ENGINEERING
Chapter 7 Transformations of Stress and Strain.
Overview Introduction
Mohr’s circle for plane stress
Transformations of Stress and Strain
Transformations of Stress and Strain
CHAPTER OBJECTIVES Derive equations for transforming stress components between coordinate systems of different orientation Use derived equations to.
BDA30303 Solid Mechanics II.
Example 7.01 SOLUTION: Find the element orientation for the principal stresses from Determine the principal stresses from Fig For the state of plane.
Strain Transformation
Review from LAB #3.
Mechanics of Materials Engr Lecture 15 Stress Transformation 2
Mechanics of Materials ENGR Lecture 19 Mohr’s Circle
Mechanics of Materials Engr Lecture 20 More Mohr’s Circles
Mechanics of Materials Engr 350 – Lecture 39 What’s On the Final Exam?
Compound Normal & Shear Stresses
Copyright ©2014 Pearson Education, All Rights Reserved
Copyright ©2014 Pearson Education, All Rights Reserved
Presentation transcript:

In general stress in a material can be defined by three normal stresses and three shear stresses. For many cases we can simplify to three stress components. If no stresses act on the outside surfaces we call the state of stress plane stress. In this case we can treat the problem in 2 dimensions. To determine the maximum normal and shear stresses it is necessary that we can transform stresses from one co-ordinate system to another.

To transform stress from one orientation to another we need to take into account 1)magnitude of each stress 2)orientation of each stress 3)the orientation of each area the stress acts on So the transformation is similar to that used for force components but is a little more involved.

Take sectionsDraw the free body diagram Force equilibrium

The state of plane stress at a point on the surface of the airplane fuselage is represented on the element oriented as shown in the figure. Represent the state of stress at the point on an element that is oriented 30° clockwise from the position. Step 1Take sections

A B Step 2Draw the two free body diagrams.

A B Step 3Force Equilibrium for A

A B

A B

General Equations of Plane-Stress Transformation

B Step 3Force Equilibrium for A

Answer

Graph showing the variation of normal stress and shear stress with angle. The principal in-plane stresses are the maximum and minimum stresses. These will occur at the maxima and minima of the curve.

The magnitude and direction of the principal stresses can therefore be defined as a circle.

Mohr’s circle can be used as a graphical technique to transform stress and/or strain. Stress transformations Combine and add Circle with radius R

Christian Otto Mohr (October 8, October 2, 1918) was a German civil engineer, one of the most celebrated of the nineteenth century.October 81835October Germancivil engineernineteenth century Starting in 1855, his early working life was spent in railroad engineering for the Hanover and Oldenburg state railways, designing some famous bridges and making some of the earliest uses of steel trusses.1855railroadHanoverOldenburg bridgessteeltrusses Even during his early railway years, Mohr's interest had been attracted by the theories of mechanics and the strength of materials, and in 1867, he became professor of mechanics at Stuttgart Polytechnic and, in 1873, at Dresden Polytechnic. Mohr had a direct and unpretentious lecturing style that was popular with his students.strength of materials1867professorStuttgartPolytechnic 1873Dresden Mohr was an enthusiast for graphical tools and developed the method, for visually representing stress in three dimensions, previously proposed by Carl Culmann. In 1882, he famously developed the graphical method for analysing stress known as Mohr's circle and used it to propose an early theory of strength based on shear stress.stressCarl Culmann1882Mohr's circlestrengthshear stress

Constructing Mohr’s Circle 1)Co-ordinate system with normal stress +ve to right and shear stress +ve down 2)Using the sign convention shown plot the center of the circle C at the average normal stress on the x axis 3)Plot a reference point at  x  xy – this represents  =0 4)Connect A with C and determine the radius. 5)Draw the circle

Principle stresses are at B and D  p is measured counter-clockwise from AC to BC & DC  s is measured clockwise from AC to EC or FC