BUCKLING OF COLUMNS. AIM To study the failure analysis of buckling of columns.

Slides:



Advertisements
Similar presentations
Stability of columns.
Advertisements

ENCE 455 Design of Steel Structures
CHAPTER OBJECTIVES Discuss the behavior of columns.
WORKSHEET 7 AXIALLY LOADED MEMBERS. Q1 Are tension structures or compression structures more efficient when loaded axially ? tension structures tension.
Indeterminate Structure Session Subject: S1014 / MECHANICS of MATERIALS Year: 2008.
Introduction to Axially Loaded Compression Members
2E4: SOLIDS & STRUCTURES Lecture 15 Dr. Bidisha Ghosh Notes: lids & Structures.
10 Columns.
Chapter 13 Buckling of Columns
2.2 STRUCTURAL ELEMENT Reinforced Concrete Column
Strength of Materials I EGCE201 กำลังวัสดุ 1
Chapter 4 AXIAL LOADING.
Column Design ( ) MAE 316 – Strength of Mechanical Components
Compression BADI Y1.
Buckling Critical Load Considerations
Compression Members.
Copyright © 2011 Pearson Education South Asia Pte Ltd
BFC (Mechanics of Materials) Chapter 5: Compression Member
ENGR 220 Section 13.1~13.2.
Axially loaded member Axial load and normal stress under equilibrium load, Elastic Deformation.
CHAPTER OBJECTIVES Discuss the behavior of columns.
Mukavemet II Strength of Materials II
Columns and Struts.
Chapter 10 Columns .
© Dr S R Satish Kumar, IIT Madras1 SECTION 7 DESIGN OF COMPRESSION MEMBERS.
Chapter Outline Shigley’s Mechanical Engineering Design.
Buckling of Slender Columns ( )
UNIT-05. Torsion And Buckling of columns
 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 Material-1 Introduction. Dr. Attaullah Shah.
COMPERSION MEMBER.  An initially straight strut or column, compressed by gradually increasing equal  and opposite axial forces at the ends is considered.
☻ 2.0 Bending of Beams sx 2.1 Revision – Bending Moments
Strength of Materials Malayer University Department of Civil Engineering Taught by: Dr. Ali Reza Bagherieh In The Name of God.
Unit-5. Torsion in Shafts and Buckling of Axially Loaded Columns Lecture Number-5 Mr. M. A.Mohite Mechanical Engineering S.I.T., Lonavala.
Strength of Materials I EGCE201 กำลังวัสดุ 1 Instructor: ดร. วรรณสิริ พันธ์อุไร ( อ. ปู ) ห้องทำงาน : 6391 ภาควิชาวิศวกรรมโยธา
☻ ☻ ☻ ☻ 2.0 Bending of Beams sx 2.1 Revision – Bending Moments
Mechanics of Materials -Beams
PLASTIC ANALYSIS OF BEAMS - SANDEEP DIGAVALLI. AT A GLANCE OF THIS TOPIC  BASIS OF PLASTIC THEORY  STRESS-STRAIN CURVE OF PLASTIC MATERIALS  STRESSES.
COLUMNS AND STRUTS.
Mechanics of Solids (M2H321546)
Columns and Struts.
SECTION 7 DESIGN OF COMPRESSION MEMBERS
Longitudinal Strain Flexure Formula
Solid Mechanics Course No. ME213.
Stress and Strain – Axial Loading
CHAPTER OBJECTIVES Discuss the behavior of columns.
10 Columns.
Buckling & Stability Critical Load
Mechanical Engineering
SECTION 7 DESIGN OF COMPRESSION MEMBERS
Unit-5. Torsion in Shafts and Buckling of Axially Loaded Columns
13.3 Columns with Various Types of Supports:
Structural Analysis 7th Edition in SI Units
Compression Members.
Buckling & Stability Critical Load
Theory of Simple Bending
Chapter 3 Buckling of Column SAIFULNIZAN JAMIAN.
Chapter 13 – Buckling of Columns
Compression Test of Steel Columns
Introduction – Concept of Stress
Axially loaded columns
CHAPTER OBJECTIVES Determine deformation of axially loaded members
( BDA ) CHAPTER V THICK CYLINDER
Chapter 6 Bending.
ENGINEERING MECHANICS
TORSION CO 2 : ABILITY TO ANALYZE TORQUE-LOADED MEMBER EVALUATE THE VALUES AND DISTRIBUTION OF BENDING AND SHEAR STRESSES IN BEAM SECTION By: ROSHAZITA.
10 Columns.
Mechanics of Materials Engr 350 – Lecture 38 Columns
Copyright ©2014 Pearson Education, All Rights Reserved
Presentation transcript:

BUCKLING OF COLUMNS

AIM To study the failure analysis of buckling of columns

BASIC DEFINITIONS ASSUMPTIONS & SIGN CONVENTIONS FAILURE ANALYSIS OF COLUMN WITH EULER EQUATION EFFECTIVE LENGTH AND SUPPORT CONDITION GRAPHICAL ANALYSIS OF STRESS VS SLENDERNESS RATIO RANKINE’S FORMULA AND ITS IMPORTANCE NUMERICAL PREVIEW

BASIC DEFINITIONS COLUMN Compressive member in vert position Consist of Short column Long column STRUTS Bar or member of structure acted upon by compressive load Eg: strut in truss, piston rods P P Short column Long column Compression/Crushing Bending / Buckling

BASIC DEFINITIONS STABLE/UNSTABLE EQUILIBRIUM Stable equilibrium: body in static equilibrium on being displaced slightly, returns to its original position Unstable equilibrium : body in equilibrium on being slightly disturbed, moves away from its equilibrium position NEUTRAL EQUILIBRIUM Body in equilibrium on being slightly disturbed, moves away from its equilibrium position and remains in the same position on removal of load Load acting- crippling/buckling/critical load unstable stable neutral

ASSUMPTIONS & SIGN CONVENTIONS Column is initially perfectly straight and the load is applied axially Uniform cross-section area Perfectly elastic and obeys Hooke’s law. homogeneous and isotropic Length very large as compared to its lateral dimensions Direct stress <<<bending stress Self-weight of column is negligible +ve Sign Convention Assumptions

The failure analysis on columns by buckling has been carried out for the fwg conditions FAILURE ANALYSIS OF COLUMN Le=0.5L P Le=L P Le=2L P Le=0.7L P Both ends hinged One end fixed other end free One end fixed other end hinged Both ends fixed

CONDITION I : BOTH ENDS HINGED Consider a column AB of length l hinged at both its ends A and B carries an axial crippling load at A. Consider any section X-X at a distance of x from B. Let the deflection at X-X is y.  The bending moment at X-X due to the load P, M = (-)P*y Where( ) Solution of this differential equation is P P XX y L B A x

(Now taking the least significant value (i.e)  ) By using Boundary conditions, At B, (x = 0, y = 0  A = 0) and At A,(x = l, y = 0) CONDITION I : BOTH ENDS HINGED Le=L P

CONDITION II : ONE END FIXED ONE END FREE Consider a column AB of length l, fixed at B and free at A, carrying an axial rippling load P at D de to which it just buckles. The deflected form of the column AB is shown in fig. Let the new position of A is A 1. Let a be the deflection at the free end. Consider any section X-X at a distance x from B. Let the deflection at xx is y. Bending moment due to critical load P at xx, B a a-y x y P a x

The solution of the above differential equation is, Where A and B are constants of integration. At B, x = 0, y = 0  A = -a Differentiating the equation ( w.r.t to x) At the fixed end B, x = 0 and CONDITION II : ONE END FIXED ONE END FREE

