MECHANICS OF SOLIDS COMPRESSION MEMBERS TUTORIAL 2 INTERMEDIATE AND SHORT COMPRESSION MEMBERS

Similar documents
Engineering Science OUTCOME 1 - TUTORIAL 4 COLUMNS

ENGINEERING SCIENCE H1 OUTCOME 1 - TUTORIAL 4 COLUMNS EDEXCEL HNC/D ENGINEERING SCIENCE LEVEL 4 H1 FORMERLY UNIT 21718P

Lecture Notes: Finite Element Analysis, J.E. Akin, Rice University

UNCERTAINTY FOCUSED STRENGTH ANALYSIS MODEL

FEA Solution Procedure

Unit III Theory of columns. Dr.P.Venkateswara Rao, Associate Professor, Dept. of Civil Engg., SVCE, Sriperumbudir

FEA Solution Procedure

3 2D Elastostatic Problems in Cartesian Coordinates

Copyright Canadian Institute of Steel Construction

The Open Civil Engineering Journal

OUTCOME 1 - TUTORIAL 3 BENDING MOMENTS. You should judge your progress by completing the self assessment exercises. CONTENTS

FEA Solution Procedure

Formal Methods for Deriving Element Equations

Modelling by Differential Equations from Properties of Phenomenon to its Investigation

1. Solve Problem 1.3-3(c) 2. Solve Problem 2.2-2(b)

08.06 Shooting Method for Ordinary Differential Equations

DESIGN OF STRAP (CANTILEVER) FOOTINGS Design Steps and Equations

PhysicsAndMathsTutor.com

Shooting Method for Ordinary Differential Equations Autar Kaw

Section 7.4: Integration of Rational Functions by Partial Fractions

The Hashemite University Department of Civil Engineering ( ) Dr. Hazim Dwairi 1

Prandl established a universal velocity profile for flow parallel to the bed given by

1 The space of linear transformations from R n to R m :

ENGINEERING COUNCIL DIPLOMA LEVEL MECHANICS OF SOLIDS D209 TUTORIAL 3 - SHEAR FORCE AND BENDING MOMENTS IN BEAMS

1 JAXA Special Pblication JAXA-SP-1-E Small-scale trblence affects flow fields arond a blff body and therefore it governs characteristics of cross-sec

Civil Engineering Design (1) Design of Reinforced Concrete Columns 2006/7

Title. Author(s)ALAMIRI, M. ASSAD; GOTO, YOSHIAKI. Issue Date Doc URL. Type. Note. File Information

Details of Check for Boundary Element Requirements

Lab Manual for Engrd 202, Virtual Torsion Experiment. Aluminum module

MAHALAKSHMI ENGINEERING COLLEGE

DEVELOPMENT OF COMPONENT EXPLOSIVE DAMAGE ASSESSMENT WORKBOOK (CEDAW)

CHAPTER 4. Stresses in Beams

Entrance exam Master Course

Flexure of Thick Simply Supported Beam Using Trigonometric Shear Deformation Theory

Mechanics of Structure

UNIVERSITY OF BOLTON SCHOOL OF ENGINEERING. BEng (HONS) CIVIL ENGINEERING SEMESTER 1 EXAMINATION 2016/2017 MATHEMATICS & STRUCTURAL ANALYSIS

EXERCISES WAVE EQUATION. In Problems 1 and 2 solve the heat equation (1) subject to the given conditions. Assume a rod of length L.

ME 354, MECHANICS OF MATERIALS LABORATORY COMPRESSION AND BUCKLING

Name :. Roll No. :... Invigilator s Signature :.. CS/B.TECH (CE-NEW)/SEM-3/CE-301/ SOLID MECHANICS

Sources of Non Stationarity in the Semivariogram

DEFINITION OF A NEW UO 2 F 2 DENSITY LAW FOR LOW- MODERATED SOLUTIONS (H/U < 20) AND CONSEQUENCES ON CRITICALITY SAFETY

PhysicsAndMathsTutor.com

Chapter 2 Introduction to the Stiffness (Displacement) Method. The Stiffness (Displacement) Method

PREDICTABILITY OF SOLID STATE ZENER REFERENCES

Bending Stress. Sign convention. Centroid of an area

Higher Maths A1.3 Recurrence Relations - Revision

ENGINEERING COUNCIL DYNAMICS OF MECHANICAL SYSTEMS D225 TUTORIAL 2 LINEAR IMPULSE AND MOMENTUM

AMS 212B Perturbation Methods Lecture 05 Copyright by Hongyun Wang, UCSC

Discontinuous Fluctuation Distribution for Time-Dependent Problems

E ect Of Quadrant Bow On Delta Undulator Phase Errors

FRTN10 Exercise 12. Synthesis by Convex Optimization

Relativity II. The laws of physics are identical in all inertial frames of reference. equivalently

