Structure I Course Code: ARCH 208 Dr. Aeid A. Abdulrazeg.

Slides:



Advertisements
Similar presentations
Stress and Strain – Axial Loading
Advertisements

Statically Determinate and Indeterminate System of Bars.
Indeterminate Structure Session Subject: S1014 / MECHANICS of MATERIALS Year: 2008.
Strength of Materials I EGCE201 กำลังวัสดุ 1
Chapter 12 Deflection of beams and shafts
Chapter 4 AXIAL LOADING.
Stress and Strain – Axial Loading
ENGR 225 Section Saint-Venant’s Principle When loading is applied at a point on a body, it tends to create a stress distribution that becomes.
ENGR 220 Section
Stress and Strain – Axial Loading
9 Deflection of Beams.
4.5 FORCE METHOD OF ANALYSIS FOR AXIALLY LOADED MEMBERS
Suitability of a structure or machine may depend on the deformations in the structure as well as the stresses induced under loading. Statics analyses.
CE 329 Structural Analysis
Hooke’s Law and Modulus of Elasticity ( )
CE 329 Structural Analysis Spring Objectives ― General List Course Objectives Describe Topical Coverage for Class Provide the Formula for Computing.
Sample Problem 9.8 For the uniform beam and loading shown, determine the reaction at each support and the slope at end A. SOLUTION: Release the “redundant”
Chapter 2 Stress and Strain -- Axial Loading
Strengths Chapter 10 Strains. 1-1 Intro Structural materials deform under the action of forces Three kinds of deformation Increase in length called an.
Chapter 4 Axial Load. Saint -Venant's Principle Saint-Venant's Principle claims that localized effects caused by any load acting on a body will dissipate.
MECHANICS OF MATERIALS Fourth Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf Lecture Notes: J. Walt Oler Texas Tech University CHAPTER.
CTC / MTC 322 Strength of Materials
Stress and Strain – Axial Loading
Stress and Strain – Axial Loading
Machine Design I (MCE-C 203) Mechatronics Dept., Faculty of Engineering, Fayoum University Dr. Ahmed Salah Abou Taleb Lecturer, Mechanical Engineering.
 2005 Pearson Education South Asia Pte Ltd 4. Axial Load 1 CHAPTER OBJECTIVES Determine deformation of axially loaded members Develop a method to find.
Strength of Materials Malayer University Department of Civil Engineering Taught by: Dr. Ali Reza Bagherieh In The Name of God.
CHAPTER OBJECTIVES Determine deformation of axially loaded members
Stress and Strain – Axial Loading
نظام المحاضرات الالكترونينظام المحاضرات الالكتروني Strength of materials.
Thermal Stress Objective: Lecture # 8
Engg College Tuwa Mechanics of Solids.( ) Presented by: PARMAR CHETANKUMAR VIKRAMSINH PARMAR NILESHKUMAR NATVARLAL PARMAR.
Mechanics of Materials – MAE 243 (Section 002) Spring 2008 Dr. Konstantinos A. Sierros.
Stress and Strain – Axial Loading
11 Energy Methods.
11 Energy Methods.
Stress and Strain – Axial Loading
Poisson’s Ratio For a slender bar subjected to axial loading:
Superposition & Statically Indeterminate Beams
Introduction – Concept of Stress
Stress and Strain – Axial Loading
Solid Mechanics Course No. ME213.
Concept of Stress.
Chapter 4 Axial Load.
Sample Problem 9.8 For the uniform beam and loading shown, determine the reaction at each support and the slope at end A. SOLUTION: Release the “redundant”
Thin Walled Pressure Vessels
3 Torsion.
Deflections using energy methods
9 Deflection of Beams.
Poisson’s Ratio For a slender bar subjected to axial loading:
3 Torsion.
CTC / MTC 222 Strength of Materials
11 Energy Methods.
Structure I Course Code: ARCH 208 Dr. Aeid A. Abdulrazeg
Structure I Course Code: ARCH 208 Dr. Aeid A. Abdulrazeg
STATICS (ENGINEERING MECHANICS-I)
CHAPTER 2 BASIC CONCEPTS OF DISPLACEMENT OR STIFFNESS METHOD:
CHAPTER OBJECTIVES Determine deformation of axially loaded members
Structure I Course Code: ARCH 208 Dr. Aeid A. Abdulrazeg.
Statics Course Code: CIVL211 Dr. Aeid A. Abdulrazeg
Stress and Strain – Axial Loading
Mechanics of Materials Engr Lecture 10 Axial Deformation #1
Poisson’s Ratio For a slender bar subjected to axial loading:
Structure I Course Code: ARCH 208 Dr. Aeid A. Abdulrazeg
Concept of Stress.
Structure I Course Code: ARCH 208 Dr. Aeid A. Abdulrazeg
Statics Course Code: CIVL211 Dr. Aeid A. Abdulrazeg
Structure I Course Code: ARCH 208 Dr. Aeid A. Abdulrazeg
Structural Analysis II
Presentation transcript:

Structure I Course Code: ARCH 208 Dr. Aeid A. Abdulrazeg

Contents Stress & Strain: Axial Loading Normal Strain Stress-Strain Test Stress-Strain Diagram: Ductile Materials Stress-Strain Diagram: Brittle Materials Hooke’s Law: Modulus of Elasticity Deformations Under Axial Loading Static Indeterminacy Thermal Stresses Answers: 1. D 2. B Dr. Aeid A. Abdulrazeg

Stress & Strain: Axial Loading Suitability of a structure or machine may depend on the deformations in the structure as well as the stresses induced under loading. Statics analyses alone are not sufficient. Considering structures as deformable allows determination of member forces and reactions which are statically indeterminate. Determination of the stress distribution within a member also requires consideration of deformations in the member.

Normal Strain

Stress-Strain Test

Stress-Strain Diagram: Ductile Materials

Stress-Strain Diagram: Brittle Materials

Hooke’s Law: Modulus of Elasticity Strength is affected by alloying, heat treating, and manufacturing process but stiffness (Modulus of Elasticity) is not.

Deformations Under Axial Loading From Hooke’s Law: From the definition of strain: Equating and solving for the deformation, With variations in loading, cross-section or material properties,

Example SOLUTION: Divide the rod into components at the load application points. Apply a free-body analysis on each component to determine the internal force. Evaluate the total of the component deflections. Determine the deformation of the steel rod shown under the given loads.

SOLUTION: Divide the rod into three components:

Static Indeterminacy Structures for which internal forces and reactions cannot be determined from statics alone are said to be statically indeterminate. A structure will be statically indeterminate whenever it is held by more supports than are required to maintain its equilibrium. Redundant reactions are replaced with unknown loads which along with the other loads must produce compatible deformations. Deformations due to actual loads and redundant reactions are determined separately and then added or superposed. Dr. Aeid A. Abdulrazeg

Example Determine the reactions at A and B for the steel bar and loading shown, assuming a close fit at both supports before the loads are applied. SOLUTION: Consider the reaction at B as redundant, release the bar from that support, and solve for the displacement at B due to the applied loads. Solve for the displacement at B due to the redundant reaction at B. Require that the displacements due to the loads and due to the redundant reaction be compatible, i.e., require that their sum be zero. Solve for the reaction at A due to applied loads and the reaction found at B.

SOLUTION: Solve for the displacement at B due to the applied loads with the redundant constraint released, Solve for the displacement at B due to the redundant constraint,

Require that the displacements due to the loads and due to the redundant reaction be compatible, Find the reaction at A due to the loads and the reaction at B

Thermal Stresses A temperature change results in a change in length or thermal strain. There is no stress associated with the thermal strain unless the elongation is restrained by the supports. Treat the additional support as redundant and apply the principle of superposition. The thermal deformation and the deformation from the redundant support must be compatible.