International Journal of Scientific & Engineering Research, Volume 4, Issue 10, October ISSN

Similar documents
Unit 18 Other Issues In Buckling/Structural Instability

G Venkateswara Rao* Structural Engineering Group, Vikram Sarabhai Space Centre, Trivandrum , India

First-Order Solutions for the Buckling Loads of Euler-Bernoulli Weakened Columns

VORONOI APPLIED ELEMENT METHOD FOR STRUCTURAL ANALYSIS: THEORY AND APPLICATION FOR LINEAR AND NON-LINEAR MATERIALS

Iraq Ref. & Air. Cond. Dept/ Technical College / Kirkuk

Design Project 1 Design of a Cheap Thermal Switch

Post Graduate Diploma in Mechanical Engineering Computational mechanics using finite element method

The Homotopy Perturbation Method for free vibration analysis of beam on elastic foundation

Critical Load columns buckling critical load

Buckling of Tapered Columns with Polygon Cross-Section

Chapter 12 Elastic Stability of Columns

Effect of Specimen Dimensions on Flexural Modulus in a 3-Point Bending Test

Mechanics of Inflatable Fabric Beams

ME 1401 FINITE ELEMENT ANALYSIS UNIT I PART -A. 2. Why polynomial type of interpolation functions is mostly used in FEM?

ANALYSIS OF YARN BENDING BEHAVIOUR

Analytical Strip Method for Thin Isotropic Cylindrical Shells

Question 1. Ignore bottom surface. Solution: Design variables: X = (R, H) Objective function: maximize volume, πr 2 H OR Minimize, f(x) = πr 2 H

Lecture 4 Honeycombs Notes, 3.054

Experimental investigation on monotonic performance of steel curved knee braces for weld-free beam-to-column connections

CHAPTER 14 BUCKLING ANALYSIS OF 1D AND 2D STRUCTURES

Open Access Prediction on Deflection of V-core Sandwich Panels in Weak Direction

Influence of residual stresses in the structural behavior of. tubular columns and arches. Nuno Rocha Cima Gomes

Analysis of Axially Loaded Non-prismatic Beams with General End Restraints Using Differential Quadrature Method

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

Simulation of Geometrical Cross-Section for Practical Purposes

MIXED RECTANGULAR FINITE ELEMENTS FOR PLATE BENDING

Bending Load & Calibration Module

Module 2 Selection of Materials and Shapes. IIT, Bombay

2766. Differential quadrature method (DQM) for studying initial imperfection effects and pre- and post-buckling vibration of plates

Comb resonator design (2)

A HIGHER-ORDER BEAM THEORY FOR COMPOSITE BOX BEAMS

ME 323 Examination #2 April 11, 2018

Correction of local-linear elasticity for nonlocal residuals: Application to Euler-Bernoulli beams

Computational Analysis for Composites

Passive Damping Characteristics of Carbon Epoxy Composite Plates

A Piezoelectric Screw Dislocation Interacting with an Elliptical Piezoelectric Inhomogeneity Containing a Confocal Elliptical Rigid Core

Formulation of Equivalent Steel Section for Partially Encased Composite Column under Concentric Gravity Loading

Free transverse vibrations of cracked nanobeams using a nonlocal elasticity model

Thermal buckling and post-buckling of laminated composite plates with. temperature dependent properties by an asymptotic numerical method

VIBRATION CONTROL OF RECTANGULAR CROSS-PLY FRP PLATES USING PZT MATERIALS

A Study on the Tube of Integral Propeller Shaft for the Rear-wheel Drive Automobile Using Carbon Composite Fiber

needed to buckle an ideal column. Analyze the buckling with bending of a column. Discuss methods used to design concentric and eccentric columns.