STEP Support Programme. STEP III Hyperbolic Functions: Solutions

Advanced topics in Finite Element Method 3D truss structures. Jerzy Podgórski

Computational Fluid Dynamics Simulation and Wind Tunnel Testing on Microlight Model

Principles of Minimum Cost Refining for Optimum Linerboard Strength

Study on the impulsive pressure of tank oscillating by force towards multiple degrees of freedom

PES Institute of Technology

UNIVERSITY OF SASKATCHEWAN ME MECHANICS OF MATERIALS I FINAL EXAM DECEMBER 13, 2008 Professor A. Dolovich

A Single Species in One Spatial Dimension

and F NAME: ME rd Sample Final Exam PROBLEM 1 (25 points) Prob. 1 questions are all or nothing. PROBLEM 1A. (5 points)

Chapter 6 Momentum Transfer in an External Laminar Boundary Layer

Structural Analysis I Chapter 4 - Torsion TORSION

PIPELINE MECHANICAL DAMAGE CHARACTERIZATION BY MULTIPLE MAGNETIZATION LEVEL DECOUPLING

Math 144 Activity #10 Applications of Vectors

Properties of Sections

Resetting and termination of reentry in a loop-and-tail cardiac model

JUT!SI I I I TO BE RETURNED AT THE END OF EXAMINATION. THIS PAPER MUST NOT BE REMOVED FROM THE EXAM CENTRE. SURNAME: FIRST NAME: STUDENT NUMBER:

EXPT. 5 DETERMINATION OF pk a OF AN INDICATOR USING SPECTROPHOTOMETRY

3.3 Operations With Vectors, Linear Combinations

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 4 Pure Bending Homework Answers

CIVIL DEPARTMENT MECHANICS OF STRUCTURES- ASSIGNMENT NO 1. Brach: CE YEAR:

Chapter 1: Differential Form of Basic Equations

Nonlinear parametric optimization using cylindrical algebraic decomposition

CONTENTS. INTRODUCTION MEQ curriculum objectives for vectors (8% of year). page 2 What is a vector? What is a scalar? page 3, 4

Lecture 7 Waveguides. TC 412 Microwave Communications

MECHANICS OF SOLIDS - BEAMS TUTORIAL 1 STRESSES IN BEAMS DUE TO BENDING

Sample Question Paper

1 Differential Equations for Solid Mechanics

1. INTRODUCTION. A solution for the dark matter mystery based on Euclidean relativity. Frédéric LASSIAILLE 2009 Page 1 14/05/2010. Frédéric LASSIAILLE

COMPLEX STRESS TUTORIAL 4 THEORIES OF FAILURE. You should judge your progress by completing the self assessment exercises.

4 Exact laminar boundary layer solutions

FREQUENCY DOMAIN FLUTTER SOLUTION TECHNIQUE USING COMPLEX MU-ANALYSIS

Simplified Identification Scheme for Structures on a Flexible Base

Pulses on a Struck String

Comparison of Euler Theory with Experiment results

Assignment Fall 2014

WEAR PREDICTION OF A TOTAL KNEE PROSTHESIS TIBIAL TRAY

Objectives: We will learn about filters that are carried out in the frequency domain.

3.4-Miscellaneous Equations

Chapter 9 Flow over Immersed Bodies

FIXED BEAMS IN BENDING

Setting The K Value And Polarization Mode Of The Delta Undulator

IDE 110 Mechanics of Materials Spring 2006 Final Examination FOR GRADING ONLY

Static Failure (pg 206)

4.MECHANICAL PROPERTIES OF MATERIALS

sin u 5 opp } cos u 5 adj } hyp opposite csc u 5 hyp } sec u 5 hyp } opp Using Inverse Trigonometric Functions

3.5 Analysis of Members under Flexure (Part IV)

Technical Note. ODiSI-B Sensor Strain Gage Factor Uncertainty

On the tree cover number of a graph

Transcription:

MECHANICS O SOIDS COMPRESSION MEMBERS TUTORIA INTERMEDIATE AND SHORT COMPRESSION MEMBERS Yo shold jdge yor progress by completing the self assessment exercises. On completion of this ttorial yo shold be able to do the following. Define an intermediate compression member. Derive and se the Rankine Gordon formlae. Solve the loads at which members fail. Define a colmn. Calclate the stresses in a colmn with an offset load. Calclate the position of the netral axis in a colmn with an off set load. It is assmed that stdents doing this ttorial already familiar with the concepts of second moments of area, bending stress, bending moments and deflection of beams. Stdents shold stdy the ttorial on strts before starting this one. D.J.DUNN 1

