BUCKLING COEFFICIENTS FOR SIMPLY SUPPORTED, FLAT, RECTANGULAR SANDWICH PANELS UNDER BIAXIAL COMPRESSION

Similar documents
MINIMUM WEIGHT STRUCTURAL SANDWICH

COMPRESSIVE EUCICLING CURVES MR SANDWICH PANELS WITH ISOTROPIC FACINGS AND ISOTROPIC OR ORTI1OTROIPIC CORES. No Revised January 1958

ri [11111 IlL DIRECTIONAL PROPERTIES Of GLASS-FABRIC-BASE PLASTIC LAMINATE PANELS Of SIZES THAT DO NOT IBUCICLE (P-Q1lAtVjr) No.

BUCKLING COEFFICIENTS FOR SANDWICH CYLINDERS OF FINITE LENGTH UNDER UNIFORM EXTERNAL LATERAL PRESSURE

STRESSES WITHIN CURVED LAMINATED BEAMS OF DOUGLAS-FIR

Laminated Beams of Isotropic or Orthotropic Materials Subjected to Temperature Change

THE BENDING STIFFNESSES OF CORRUGATED BOARD

EFFECT OF ELLIPTIC OR CIRCULAR HOLES ON THE STRESS DISTRIBUTION IN PLATES

FLEXURE OF STRUCTURAL SANDWICH CONSTRUCTION

WRINI CLING Of THE FACINGS OF SANDWICH CONSTRUCTION %EJECTED TO EDGEWISE COMPRESSION Sandwich Constructions Having Honeycomb Cores

CHAPTER THREE SYMMETRIC BENDING OF CIRCLE PLATES

Machine Direction Strength Theory of Corrugated Fiberboard

ELASTIC STAIBILITY CIF TUE FACINGS Of HAT SANDWICI-1 PANELS WIASI SUBJECTED TO COMBINED EDGEWISE STRESSES

EDGEWISE COMPRESSIVE STREW -Ill Of PANELS AND FIATWISE FLEXURAL STREW -Hi Of STRIPS Of SANDWICH CONSTRUCTIONS

Size Effects In the Crushing of Honeycomb Structures

Exercise: concepts from chapter 8

TABLE OF CONTENTS. Mechanics of Composite Materials, Second Edition Autar K Kaw University of South Florida, Tampa, USA

Samantha Ramirez, MSE. Stress. The intensity of the internal force acting on a specific plane (area) passing through a point. F 2

Nomenclature. Length of the panel between the supports. Width of the panel between the supports/ width of the beam

Tvestigated using the quadratic form of the Tsai-Wu strength theory [I].

REVIEW OF BUCKLING MODE AND GEOMETRY EFFECTS ON POSTBUCKLING STRENGTH OF CORRUGATED CONTAINERS

Mechanics of Composite Materials, Second Edition Autar K Kaw University of South Florida, Tampa, USA

A Suggested Analytical Solution for Vibration of Honeycombs Sandwich Combined Plate Structure

Enhancing Prediction Accuracy In Sift Theory

Module III - Macro-mechanics of Lamina. Lecture 23. Macro-Mechanics of Lamina

Mechanical Behavior of Composite Tapered Lamina

STRESSED-SKIN PANEL DEFLECTIONS AND STRESSES USDA FOREST SERVICE RESEARCH PAPER

CORRELATING OFF-AXIS TENSION TESTS TO SHEAR MODULUS OF WOOD-BASED PANELS

Tensile stress strain curves for different materials. Shows in figure below

RELATIONSHIP BETWEEN RADIAL COMPRESSIVE MODULUS OF ELASTICITY AND SHEAR MODULUS OF WOOD Jen Y. Liu Research Engineer

INTRODUCTION TO STRAIN

MECHANICS OF MATERIALS

CORRELATING OFF-AXIS TENSION TESTS TO SHEAR MODULUS OF WOOD-BASED PANELS

THE INFLUENCE OF THERMAL ACTIONS AND COMPLEX SUPPORT CONDITIONS ON THE MECHANICAL STATE OF SANDWICH STRUCTURE

Experiment Five (5) Principal of Stress and Strain

Optimum Fiber Distribution in Singlewall Corrugated Fiberboard

Presented By: EAS 6939 Aerospace Structural Composites

August 3,1999. Stiffness and Strength Properties for Basic Sandwich Material Core Types UCRL-JC B. Kim, R.M. Christensen.