7.5 Elastic Buckling Columns and Buckling

Free vibration analysis of beams by using a third-order shear deformation theory

2018. Nonlinear free vibration analysis of nanobeams under magnetic field based on nonlocal elasticity theory

Chapter 5 Elastic Strain, Deflection, and Stability 1. Elastic Stress-Strain Relationship

Closed-form solution of linear buckling for tapered tubular columns with constant thickness

Chapter 2 Examples of Optimization of Discrete Parameter Systems

Geometry-dependent MITC method for a 2-node iso-beam element

A new computational method for threaded connection stiffness

COURSE TITLE : APPLIED MECHANICS & STRENGTH OF MATERIALS COURSE CODE : 4017 COURSE CATEGORY : A PERIODS/WEEK : 6 PERIODS/ SEMESTER : 108 CREDITS : 5

ME 354, MECHANICS OF MATERIALS LABORATORY COMPRESSION AND BUCKLING

Collapse behaviour and simplified modeling of triangular cross-section columns

Bending Analysis of a Cantilever Nanobeam With End Forces by Laplace Transform

Comb Resonator Design (2)

Cone-shaped socket connections for cylindrical members

Nonlinear bending analysis of laminated composite stiffened plates

Free Vibrations of Timoshenko Beam with End Mass in the Field of Centrifugal Forces

Static and free vibration analysis of carbon nano wires based on Timoshenko beam theory using differential quadrature method

Dual and Optimality Criteria Methods 9

Small-Scale Effect on the Static Deflection of a Clamped Graphene Sheet

1859. Forced transverse vibration analysis of a Rayleigh double-beam system with a Pasternak middle layer subjected to compressive axial load

FREE VIBRATIONS OF UNIFORM TIMOSHENKO BEAMS ON PASTERNAK FOUNDATION USING COUPLED DISPLACEMENT FIELD METHOD

Transactions of the VŠB Technical University of Ostrava, Mechanical Series. article No Roland JANČO *

1.050: Beam Elasticity (HW#9)

APPLICATION OF VARIATIONAL METHODS AND GALERKIN METHOD IN SOLVING ENGINEERING PROBLEMS REPRESENTED BY ORDINARY DIFFERENTIAL EQUATIONS

CWR track vibration characteristics varying with the change of supporting condition

Material Selection of Compliant Mechanism for Vibration Isolation

: APPLIED MECHANICS & STRENGTH OF MATERIALS COURSE CODE : 4021 COURSE CATEGORY : A PERIODS/ WEEK : 5 PERIODS/ SEMESTER : 75 CREDIT : 5 TIME SCHEDULE

INVESTIGATING THERMAL EFFECTS IN NONLINEAR BUCKLING ANALYSIS OF MICRO BEAMS USING MODIFIED STRAIN GRADIENT THEORY *

QUESTION BANK SEMESTER: III SUBJECT NAME: MECHANICS OF SOLIDS

PLATE GIRDERS II. Load. Web plate Welds A Longitudinal elevation. Fig. 1 A typical Plate Girder

Presented By: EAS 6939 Aerospace Structural Composites

Optimization of Isogrid Rib-Pattern on Mechanical Housing

Stability of Functionally Graded Plate under In-Plane Time-Dependent Compression

Longitudinal buckling of slender pressurised tubes

NON LINEAR BUCKLING OF COLUMNS Dr. Mereen Hassan Fahmi Technical College of Erbil

PES Institute of Technology

Finite Element Simulation of Bar-Plate Friction Welded Joints Steel Product Subjected to Impact Loading

Advanced Vibrations. Distributed-Parameter Systems: Exact Solutions (Lecture 10) By: H. Ahmadian

The problem of isotropic rectangular plate with four clamped edges

Buckling Analysis of Axially Compressed Square Elastic Tubes with Weakly Supported Edges

Parametric study on the transverse and longitudinal moments of trough type folded plate roofs using ANSYS

William J. McCutcheon U.S. Department of Agriculture, Forest Service Forest Products Laboratory Madison, Wisconsin 53705

Materials: engineering, science, processing and design, 2nd edition Copyright (c)2010 Michael Ashby, Hugh Shercliff, David Cebon.