INTRODUCTION Yo shold recall that compression members fall into three grops, long (strts) intermediate and short (colmns). irst we need to now that a material may fail de to exceeding the ltimate (maximm) compressive stress. This is often referred to as the crshing stress. If this was the only factor casing failre the load that prodces it wold be given by the formla = A = Ultimate compressive load = ltimate compressive stress A = cross sectional area. In reality, there is often bending associated with the failre and this is especially tre with intermediate members. 1. INTERMEDIATE COMPRESSION MEMBERS It is fond that steel strts with a slenderness ratio of 80 to 10 fail at smaller loads than predicted by Eler. These are intermediate compression members in which compression and bending have an effect on failre. 1.1 RANKINE - GORDON THEORY GORDON sggested that for sch members, an empirical formla be sed (based on experimental data). RANKINE modified Gordon's formla. The following shows the reasoning for this formla. π EI E = Eler's critical load. and this applies to strts. = Ultimate compressive load = A and this applies to colmns. = ltimate compressive stress. A = cross sectional area. Rankine sggested that an intermediate compression member fails de to both bckling and compression to more or less degrees. Based on experimental data, it is fond that a reasonable prediction of the load at failre is given by the reciprocal formla. 1 1 1 E This rearranges to R E R = Rankine s Critical load. R E D.J.DUNN

The formla indicates that for slender members E dominates and for short members dominates. URTHER DEVEOPMENT Consider the frther development of Eler's formla for strts. Slendernes s Ratio S.R. Rearrange to make I the sbject k I A (S.R.) A I π EI Eler' s critical load for strtsis E Sbstitte the above formla for I nto this. π EA π EA E k k If we divide by thecross sectional area we convert the force into a nominal stress called Eler' s critical A I (S.R.) stress A k E E π E π Ek E...(1) A k If we plot this stress against slenderness ratio we get the reslt shown on figre 1. The graph is called Eler's Hyperbola. Next we consider the frther development of the Rankine formla. Sbstitte the following into Rankine s formla. = A e = EI/ R e e k A EA n EAn k A D.J.DUNN 3

D.J.DUNN 4 E where...() 1 A E 1 A EA n A a n k a k A k EA n R R Althogh there is a theoretical vale for the constant a based on material properties, it is sal to determine it from experiment. The experimental vale varies slightly from the theoretical. Typical vales of a are Material MPa a Mild Steel 35 1/7500 Wroght Iron 47 1/9000 Cast Iron 557 1/1600 Timber 35 1/3000 GRAPHICA REPRESENTATION The diagram shows E (eqation ) and R (eqation 1) plotted against slenderness ratio. The ltimate compressive stress is marked on the stress axis. The reslt shows how R tends to as the member becomes short and tends to E as the member gets longer. The region of interest is arond the S.R. = 80 point where the correct stress lays between the other two vales. igre 1

WORKED EXAMPE No.1 ind the Rankine critical load for a strt with an I section as shown given = 35 MPa, E = 05 MPa and = 16 m. The strt is bilt in rigidly at each end. SOUTION igre The strt will bend abot the axis of minimm resistance and hence minimm I so we mst determine which is the minimm I. HORIZONTA N-A The section is symmetrical so sbtract I for the two ct ots from the vale for the oter rectangle. Remember that for a rectangle I = BD 3 /1 abot its centre line. or the oter rectangle I = 50 x 30 3 /1 = 68.67 x 10 6 mm 4 or one ct ot I = 10 x 300 3 /1 = 70 x 10 6 mm 4 or the section I = 68.67 x 10 6 x 70 x 10 6 = 14.66 x 10 6 mm 4 VERTICA N-A Treat this as three rectangles and add them together. Two ends I = x 10 x 50 3 /1 = 6.04 x 10 6 mm 4 Middle I = 300 x 10 3 /1 = 5000 mm 4 Add together I = 6.06 x 10 6 mm 4 The minimm I is abot the vertical axis so se I = 6.06 x 10 6 mm 4 A = (50 x 10) x + (300 x 10) = 8000 mm. k = (I/A) = (6x10 6 /8000) = 57 mm mode n = a = 0.00016 6 6 A 8000x10 x35x10 R a k 1 n 66.kN 0.00016 1 16 0.057 D.J.DUNN 5