Substitute A = -a and B = 0 in equation (i) we get, At the free end A, x = l, y = a, substitute these values in equation (ii) (ii)  The crippling load for the columns with one end fixed and other end free. Le=2L P CONDITION II : ONE END FIXED ONE END FREE

CONDITION III : BOTH ENDS FIXED Solution of this differential equation is P P XX y L B A x M M B = 0 … on applying bdy condition ….On substitution and applying 2 nd bdy condition Le=0.5L P

CONDITION IV : FIXED/HINGED Differential equation Solution of differential equation Applying bdy condition P P X X y L B A x M M H

EFFECTIVE LENGTH AND SUPPORT CONDITION Pinned/PinnedFixed/FreeFixed/FixedPinned/Fixed Le = LLe = 2LLe = L/2Le = 0.7L Le=0.5L P Le=L P Le=2L P Le=0.7L P Both ends hinged One end fixed other end free One end fixed other end hinged Both ends fixed

The Euler formula was derived with the assumption that load is always applied through the centroid of the column & column is straight. Manufactured columns are never perfectly straight & begin to bend slightly upon the application of the load. To investigate this effect load, P is applied to the column at a short eccentric distance, e from the centroid of the cross section. SECANT FORMULA P P P P M=Pe e l l

Secant Formula SECANT FORMULA

GRAPHICAL ANALYSIS OF STRESS VS SLENDERNESS RATIO For a steel column if (L/r) ≥ 89, Euler’s formula can be used to determine the buckling load since the stress in the column remains elastic. (L/r) - Slenderness ratio. Buckling will occur about the axis when the ratio gives the greatest value. Critical stress= P(e)/A= (Π^2 ) EI/A*l(e)^2= (Π^2 ) E/(l(e)/k)^2 L/r FAILURE BY BUCKLING FAILURE BY CRUSHING

Euler’s formula long columns(buckling condition) Rankine’s formula applicable to all columns irrespective of whether they are short or long. If P is the crippling load by Rankine’s formula. P c is the crushing load of the column material P E is the crippling load by Euler’s formula. RANKINE’S FORMULA AND ITS IMPORTANCE 1/P= 1/Pe +1/Pc Also, 1/P=1/Pe(long columns) 1/P=1/Pc(short columns)

DERIVATION OF RANKINE GORDEN FORMULA Substitute the value of P c = f c A and where, f c =Ultimate crushing stress of the column material. A=Cross-sectional are of the column L=Effective length of the column I=Ak 2 Where k = Least radius of gyration. where  = Rankine’s constant P = Crushing Load

21.A column with alone end hinged and the other end fixed has a length of 5m and a hollow circular cross section of outer diameter 100 mm and wall thickness 10 mm. If E = 1.60 x 10 5,stress =350N/mm 2 and crushing strength, Find the load that the column may carry with a factor of safety of 2.5 according to Euler theory and Rankine – Gordon theory. If the column is hinged on one side and fixed on other, find the safe load according to the two theories. NUMERICAL ON BUCKLING OF COLUMN Given: Length= 5 m = 5000 mm Outer diameter D = 100 mm Inner diameter d = D-2t = 100 – 2 (10) = 80 mm Thickness = 10 mm E=1.60 x 10 5 N/mm 2 FOS= 2.5 Stress =350N/mm 2

1. Calculation of load by Euler’s theory: Column with one end fixed and other end hinged. (i) I = x 10 5 mm 4 By putting the value of I in the eqn (I), we get P = x 10 3 N NUMERICAL ON BUCKLING OF COLUMN

ii.Calculation of load by Rankine-Gordon theory: Rankine’s Constant (assume the column material is mild steel) K = least radius of gyration mKwhere Ans: Euler’s Theory P = x 10 4 N Rankine’s Theory P = x 10 4 N Safe Load= P/2.5 Euler’s Theory = N Rankine’s theory = N NUMERICAL ON BUCKLING OF COLUMN

BIBLIOGRAPHY content/uploads/sites NPTEL lectures

- END - Thank you