CO-ROTATIONAL DYNAMIC FORMULATION FOR 2D BEAMS

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

ENG2000 Chapter 7 Beams. ENG2000: R.I. Hornsey Beam: 1

INFLUENCE OF FLANGE STIFFNESS ON DUCTILITY BEHAVIOUR OF PLATE GIRDER

Regression-Based Neural Network Simulation for Vibration Frequencies of the Rotating Blade

9.1 Introduction to bifurcation of equilibrium and structural

For more Stuffs Visit Owner: N.Rajeev. R07

REPORT TO D-FLEX LTD APRIL 2009 REPORT. (to D-Flex Ltd, NWDA Innovation Vouchers Award, 28 April 2009)

Retrospectives on My Studies of Solid Mechanics (II)

Numerical simulation of delamination onset and growth in laminated composites

Chapter 4 Deflection and Stiffness

Nonlocal material properties of single walled carbon nanotubes

Downloaded from Downloaded from / 1

Some Aspects Of Dynamic Buckling of Plates Under In Plane Pulse Loading

Investigation of Circular Flexural Hinge Used in Compliant Mechanism Using FEA Tool.

Transcription:

International Journal of Scientific & Engineering Research, Volume 4, Issue 0, October-203 956 Optimum Design for Minimum Mass Configuration Of Stepped Cantilever Compound Columns With Constraint On Axial Buckling Load V. Sridhar Patnaik *, G. Venkateswara Rao $ and A.V.S.S.K.S. Gupta + Abstract--This paper presents a mathematical programming technique for obtaining minimum weight (volume) of a two stepped cantilever column, subjected to axial load constraint. Optimum configurations of circular cross-sections for isotropic column of single material and compound columns made of two different materials in each segment of step, subjected to constant axial load, are designed for the ratios of stepped diameters and segment length. This problem is optimized under equality constraints as well as specified lower and upper bounds. The evaluation of the objective function requires the solution of the buckling problem of column with variable ratios of length (L 2 /L) and stepped diameters (d /d 2 ), subjected to a given axial buckling load. This problem is solved by using the Kuhn-Tucker method for the defined objective function with defined variables. Besides its accuracy yields a minor error as compared with FEM solution, overcomes the shortcomings of FEM solution, which would require resizing of elements and recomputation of their stiffness properties during optimization process. Index Terms: Buckling; two stepped columns; compound column; different materials; buckling load constraint; minimum mass configuration; optimum design. * Associate Professor, Department of Mechanical Engineering, VITAM college of Engineering, Visakhapatnam 53 73, India $ + Research Professor, Department of Mechanical Engineering, Vardhaman College of Engineering, Shamshabad, Hyderabad 50 28, India. Corresponding author, email: hydrao944@yahoo.co.in Professor, Department of Mechanical Engineering, Jawaharlal Nehru Technological University, Hyderabad 500 085, India 203

International Journal of Scientific & Engineering Research, Volume 4, Issue 0, October-203 957 INTRODUCTION In the present study, structures made of different combinations of materials, like composite and compound structures, such as beams and plates, are taken for analysis, due to their significance in many engineering applications. Also the design of structures with minimum weight configuration has attracted the interest of researchers. Automated design of large scale structures subjected to the frequency and buckling load constraints were dealt in the works as reported in the research works [],[2],[3],[4]. The closed form solution in optimizing the volume of cantilever column subjected to concentrated tip load with a linear buckling load constraint is discussed in the works of J.Kiusalaas and G.B.Reddy [5] and I.Tadjbaksh and T.B.Keller [6]. FEM based optimality criterion approach for minimum weight of a cantilever column, is reported in the works of G. Venkateswara Rao and R.Narayanaswami [7]. The present authors discussed earlier the benefits of stepped beams with two different cross sections, made of single material or two different materials through a parametric study, subjected to buckling load constraint, are reported in the research works of [8],[9]. A variation formulation is developed which forms the basis for the finite element analysis for the post buckling analysis of cantilever columns, dealt in [0]. A method is presented to obtain absolute design variables from the converged design vector obtained through the resizing formula. Lee and Choi [] investigated thermal buckling and post buckling behavior of composite beam for the purpose of increasing the critical buckling temperature and reducing the lateral deflection for the thermal buckling. The effect of modulus ratio and length to thickness ratio on the critical thermal load was studied in the works of Aydog du [2] and Khdeir [3]. Shape optimization is done to optimize the buckling load of a Euler-Bernoulli beam, keeping volume constant, with variable stiffness, is solved by using analog equation method for the fourth -order ordinary differential equation, is presented in the works of J.T.Katsikadelis, and G.C.Tsiatas [4]. The difficulty in joining of the different materials efficiently in the manufacturing of compound columns is overcome by the modern welding techniques, namely friction welding, friction stir welding, explosive welding, cold roll welding and resistance spot welding, which are dealt in the research works reported in [7], [8], [9]. STATEMENT OF A PROBLEM In the present study, the formulation presented is for the two stepped cantilever column of single material as shown in Fig. a and the compound columns of two different materials, having two segments of lengths L and L 2, with free-clamped ends as shown in Fig. b. In the case of the two materials, the 203

