Chapter Outline Shigley’s Mechanical Engineering Design.

Slides:



Advertisements
Similar presentations
Mohr Circle for stress In 2D space (e.g., on the s1s2 , s1s3, or s2s3 plane), the normal stress (sn) and the shear stress (ss), could be given by equations.
Advertisements

Chapter 6 Bending.
MECH 401 Mechanical Design Applications Dr. M. O’Malley – Master Notes
Chapter Outline Shigley’s Mechanical Engineering Design.
CTC / MTC 222 Strength of Materials Chapter 1 Basic Concepts.
Design of Shaft A shaft is a rotating member usually of circular cross-section (solid or hollow), which transmits power and rotational motion. Machine.
MAE 314 – Solid Mechanics Yun Jing
CHAPTER 6 BENDING.
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,
Deformation of Solids Stress is proportional to Strain stress = elastic modulus * strain The SI unit for stress is the Newton per meter squared (N/m 2.
Introduction – Concept of Stress
PLANE STRESS TRANSFORMATION
Load and Stress Analysis
Copyright © 2011 Pearson Education South Asia Pte Ltd
Principle and Maximum Shearing Stresses ( )
ENGR 225 Section
SWEDISH COLLEGE OF ENGINEERING & TECHNOLOGY
Contact Stress (3.19) MAE 316 – Strength of Mechanical Components
Chapter Outline Shigley’s Mechanical Engineering Design.
Solid mechanics 1.1 – key points
Chapter 2: Load, Stress and Strain
Mechanics of Materials(ME-294)
Introduction – Concept of Stress
Ken Youssefi Mechanical Engineering Department 1 Normal & Shear components of stress Normal stress is perpendicular to the cross section,  (sigma). Shear.
Chapter 1 Stress.
Engineering Mechanics: Statics
Distributed Forces: Moments of Inertia
Mechanics of Materials Goal:Load Deformation Factors that affect deformation of a structure P PPP Stress: intensity of internal force.
IV. Basics of continuum mechanics, Stress Reading Suppe, Chapter 3 Twiss&Moores, chapter 15 Additional References : Jean Salençon, Handbook of continuum.
CTC / MTC 222 Strength of Materials Final Review.
Copyright © 2010 Pearson Education South Asia Pte Ltd
MAE 343-Intermediate Mechanics of Materials QUIZ No.1 - Thursday, Aug. 26, 2004 List three possible failure modes of a machine element (5points) List the.
9 Torsion.
Chapter 1: Stress Review important principles of statics
Load and Stress Analysis
STRENGTHS Chapter Intro Dealing with relationship between the external loads applied to an elastic body and the intensity of the internal forces.
8 Principle Stresses Under a Given Loading. © 2002 The McGraw-Hill Companies, Inc. All rights reserved. MECHANICS OF MATERIALS ThirdEdition Beer Johnston.
CHAPTER OBJECTIVES Analyze the stress developed in thin-walled pressure vessels Review the stress analysis developed in previous chapters regarding axial.
Mechanics of Materials – MAE 243 (Section 002) Spring 2008 Dr. Konstantinos A. Sierros.
Overview of Mechanical Engineering for Non-MEs Part 2: Mechanics of Materials 6 Introduction – Concept of Stress.
CTC / MTC 222 Strength of Materials Chapter 1 Basic Concepts.
Lecture 7 Mechanical Properties of Rocks
Theoretical Mechanics STATICS KINEMATICS
CHAPTER OBJECTIVES To show how to transform the stress components that are associated with a particular coordinate system into components associated with.
COMBINED LOADING.  Analyze the stress developed in thin-walled pressure vessels  Review the stress analysis developed in previous chapters regarding.
Copyright Kaplan AEC Education, 2005 Mechanics of Materials Outline Overview AXIALLY LOADED MEMBERS, p. 262 Modulus of Elasticity Poisson’s Ratio Thermal.
Stress and Strain ( , 3.14) MAE 316 – Strength of Mechanical Components NC State University Department of Mechanical & Aerospace Engineering Stress.
Triaxial State of Stress at any Critical Point in a Loaded Body
Objectives  Introduce the concept of pressure;  Prove it has a unique value at any particular elevation;  Show how it varies with depth according.
The McGraw-Hill Companies © 2012
Chapter 6: Bending.
Axial Force Definition: Force which is parallel to the longitudinal axis of the member.
Lecture 1 Stress 16 July 2007 ENT 450 Mechanics of Materials Dr. Haftirman 1 ENT 450 MECHANICS OF MATERIALS (MoM) RC. Hibbler Lecture: DR. HAFTIRMAN Teaching.
The McGraw-Hill Companies © 2012
BME 315 – Biomechanics Chapter 4. Mechanical Properties of the Body Professor: Darryl Thelen University of Wisconsin-Madison Fall 2009.
Principal Stresses and Strain and Theories of Failure
BME 315 – Biomechanics Chapter 4. Mechanical Properties of the Body Professor: Darryl Thelen University of Wisconsin-Madison Fall 2009.
MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt Oler Texas Tech.
1. PLANE–STRESS TRANSFORMATION
DEPARTMENT OF MECHANICAL AND MANUFACTURING ENGINEERING
Stress = Force/Area Force is measured in units of mass*acceleration 1 N (Newton) = 1 kg * m * s-2 another common unit for force is the pound.
Introduction – Concept of Stress
Concept of Stress.
Ch. 2: Fundamental of Structure
Concept of Stress.
CHAPTER OUTLINE Introduction Equilibrium of a deformable body Stress
Copyright ©2014 Pearson Education, All Rights Reserved
CE Statics Chapter 7 – Lecture 3.
Presentation transcript:

Chapter Outline Shigley’s Mechanical Engineering Design

Free-Body Diagram Example 3-1 Shigley’s Mechanical Engineering Design

Free-Body Diagram Example 3-1 Fig. 3-1 Shigley’s Mechanical Engineering Design

Free-Body Diagram Example 3-1 Shigley’s Mechanical Engineering Design

Free-Body Diagram Example 3-1 Shigley’s Mechanical Engineering Design

Free-Body Diagram Example 3-1 Shigley’s Mechanical Engineering Design

Shear Force and Bending Moments in Beams Cut beam at any location x1 Internal shear force V and bending moment M must ensure equilibrium Fig. 3−2 Shigley’s Mechanical Engineering Design

Sign Conventions for Bending and Shear Fig. 3−3 Shigley’s Mechanical Engineering Design

Distributed Load on Beam Distributed load q(x) called load intensity Units of force per unit length Fig. 3−4 Shigley’s Mechanical Engineering Design

Relationships between Load, Shear, and Bending The change in shear force from A to B is equal to the area of the loading diagram between xA and xB. The change in moment from A to B is equal to the area of the shear-force diagram between xA and xB. Shigley’s Mechanical Engineering Design

Shear-Moment Diagrams Fig. 3−5 Shigley’s Mechanical Engineering Design

Moment Diagrams – Two Planes Fig. 3−24 Shigley’s Mechanical Engineering Design

Combining Moments from Two Planes Add moments from two planes as perpendicular vectors Fig. 3−24 Shigley’s Mechanical Engineering Design

Singularity Functions A notation useful for integrating across discontinuities Angle brackets indicate special function to determine whether forces and moments are active Table 3−1 Shigley’s Mechanical Engineering Design

Example 3-2 Fig. 3-5 Shigley’s Mechanical Engineering Design

Example 3-2 Shigley’s Mechanical Engineering Design

Example 3-2 Shigley’s Mechanical Engineering Design

Example 3-3 Fig. 3-6 Shigley’s Mechanical Engineering Design

Example 3-3 Shigley’s Mechanical Engineering Design

Example 3-3 Fig. 3-6 Shigley’s Mechanical Engineering Design

Normal stress is normal to a surface, designated by s Tangential shear stress is tangent to a surface, designated by t Normal stress acting outward on surface is tensile stress Normal stress acting inward on surface is compressive stress U.S. Customary units of stress are pounds per square inch (psi) SI units of stress are newtons per square meter (N/m2) 1 N/m2 = 1 pascal (Pa) Shigley’s Mechanical Engineering Design

Represents stress at a point Coordinate directions are arbitrary Stress element Represents stress at a point Coordinate directions are arbitrary Choosing coordinates which result in zero shear stress will produce principal stresses Shigley’s Mechanical Engineering Design

Two bodies with curved surfaces pressed together Contact Stresses Two bodies with curved surfaces pressed together Point or line contact changes to area contact Stresses developed are three-dimensional Called contact stresses or Hertzian stresses Common examples Wheel rolling on rail Mating gear teeth Rolling bearings Shigley’s Mechanical Engineering Design

Spherical Contact Stress Two solid spheres of diameters d1 and d2 are pressed together with force F Circular area of contact of radius a Shigley’s Mechanical Engineering Design

Spherical Contact Stress Pressure distribution is hemispherical Maximum pressure at the center of contact area Fig. 3−36 Shigley’s Mechanical Engineering Design

Spherical Contact Stress Maximum stresses on the z axis Principal stresses From Mohr’s circle, maximum shear stress is Shigley’s Mechanical Engineering Design

Spherical Contact Stress Plot of three principal stress and maximum shear stress as a function of distance below the contact surface Note that tmax peaks below the contact surface Fatigue failure below the surface leads to pitting and spalling For poisson ratio of 0.30, tmax = 0.3 pmax at depth of z = 0.48a Fig. 3−37 Shigley’s Mechanical Engineering Design

Cylindrical Contact Stress Two right circular cylinders with length l and diameters d1 and d2 Area of contact is a narrow rectangle of width 2b and length l Pressure distribution is elliptical Half-width b Maximum pressure Fig. 3−38 Shigley’s Mechanical Engineering Design

Cylindrical Contact Stress Maximum stresses on z axis Shigley’s Mechanical Engineering Design

Cylindrical Contact Stress Plot of stress components and maximum shear stress as a function of distance below the contact surface For poisson ratio of 0.30, tmax = 0.3 pmax at depth of z = 0.786b Fig. 3−39 Shigley’s Mechanical Engineering Design