Copyright © 2009 Pearson Education, Inc. Lecture 8a – States of Matter Solids.

Slides:



Advertisements
Similar presentations
PH0101 UNIT 1 LECTURE 1 Elasticity and Plasticity Stress and Strain
Advertisements

Chapter 13 - Elasticity A PowerPoint Presentation by
Springs and Elasticity ClassAct SRS enabled. In this presentation you will: Explore the concept of elasticity as exhibited by springs.
Edexcel AS Physics Unit 1 : Chapter 7: Solid Materials
Professor Joe Greene CSU, CHICO
Elasticity by Ibrhim AlMohimeed
Solid Materials.
Chapter 11 Mechanical Properties of Materials
LECTURER 2 Engineering and True Stress-Strain Diagrams
Normal Strain and Stress
Chapter 3 Mechanical Properties of Materials
Stress, Strain, and elastic moduli
EXPERIMENT # 3 Instructor: M.Yaqub
Copyright © 2009 Pearson Education, Inc. Chapter 12 Elasticity.
Chapter 12 Equilibrium and Elasticity Key contents Conditions for mechanical equilibrium Indeterminate structure Stress, strain, modulus of elasticity.
Structure Strength Lecturer: Professor Stephen T. Thornton.
Physics. Properties of Matter Session Session Objectives.
Mechanics of Materials II
Deforming Solids.
Objectives  Understand how elasticity is related to Hooke’s Law for springs.  Know that the change in length of an object is proportional to the force.
1.3.4 Behaviour of Springs and Materials
Elastic Stress-Strain Relationships
CHAPTER OBJECTIVES Show relationship of stress and strain using experimental methods to determine stress-strain diagram of a specific material Discuss.
Elasticity and Strength of Materials
Strong forces are needed to stretch a solid object. The force needed depends on several factors.
2.2 Materials Materials Breithaupt pages 162 to 171.
Physics 121.
FYI: All three types of stress are measured in newtons / meter2 but all have different effects on solids. Materials Solids are often placed under stress.
1 Physics for Scientists & Engineers, with Modern Physics, 4 th edition Giancoli Piri Reis University / Physics -I.
Class #1.2 Civil Engineering Materials – CIVE 2110
Static Equilibrium; Elasticity and Fracture
EGR 280 Mechanics 6 – Introduction to Mechanics of Materials.
Physics Notes Ch 9 Statics Statics – The study of forces in equilibrium. The net force and the net torque on an object (or on a system) are zero. The.
Stress and Strain  Tensile Stress- the ratio of the magnitude of the applied force F to the cross-sectional area A: Mathematically, Stress= Force/Area=F/A.
ELASTICITY. Elasticity  Elasticity is a branch of Solid mechanics that deals with the elastic behavior of solids. It is the property of material of a.
Strengths Chapter 10 Strains. 1-1 Intro Structural materials deform under the action of forces Three kinds of deformation Increase in length called an.
– SOLID MECHANICS S.ARAVINDAN Lecturer Department of Aeronautical Engineering Rajalakshmi Engineering College 1.
STRUCTURES Outcome 3 Gary Plimer 2008 MUSSELBURGH GRAMMAR SCHOOL.
Static Equilibrium; Elasticity and Fracture
Mechanical Properties of Materials
Materials PHYA2. MATERIALS DENSITY, SPRINGS, STRESS AND STRAIN Topics 11, pp.162–173.
Copyright © 2009 Pearson Education, Inc. An object with forces acting on it, but with zero net force, is said to be in equilibrium. The Conditions for.
© 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
Chapter 2 Properties of Metals.
1.To understand the keywords associated with the deformation of different types of solids 2.To be able to calculate stress, strain and hence Young’s modulus.
Chapter 9: Mechanical Properties of Matter
Describe each section of the graph below.. Spring follows Hooke’s law; it has elastic behaviour. Elastic limit is reached, it is permanently deformed.
1.To understand the keywords associated with the deformation of different types of solids 2.To be able to calculate stress, strain and hence Young’s modulus.
Unit 1 Key Facts- Materials Hooke’s Law Force extension graph Elastic energy Young’s Modulus Properties of materials.
UNIVERSITY OF GUYANA FACULTY OF NATURAL SCIENCES DEPART. OF MATH, PHYS & STATS PHY 110 – PHYSICS FOR ENGINEERS LECTURE 12 (THURSDAY, NOVEMBER 17, 2011)
ENGR 107 – Introduction to Engineering Static Equilibrium, and Stress and Strain (Lecture #8)
STRUCTURES Young’s Modulus. Tests There are 4 tests that you can do to a material There are 4 tests that you can do to a material 1 tensile This is where.
Chapter 12 Lecture 22: Static Equilibrium and Elasticity: II.
© Pearson Education Ltd 2008 This document may have been altered from the original Week 13 Objectives Define and use the terms stress, strain and Young.
Elasticity Yashwantarao Chavan Institute of Science Satara Physics
Boundless Lecture Slides Free to share, print, make copies and changes. Get yours at Available on the Boundless Teaching Platform.
Hooke’s Law & springs Objectives
PROPERTIES OF MATERIALS ENF 150 Chapter 10: Properties of Materials.
Stress and Strain Review and Elastic Energy
3.4.2 mechanical properties of matter
Types of Solids There are three main types of solid:
Chapter 9 Static Equilibrium; Elasticity and Fracture
Chapter 7 Deforming Solids.
young’s modulus 10:00 Particle Physics :30 3 Experiments 12:00
(a) Describe what material the spring is made from;
Elastic Deformation: Stress, Strain and Hook’s Law
Describing deformation
Presentation transcript:

Copyright © 2009 Pearson Education, Inc. Lecture 8a – States of Matter Solids

Copyright © 2009 Pearson Education, Inc. Elasticity; Stress and Strain Units of Chapter 12

Copyright © 2009 Pearson Education, Inc. Hooke’s law: the change in length is proportional to the applied force Elasticity; Stress and Strain

Copyright © 2009 Pearson Education, Inc. This proportionality holds until the force reaches the proportional limit. Beyond that, the object will still return to its original shape up to the elastic limit. Beyond the elastic limit, the material is permanently deformed, and it breaks at the breaking point Elasticity; Stress and Strain

Copyright © 2009 Pearson Education, Inc. Stress-Strain Graph The graph which results from plotting the applied stress on a test specimen in tension versus the corresponding strain. The test is usually carried out at a constant rate of elongation or strain.

Copyright © 2009 Pearson Education, Inc. Stress-Strain Graph

Copyright © 2009 Pearson Education, Inc. The change in length of a stretched object depends not only on the applied force, but also on its length, cross-sectional area and the material from which it is made. The material factor, E, is called the elastic modulus or Young’s modulus, and it has been measured for many materials Elasticity; Stress and Strain

Copyright © 2009 Pearson Education, Inc Elasticity; Stress and Strain

Copyright © 2009 Pearson Education, Inc Elasticity; Stress and Strain Example 12-7: Tension in piano wire. A 1.60-m-long steel piano wire has a diameter of 0.20 cm. How great is the tension in the wire if it stretches 0.25 cm when tightened?

Copyright © 2009 Pearson Education, Inc Elasticity; Stress and Strain Stress is defined as the force per unit area. Strain is defined as the ratio of the change in length to the original length. Therefore, the elastic modulus is equal to the stress divided by the strain:

Copyright © 2009 Pearson Education, Inc. In tensile stress, forces tend to stretch the object Elasticity; Stress and Strain

Copyright © 2009 Pearson Education, Inc. Compressional stress is exactly the opposite of tensional stress. These columns are under compression Elasticity; Stress and Strain

Copyright © 2009 Pearson Education, Inc. The three types of stress for rigid objects: 12-4 Elasticity; Stress and Strain

Copyright © 2009 Pearson Education, Inc. Strain Energy Definition of Strain Energy The mechanical energy stored-up in stressed materials Definition of Elastic Strain Energy The potential energy stored in a strained solid equal to the work performed in deforming the solid from its unstrained state less any energy dissipated by inelastic deformation. Source