International Journal of Scientific & Engineering Research, Volume 4, Issue 0, October-203 958 segment of length L 2 and area A 2 is made of a material having higher modulus of elasticity such as steel, copper and titanium as shown in Fig. b. The admissible function for the lateral displacement Y satisfying the geometric boundary conditions in non-dimensional form is given by Y = a cos πx () 2L The boundary conditions considered for the cantilever column are Y = dy = 0 at x = 0 dx d 2 y = d3 y dx 2 dx 3 = 0 at x = L (2) By using energy method, an expression for buckling load for a cantilever compound column obtained is as P = π2 E 2 I 2 4L 2 ζ+( ζ)i 2 E 2 π (3) I2E2 sin ζπ Where ζ = L 2 /L and L +L 2 =L The expressions for buckling load, worked out to be in non-dimensional form as λ LM = PL2 = π2 E 2 I 2 4 ζ+( ζ) π (4) I2E2 sin ζπ I 2E 2 According to the scope of this paper, the objective function for the stepped compound cantilever column as shown in Fig. b is To minimize mass per unit length M = π 4 ρ 2 d 2 ρ 2 ( ζ) + d 2 2 ζ (5) To buckle with the maximum load, the constraint equation for buckling axial load, P = P can be stated as P Θ = ζ 4 + ( ζ) 4 d 2 E 2 d π Where P Θ = 0.28E 2 P L 2 E 2 d 4 d 2 4 sin ζπ (6) The Kuhn-Tucker conditions by differentiating objective function (5) and constraint (6) with respect to the design variables d, d2, and ζ We get 203

International Journal of Scientific & Engineering Research, Volume 4, Issue 0, October-203 959 M d + λ PΘ d = 0 (7) M d 2 + λ PΘ d 2 = 0 (8) M ζ + λ PΘ ζ = 0 (9) Eliminating λ from equations (7) and (8) and simplifying, we get the generalized equation for the ratio of stepped diameters d 2 = ζ ζ sin ζπ π ( ζ) ζ+ π sin ζπ E 2 /6 (0) Solution Procedure. The solution of the (0), i.e. stepped diametral ratio, d 2 is determined for the known values of the modulus ratio (E 2 ) by varying length ratio (ζ=l 2 /L). 2. The design parameter d 2 is obtained from the evaluated diametral ratio, d 2 for the known diameter (d ) of segment of such that it is satisfying (3) for the known values of constrained buckling load (P * ) and area moment of inertia (I ) of segment. 3. Mass of the beam is calculated for the values of d, d2, ζ, ρ 2 and ρ 2 by using (5). 3. As can be seen, the values in Table 2, reference values show good agreement with the present solutions. (less than 4% error) NUMERICAL RESULTS AND DISCUSSION Using the generalized expression for the diametric ratio (d 2 ) which expressed in the terms of length ratio ζ and modulus ratio, E 2 developed in the preceding section, a two stepped cantilever compound column,subjected to an end concentrated compressive load, is evaluated for the minimum weight configuration. In the present analysis, the length of the column is taken as 0.254m (00 in) and the diameter of the aluminum segment is 30.48mm (.2in). The buckling load constraint (P * ) considered for all the material configurations, is 453.59 kgf (000lb). The material properties, namely, the Young s modulus and density of aluminum, copper, steel and titanium, considered in this analysis are presented in Table. 203