Homework No. 1 MAE/CE 459/559 John A. Gilbert, Ph.D. Fall 2004

Bending of Simply Supported Isotropic and Composite Laminate Plates

ME 582 Advanced Materials Science. Chapter 2 Macromechanical Analysis of a Lamina (Part 2)

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

Improved Design Formulae for Buckling of Orthotropic Plates under Combined Loading

Stress, Strain Stress strain relationships for different types of materials Stress strain relationships for a unidirectional/bidirectional lamina

MECHANICS OF MATERIALS

Chapter 3. Load and Stress Analysis

Jeff Brown Hope College, Department of Engineering, 27 Graves Pl., Holland, Michigan, USA UNESCO EOLSS

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 2 Stress & Strain - Axial Loading

Structural Dynamics Lecture Eleven: Dynamic Response of MDOF Systems: (Chapter 11) By: H. Ahmadian

STRENGTH AND STIFFNESS REDUCTION OF LARGE NOTCHED BEAMS

Lecture 8. Stress Strain in Multi-dimension

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

EFFECTIVE THICKNESS OF PAPER: APPRAISAL AND FURTHER DEVELOPMENT

Chapter 2 - Macromechanical Analysis of a Lamina. Exercise Set. 2.1 The number of independent elastic constants in three dimensions are: 2.

five Mechanics of Materials 1 ARCHITECTURAL STRUCTURES: FORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS SUMMER 2017 lecture

Buckling Behavior of 3D Randomly Oriented CNT Reinforced Nanocomposite Plate

SANDWICH COMPOSITE BEAMS for STRUCTURAL APPLICATIONS

DEFLECTION OF BEAMS WlTH SPECIAL REFERENCE TO SHEAR DEFORMATIONS

LATERAL STABILITY OF DEEP BEAMS WITH SHEAR-BEAM SUPPORT

THEORETICAL DESIGN OF A NAILED OR BOLTED JOINT UNDER LATERAL LOAD 1. Summary

BIAXIAL STRENGTH INVESTIGATION OF CFRP COMPOSITE LAMINATES BY USING CRUCIFORM SPECIMENS

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

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

Basic Energy Principles in Stiffness Analysis

Chapter 2: Elasticity

PURE BENDING. If a simply supported beam carries two point loads of 10 kn as shown in the following figure, pure bending occurs at segment BC.

Chapter 3. Load and Stress Analysis. Lecture Slides

Lecture 15 Strain and stress in beams

STRAIN. Normal Strain: The elongation or contractions of a line segment per unit length is referred to as normal strain denoted by Greek symbol.

INELASTIC BUCKLING ANALYSIS OF AXIALLY COMPRESSED THIN CCCC PLATES USING TAYLOR-MACLAURIN DISPLACEMENT FUNCTION

MECHANICS OF COMPOSITE STRUCTURES

MATERIAL ELASTIC ANISOTROPIC command

International Journal of Advanced Engineering Technology E-ISSN

MECHANICS OF MATERIALS

Problem " Â F y = 0. ) R A + 2R B + R C = 200 kn ) 2R A + 2R B = 200 kn [using symmetry R A = R C ] ) R A + R B = 100 kn

SIZE EFFECTS IN THE COMPRESSIVE CRUSHING OF HONEYCOMBS

Bilinear Modelling of Cellulosic Orthotropic Nonlinear Materials

NONLINEAR ELASTIC CONSTITUTIVE RELATIONS FOR CELLULOSIC MATERIALS

DEPARTMENT OF MECHANICAL ENIGINEERING, UNIVERSITY OF ENGINEERING & TECHNOLOGY LAHORE (KSK CAMPUS).

