CTC / MTC 222 Strength of Materials

Slides:



Advertisements
Similar presentations
Sample Problem 4.2 SOLUTION:
Advertisements

Limit States Flexure Shear Deflection Fatigue Supports Elastic Plastic
Beams Stephen Krone, DSc, PE University of Toledo.
Chapter 11 Mechanical Properties of Materials
Sample Problem 4.2 SOLUTION:
Course Title: Strength of Materials (CVE 202)
4 Pure Bending.
Beams and Strain Gages. Cantilever Beam One End Fixed, One End Free.
Chapter 6 Bending.
Copyright Joseph Greene 2003 All Rights Reserved 1 CM 197 Mechanics of Materials Chap 16: Deflections of Beams Professor Joe Greene CSU, CHICO Reference:
Shear Force and Bending Moment
LRFD-Steel Design Dr. Ali Tayeh Second Semester
Strength of Material-5 Torsion Dr. Attaullah Shah.
Chapter 3 Torsion Torsion Engr. Othman A. Tayeh. DEFORMATIONS IN A CIRCULAR SHAFT Φ the angle of twist.
CHAPTER 6 BENDING.
Chapter 6 Section 3,4 Bending Deformation, Strain and Stress in Beams
CTC / MTC 222 Strength of Materials Chapter 5 Torsional Shear Stress and Torsional Deformation.
CHAPTER 7 TRANSVERSE SHEAR.
CTC / MTC 222 Strength of Materials
4 Pure Bending.
CTC / MTC 222 Strength of Materials
4 Pure Bending.
CM 197 Mechanics of Materials Chap 14: Stresses in Beams
Stress Analysis -MDP N161 Bending of Beams Stress and Deformation
Copyright © 2011 Pearson Education South Asia Pte Ltd
Beams: Pure Bending ( ) MAE 314 – Solid Mechanics Yun Jing Beams: Pure Bending.
CTC / MTC 222 Strength of Materials
Sample Problem 4.2 SOLUTION:
CTC / MTC 222 Strength of Materials
10 Pure Bending.
MECHANICS OF MATERIALS
BFC (Mechanics of Materials) Chapter 3: Stress in Beam
Bending Shear and Moment Diagram, Graphical method to construct shear
Shear Forces and Bending Moments in Beams
Dr. Ali I. Tayeh First Semester
CTC / MTC 222 Strength of Materials
CTC / MTC 222 Strength of Materials Final Review.
LRFD- Steel Design Dr. Ali I. Tayeh second Semester Dr. Ali I. Tayeh second Semester.
 2005 Pearson Education South Asia Pte Ltd 7. Transverse Shear 1 CHAPTER OBJECTIVES Develop a method for finding the shear stress in a beam having a prismatic.
3. Stresses in Machine Elements Lecture Number – 3.1 Prof. Dr. C. S. Pathak Department of Mechanical Engineering Sinhgad College of Engineering, Pune Strength.
Pure Bending of Straight Symmetrical Beams
CTC / MTC 322 Strength of Materials
Mechanics of Materials – MAE 243 (Section 002) Spring 2008 Dr. Konstantinos A. Sierros.
Chapter 4 Pure Bending Ch 2 – Axial Loading Ch 3 – Torsion
Mechanics of Materials – MAE 243 (Section 002) Spring 2008
Machine Design I (MCE-C 203) Mechatronics Dept., Faculty of Engineering, Fayoum University Dr. Ahmed Salah Abou Taleb Lecturer, Mechanical Engineering.
CTC / MTC 222 Strength of Materials Chapter 3 Design for Direct Stress.
Forging new generations of engineers
Chapter 4 Pure Bending Pure Bending Engr. Othman A. Tayeh.
Mechanics of Materials(ME-294)
Chapter 4 Pure Bending Ch 2 – Axial Loading Ch 3 – Torsion Ch 4 – Bending -- for the designing of beams and girders.
Chapter 4 Pure Bending Eng. Mahmoud AlQazzaz.
CTC / MTC 222 Strength of Materials
Chapter 6: Bending.
EGM 5653 Advanced Mechanics of Materials
Analysis and Design of Beams for Bending
Analysis and Design of Beams for Bending
Sample Problem 4.2 SOLUTION:
Chapter 6 Section 3,4 Bending Deformation, Strain and Stress in Beams
Pure Bending.
Stresses, Strains and Deflections of Steel Beams in Pure Bending
4 Pure Bending.
Structure I Course Code: ARCH 208 Dr. Aeid A. Abdulrazeg
Theory of Simple Bending
Sample Problem 4.2 SOLUTION:
Analysis and Design of Beams for Bending
Forging new generations of engineers
4 Pure Bending.
Bending Deformation of a Straight Member
Presentation transcript:

CTC / MTC 222 Strength of Materials Chapter 8 Stress Due to Bending

Chapter Objectives Compute the maximum bending stress in a beam using the flexure formula. Compute the bending stress at any point in a beam cross section. Determine the appropriate design stress and design beams to carry a given load safely

The Flexure Formula Positive moment – compression on top, bent concave upward Negative moment – compression on bottom, bent concave downward Maximum Stress due to bending (Flexure Formula) σmax = M c / I Where M = bending moment, I = moment of inertia, and c = distance from centroidal axis of beam to outermost fiber For a non-symmetric section distance to the top fiber, ct , is different than distance to bottom fiber cb σtop = M ct / I σbot = M cb / I Conditions for application of the flexure formula Listed in Section 8-3, p. 308

The Flexure Formula Conditions for application of flexure formula Beam is straight, or nearly straight Cross-section is uniform Beam is not subject to torsion Beam is relatively long and narrow in proportion to its depth Beam is made from a homogeneous material with equal moduli of elasticity in tension and compression Stress is below the proportional limit No part of beam fails from instability Location where stress is computed is not close to point of application of a concentrated load

Stress Distribution For a positive moment, top of beam is in compression and bottom is in tension Stress at centroidal axis (neutral axis) is zero Stress distribution within cross section is linear Magnitude of stress is directly proportional to distance from neutral axis Stress at any location in cross section due to bending σ = M y / I , where y = distance from neutral axis of beam to location in cross section

Section Modulus, S Maximum Stress due to bending σmax = M c / I Both I and c are geometric properties of the section Define section modulus, S = I / c Then σmax = M c / I = M / S Units for S – in3 , mm3 Use consistent units Example: if stress, σ, is to be in ksi (kips / in2 ), moment, M, must be in units of kip – inches For a non-symmetric section S is different for the top and the bottom of the section Stop = I / ctop Sbot = I / cbot

Stress Concentration Factors Changes in cross-section of a member can cause stress concentrations Stress concentration factor KT Depends on geometry of the member Can be measured experimentally, or by computerized analyses KT = σmax / σnom Solving for and σmax using σnom = M / S σmax = M KT / S See Sections 3-9, 8-9 and Appendix A-21

Flexure Center For the flexure formula to apply, the applied load must not cause the beam to twist The loads must pass through the flexural center or shear center, of the beam If section has an axis of symmetry, the shear center is on that axis If section doesn’t have an axis of symmetry, the shear center may be outside the limits of the section itself Example - Channel

Calculation of Design Stress Design stress (or allowable stress), σd Sometimes based on yield strength: σd = Sy / N Sometimes based on ultimate strength σd = Su / N Ductile Materials - >5% elongation before failure Static loads - σd = Sy / N , N = 2 Repeated loads - σd = Su / N , N = 8 Impact or shock load - σd = Su / N , N = 12 Brittle Materials - <5% elongation before failure Static loads - σd = Su / N , N = 6 Repeated loads - σd = Su / N , N = 10 Impact or shock load - σd = Su / N , N = 15 Design stresses for specific materials are specified in design codes Examples: AISC or Aluminum Association