International Journal of Scientific & Engineering Research, Volume 4, Issue 0, October-203 960 Table 2 shows comparison of the minimum weights of the two stepped cantilever compound column, made of steel or different material combinations, namely, steel-aluminum, copper-aluminum and titanium-aluminum, which give the same constraint buckling load. The minimum mass obtained for stepped steel column from the present study is 4.925kg, compared with that of through continuum analysis [6] and finite element based optimality approach [7], and found to be 3.5% and 2.4% respectively higher. The present results for minimum masses of compound columns are showing more accuracy, when compared with that of from [8], [9]. It is seen from the table 2 that for the same constraint load, the minimum mass for titanium-aluminum compound column is showing least among the other combinations of materials. And also observed to be 3.2% saving in minimum mass for stepped compound aluminum steel column with reference to the mass of stepped steel column. CONCLUSIONS The optimality for minimum mass configuration developed for a two stepped cantilever column for the design variables of length ratio, diameters ratio and modulus ratio in this paper, is applicable for any combinations of two different materials. The present solutions have shown good agreement with the reference values. The advantage of this concept is that the manufacturing process involved in obtaining a desired continuous change of the area moment of inertia of the column (beam) is avoided by using compound column (beam). The same analysis on a stepped steel column shows the advantage of using a stepped compound column. This shows that if the steps are more, the geometric constraint becomes milder and the value obtained for the optimum mass of the multi-stepped beam will be closer to the exact value, when compared to the present two stepped configuration. ACKNOWLEDGMENT The authors gratefully acknowledge the managements of the respective Institutes for their constant encouragement during the course of this work. NOTATION L, L2 : Stepped lengths of the beam 203

International Journal of Scientific & Engineering Research, Volume 4, Issue 0, October-203 96 L : Total length of the beam L 2 : Length ratio (ζ) L d, d 2 : Diameters of stepped lengths L and L 2 respectively A, A 2 : Cross-sectional areas of stepped lengths L and L 2 respectively E, E 2 : Young s modulii of stepped lengths L and L 2 respectively ρ, ρ 2 : Densities of stepped lengths L and L 2 respectively I, I 2 : Area moment of inertias of stepped lengths L and L 2 respectively d 2 : Stepped diametral ratio, d d 2 A 2 : Area ratio, A A 2 I I 2 : Inertia ratio, I2 E 2 E : Modulus of ratio, E2 ρ ρ 2 : Density ratio, ρ2 M : Mass of the beam P : Axial end concentrated compressive load P * : Constraint value of the buckling load W : Lateral displacement λ LM : Non dimensional Buckling load parameter REFERENCES. V. B. Venkayya, N. S. Khot and L. Berke, Application of optimality criteria approaches to automated design of large practical structures, AGARD-CP-23. 3-I-3-9, 973. 2. L. Berke and N. S. Knot, Use of optimality criteria methods for large scale systems, AGARD-LS-70. l-l-l-29,974. 3. N. S. Khot, V. B. Venkayya and L. Berke, Optimum design of composite structures with stress and displacement constraints, AIAA J. 4, 3-32, 976. 4. N. S. Khot, V. B. Venkayya and L. Berke, Optimum structural design with stability constraints, Int. J. Num. Met. Engng, 0, 097-l II4, 976. 203