2. (a) Explain different types of wing structures. (b) Explain the advantages and disadvantages of different materials used for aircraft

Mechanics of Materials Primer

Getting Started with Composites Modeling and Analysis

Laminated Composite Plates and Shells

ANALYTICAL SOLUTIONS USING HIGH ORDER COMPOSITE LAMINATE THEORY FOR HONEYCOMB SANDWICH PLATES WITH VISCOELASTIC FREQUENCY DEPENDENT DAMPING

Sample Question Paper

(laod No \' V,R A " FI- 1 4, <4. ELASTIC STABILITY Of CYLINDRICAL SANDWICH SHELLS UNDER AXIAL AND LATERAL LOAD. July 1955

ELASTICITY (MDM 10203)

BEAMS AND PLATES ANALYSIS

TORSION OF SANDWICH PANELS OF TRAPEZOIDAL, TPIANGUIAP, AND RECTANGULAR CROSS SECTIONS

ELASTICITY AND FRACTURE MECHANICS. Vijay G. Ukadgaonker

December 1991 Technical Paper. An analysis and design method is presented for the design of composite sandwich cover panels that includes

Lab Exercise #5: Tension and Bending with Strain Gages

BUCKLING OF SKEW PLATES WITH CONTINUITY OR ROTATIONAL EDGE RESTRAINT

Finite element modelling of infinitely wide Angle-ply FRP. laminates

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

International Journal of Innovative Research in Science, Engineering and Technology Vol. 2, Issue 7, July 2013

[5] Stress and Strain

PLASTIC FLOW THROUGHOUT VOLUME OF THIN ADHESIVE!BONDS. No March 1958 (.2. Will In' iriculture ROOM. Mum mina

Simulation of Mechanical and Thermal Properties for Sandwich Panels with Cellular Wood Cores

Mechanical Behavior of Circular Composite Springs with Extended Flat Contact Surfaces

Transcription:

U. S. FOREST SERVICE RESEARCH PAPER FPL 135 APRIL 1970 BUCKLING COEFFICIENTS FOR SIMPLY SUPPORTED, FLAT, RECTANGULAR SANDWICH PANELS UNDER BIAXIAL COMPRESSION FOREST PRODUCTS LABORATORY, FOREST SERVICE U.S. DEPARTMENT OF AGRICULTURE, MADISON, WIS. This Report is One of a Series Issued in Cooperation with the MIL-HDBK-23 WORKING GROUP ON COMPOSITE CONSTRUCTION FOR AEROSPACE VEHICLES of the Departments of the AIR FORCE, NAVY, AND COMMERCE

ABSTRACT Presents the derivation of formulas for the buckling coefficients of simply supported, flat, rectangular sandwich panels under edgewise (in-plane) biaxial compression loads. Values of the coefficients are presented in graphs for sandwich with isotropic and orthotropic facings on isotropic and orthotropic (honeycomb) cores.