SE ASSESSMENT EXERCISE No.1 1. A strt is 0. m diameter and 15 m long. It is pinned at both ends. Calclate Eler's critical load. Take E = 05 GPa (Answer 706.5 kn). A strt has a rectanglar section 0. m x 0.1 m. It is 8 m long. The bottom is bilt in and the top is free. Dring a test, it bckled at 164 kn. Given the ltimate compressive stress of the material is 345 MPa : Calclate the Rankine constant "a". (0.000133) A second strt made of the same material has a rectanglar section 0.3 m x 0.m. It is 6 m long and pinned at both ends. Using the constant a fond previosly, find the Rankine bckling load. (Answer 8.5 MN) D.J.DUNN 6

. COUMNS A colmn is a thick compression member. Strts fail de to bending bt colmns fail in compression. Colmns are sally made of brittle material which is strong in compression sch as cast iron, stone and concrete. These materials are weak in tension so it is important to ensre that bending does not prodce tensile stresses in them. If the compressive stress is too big, they fail by crmbling and cracking OSET OADS igre 3 Colmns often spport offset loads and these prodce bending stresses that combine with the compressive stress. This is illstrated in figre 4. igre 4 If a load is applied on the centre of the section, the stress in the colmn will be a direct compressive stress given by D = - /A Remember that compressive stresses are always negative. When the load is applied a distance 'x' from the centroid, a bending moment is indced in the colmn as shown. The bending moment is M = x where x is the off set distance. D.J.DUNN 7

rom the well known formla for bending stress we have B = My/I y is the distance from the centroid to the edge of the colmn. The stress prodced will be +ve (tensile) on one edge and -ve (compressive) on the other. On the compressive edge this will add to the direct compressive stress making it larger so that = B + D = -My/I - /A On the tensile edge the reslting stress is Sbstitte M = x = B + D = My/I - /A = = xy/i - /A WORKED EXAMPE No. A colmn is 0.5 m diameter and carries a load of 500 kn offset from the centroid by 0.1m. Calclate the extremes of stresses. SOUTION = 500 kn x = 0.1 m y = D/ = 0.5 m Tensile Edge = B + D = xy/i - /A = 500 000 x 0.1 x 0.5 /( x 0.54/64) - 500 000/( x 0.5/4) = 1.58 MPa (Tensile) Compressive Edge = B + D = -xy/i - /A = -500 000 x 0.1 x 0.5 /( x 0.54/64) - 500 000/( x 0.5/4) = -6.61MPa (compressive) D.J.DUNN 8

NEUTRA AXIS The netral axis is the axis of zero stress. In the above example, the stress varied from 1.58 MPa on one edge to -6.61 MPa on the other edge. Somewhere in between there mst a vale of y which makes the stress zero. This does not occr on the centroid bt is by definition the position of the netral axis. Ideally this axis shold not be on the section at all so that no tensile stress occrs in the colmn. The position of the netral axis can easily be fond by drawing a stress distribtion diagram and then either scaling off the position or calclate it from similar triangles. WORKED EXAMPE No.3 Determine the position of the netral axis for the colmn in example. SOUTION Drawing a graph of stress against position (y) along a diameter we get the figre shown (not drawn to scale). If it is drawn to scale the position of the netral axis may be scaled off. igre 5 Using similar triangles we arrive at the soltion as follows. A + B = 0.5 A = 0.5 - B A/1.58 = B/6.61 (0.5 - B)/1.58 = B/6.61 3.3105-6.61B = 1.58 B B = 0.406 m D.J.DUNN 9

SE ASSESSMENT EXERCISE No. 1. A colmn is 0.4 m diameter. It has a vertical load of 300 kn acting 0.05m from the centroid. Calclate the stresses on the extreme edges. (Answers 0 MPa and -4.77 MPa).. A colmn of diameter D has an offset load. Show that if the stress on one edge is zero, the offset position is D/8. 3. A colmn is made from cast iron tbe 0.4 m otside diameter with a wall 40 mm thick. The top is covered with a flat plate and a vertical load of 70 kn is applied to it. Calclate the maximm allowable offset position of the load if the material mst always remain in compression. (Answer 0.08 m) 4. A hollow cast iron pillar, 38 cm otside diameter and wall thickness 7.5 cm, carries a load of 75 kn along a line parallel to, bt displaced 3 cm from, the axis of the pillar. Determine the maximm and minimm stresses in the pillar. What is the maximm allowable eccentricity of the load relative to the axis of the pillar if the stresses are to be compressive at all points of the cross section? D.J.DUNN 10