International Journal of Scientific & Engineering Research, Volume 4, Issue 0, October-203 962 5. J. Kiusalaas and G. B. Reddy, DESAP2-a structural design program with stress and buckling constraints, Volume : Theoretical and User s Manual. NASA CR-2797, 977. 6. I. Tadjbakhsh and J. B. Keller, Strongest columns and Iso parametric inequalities for eigenvalues, Transactions of the ASME 84.59-I64, 962. 7. G. Venkateswara Rao and R.Narayanaswami, Optimum design of cantilever columns in the post buckling region with constraint on axial load-an optimality criterion approach, computers and structures, vol.2, pp.843-848, 980. 8. G.VenkateswaraRao,V.Sridhar patnaik and A.V.S.S.K.S.Gupta, Near optimum configuration of stepped hinged beams with buckling load constraint, Journal of Structural Engineering, Vol. 40, No. 2, pp. 05-4 No. 40-5, 203. 9. G.VenkateswaraRao,V.Sridhar patnaik and A.V.S.S.K.S.Gupta, Minimum mass design of compound cantilever columns with buckling load constraint through numerical search, Int. J. Mech. Eng. & Rob. Res., Vol., No. 2, pp.96-206, 202. 0. G.VenkateswaraRao. and P.C.Raju, Post-buckling of uniform cantilever columns-galerkin finite element solution, Engng. Fracture Mech. 9, l-4, 977.. J.J.Lee, and S.Choi,, Thermal buckling and post buckling analysis of a laminated composite beam with embedded SMA actuators, Comp. Struct.. Vol. 47,695-703, 999. 2. M.Aydogdu, Thermal buckling analysis of cross-ply laminated composite beams with general boundary conditions, Comp. Sci. and Tech.. vol. 67, 096-04, 2007. 3. A.A.Khdeir, Thermal buckling of cross-ply laminated composite beams, Acta Mech. vol. 49, 20-23, 200. 4. J.T.Katsikadelis., and G.C.Tsiatas, Buckling load optimization of beams, Arch Applied mechanics,74:790-799. 5. S. P. Timoshenko and J. M. Gere, Theory of Elastic stability, McGraw-Hill. New York, 96. 6. 0. C. Zienkiewicz, Finite element Method in Engineering Science, McGraw- Hill, New York, 97. 7. M.Aritoshi, K.Okita, T.Enjo, K.Ikeuchi and F.Matsuda, Friction Welding of Oxygen Free Copper to Pure Aluminum, Q.J. Jpn. Welding Soc., Vol. 9, pp. 467-474, 99. 8. C.J.Dawes, Micro-Friction Welding Aluminum Studs to Mild Steel Plates, Metal Construction, Vol. 9, pp. 96-97, 977. 9. W.Lee, M.Schmuecker, U.A.Mercardo, G.Biallas and S.Jung, Interfacial Reaction in Steel- Aluminum Joints Made by Friction Stir Welding, Scripta Materialia, Vol. 55, pp. 355-358, 2006. 203

International Journal of Scientific & Engineering Research, Volume 4, Issue 0, October-203 963 TABLE : Mechanical properties of aluminum, steel, copper and titanium. Material Young s Modulus GPa Density Kg 3 m Aluminum 69 2780 Steel 204 7750 Copper 0 8940 Titanium 5 4429 TABLE 2: Summary of minimum mass designs of two stepped cantilever columns with single /two materials subjected to buckling load 203

International Journal of Scientific & Engineering Research, Volume 4, Issue 0, October-203 964 constraint of 453.5927 Kg (000lb). Parameter Present study Ref.[6] Ref.[7] Ref.[8] Ref.[9] Materials of stepped beam 4.925 4.48 4.577 5.829 4.979 Steel isotropic beam Minimum mass in kg. 3.970 -- -- 4.005 4.83 20.957 -- -- 2.088 2.457.025 -- --.07.768 Steel-aluminum compound beam copper-aluminum compound beam Titanium-aluminum compound beam Figure a.two Stepped Steel Column 203

International Journal of Scientific & Engineering Research, Volume 4, Issue 0, October-203 965 Figure b. Two Stepped Compound Column 203