BUCKLING COEFFICIENTS FOR SIMPLY SUPPORTED, FLAT, RECTANGULAR SANDWICH PANELS UNDER BIAXIAL COMPRESSION. By EDWARD W. KUENZI, Engineer 2 Forest Products Laboratory 3 Forest Service U.S. Department of AgricuIture INTRODUCTION Structural sandwich components comprising thin, stiff facings bonded to both surfaces of a thick, lightweight core can provide highly efficient constructions for carrying various loads. It is essential that such sandwich carry in-plane or edgewise loads without buckling and that criteria for buckling account for the effects of low transverse shear rigidity of the sandwich core. Previous work for buckling of sandwich panels under uniaxial compression utilized an approximate energy method 4,5 which is exact for panels with simply supported edges. The derivation here will also use an energy method to obtain a solution for the buckling coefficients of panels under biaxial compression. 1 This paper is issued in cooperation with the MIL-HDBK-23 Working Group on Structural Sandwich Composites under Air Force DO F33615-70-M-5000. 2 The author wishes to acknowledge the work of Gordon H. Stevens in checking the mathematical manipulations and Fred Rattner in computing values of the buckling coefficients. 3 Maintained at Madison, Wis., in cooperation with the University of Wisconsin. 4 Ericksen, Wilhelm S. and March, H. W. Compressive Buckling of Sandwich Panels Havings Dissimilar Facings of Unequal Thickness. U.S. Forest Products Lab. Rep. 1583-B, Rev. 5 Kuenzi, Edward W., Norris, Charles B., and Jenkinson, Paul M. Buckling Coefficients for Simply Supported and Clamped Flat, Rectangular Sandwich Panels under Edgewise Compression. U.S. Forest Service Res. Note FPL-070. Dec. 1964. Forest Products Lab., Madison,

NOTATION a,b - Length of panel edge (see fig. 1) c - Subscript denoting core D - Bending stiffness or twisting stiffness, depending on subscripts (For sandwich with thin, equal facings E - Young s modulus of elasticity of facing G - Modulus of rigidity; for facings, G is associated with shear distortion xy in the plane of the facing; for cores, G and G are associated cxz cyz with shear distortion in the xz and yz planes, respectively. H - Energy expressions h - Distance between facing centroids K - Buckling coefficient m - Number of half waves in direction of x axis 0 - Subscript denoting initial N - Load per unit length of edge (see fig. 1) n - Number of half waves in direction of y axis R - Ratio shear moduli; R = G /G cxz cyz S - Shear load normal to surface of panel, per unit length of edge t - Facing thickness u - Transverse shear stiffness, V- Parameter relating shear and bending stiffness W- Special parameter relating shear and bending stiffness for sandwich with corrugated core w- Deflection normal to sandwich panel x- Axis: subscript denoting parallel to x axis (see fig. 1) y- Axis; subscript denoting parallel to y axis (see fig. 1) z- Axis; subscript denoting parallel to z axis (see fig. 1) µ- Facing Poisson s ratio; with subscripts µ is the ratio of contraction xy in the y direction to extension in the x direction due to a tensile stress in the x direction Figure 1. Notation M 137 511 FPL 135 2

DERIVATION OF BUCKLING LOAD FORMULA The buckling load formula is derived by equating the strain energy due to shear and bending of the panel to the potential energy of the external loads after assumption of a suitable deflected surface of the panel. The resultant expression is minimized with respect to parameters defining core shear distortion to eventually obtain buckling coefficients. The strain energy due to shear and bending of the panel is given by Libove and Batdorf 6 as: (1) and substitution of these into (1)results in (2) 6 Libove, Charles and Batdorf, S. B. A General Small-Deflection Theory for Flat Sandwich Plates. NACA Tech. Note 1526. April 3

For a very rigid core U and g and expression (2) reduces to the usual one for plates. 6 The potential energy of the external loads is given by Libove and Batdorf (3) The deflection of a sandwich panel with simply supported edges is assumed to be (4) After (4) into (1) and (2) and equating (1) and (2) the following expression is obtained after some manipulation: where the buckling coefficient K is given by FPL 135 4

Formula (6) is then minimized with respect to g x and g y by equating partial derivatives to zero and solving the two resultant equations simultaneously for g x and g y. The resultant formulas for g x and g y are given by where (9) The critical buckling value of N x (N xcr ) is then obtained from (5) after substitution of (6), (7), and (8) and minimizing for integral values of the half waves m and n for various values of the ratios N y /N x, a/b, property values, and V. COMPUTATION OF BUCKLING COEFFICIENTS Buckling coefficients, K, were computed for sandwich with isotropic and orthotropic facings having cores of isotropic, orthotropic, or of corrugated material, For isotropic facings it was assumed that D x /D y = 1, µ xy = 0.25, and D xy /(D x D y ) 1/2 =0.375. For orthotropic facings it was assumed that D x /D y = 1, µ xy = 0.2, and D xy /(D x D y )1/2 = 0.21. 7 7 These ratios correspond to many types of glass-fabric laminate facings summarized in table 1 of Forest Products Lab. Report 1867, "Compressive Buckling Curves for Simply Supported Sandwich Panels with Glass-Fabric-Laminate Facings and Honeycomb Cores," by B. Norris, 1958. 5

For cores it was assumed that R = 1 for isotropic core and R = 0.4 or 2.5 for 8 orthotropic honeycomb cores with hexagonal cells. Computations for sandwich with corrugated cores were carried out for R = 0.01 or 100 thus simulating the usual assumption for this core that it is infinitely stiff in shear parallel to corrugation flutes but has a finite shear stiffness perpendicular to the flutes. For flutes parallel to the X axis the core shear parameter V is replaced by (10) Curves of buckling coefficients for sandwich with isotropic facings and isotropic and orthotropic cores are given in figures 2, 3, 4, and 5. Coefficients for sandwich with orthotropic facings and isotropic and orthotropic cores are given in figures 6, 8, and 9. Coefficients for sandwich with corrugated cores and isotropic and orthotropic facings are given in figures 10, 11, 12, and 13. These curves show the buckling coefficient K as ordinate for various panel aspect ratios (a/b) as abscissa. The abscissa scale is inverted at (a/b = 1) so that the curves can be extended to the infinitely long panel (a/b or b/a = 0). Computation of the buckling coefficients showed that minimum values were always obtained for n = 1 and for m = 1, 2, 3 for small values of N /N. For v x larger values of N y /N x the value of m = 1 produced minimum buckling coefficients. The curves for which m = 1, 2, 3 produced minimums had the familiar cusped appearance indicated in the top dotted lines on figure 2. These cusps are omitted on the other. curves and the envelope or asymptotes are shown for use in design. APPROXIMATE VALUES For square isotropic sandwich panels the buckling coefficient can be computed by the following approximate formula: (11) 8 These ratios were experimentally determined for aluminum honeycomb core in Forest Products Lab. Report 1849, "Mechanical Properties of Aluminum Honeycomb Cores," by E. W. Kuenzi. FPL 135 6

Figure 2.. Buckling coefficients for simply supported sandwich panels in biaxial compression. V = 0, W = 0 M 137 509

Figure 3. Buckling coefficients for simply supported sandwich panels in biaxial compression. V = 0.1 M 137 501

Figure 4. Buckling coefficients for simply supported sandwich panels in biaxial compression. V a 0.2 137 506

Figure 5. Buckling coefficients for simply supported sandwich panels in biaxial compression. V = 0.4 M 137 508

Figure 6. Buckling coefficients for simply supported sandwich panels in biaxial compression. V = 0, W = 0 M 137 507

Figure 7. Buckling coefficients for simply supported sandwich panels in biaxial compression. V = 0.1 M 137 510

Figure 8. Buckling coefficients for simply supported sandwich panels in biaxial compression. V = 0.2 M 137 504

Figure 9. Buckling coefficients for simply supported sandwich panels in biaxial compression. V = 0.4 M 137 502

Figure 10. Buckling coefficients for simply suipported sandwich panels in biaxial compression. M 137 499

Figure 11. Buckling coefficients for simply supported sandwich panels in biaxial compression. M 137 500

Figure 12. Buckling coefficients for simply supported sandwich panels in biaxial compression. M 137 503

Figure 13, Buckling coefficients for simply supported sandwich panels in biaxial compression. M 137 505