Mechanical behavior and failure of sandwich structures

The failure behavior of composite sandwich beams under three- and four-point bending was studied. The beams were made of unidirectional carbon/epoxy facings and various core materials including PVC closed-cell foams, a polyurethane foam and an aluminum honeycomb. Various failure modes including fa...

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Дата:2013
Автор: Gdoutos, Е.
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Опубліковано: Інститут електрозварювання ім. Є.О. Патона НАН України 2013
Назва видання:Автоматическая сварка
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Цитувати:Mechanical behavior and failure of sandwich structures / Е. Gdoutos // Автоматическая сварка. — 2013. — № 10-11 (726). — С. 107-111. — Бібліогр.: 11 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
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spelling irk-123456789-1032362016-06-16T03:03:08Z Mechanical behavior and failure of sandwich structures Gdoutos, Е. Пленарные доклады Международной конференции The failure behavior of composite sandwich beams under three- and four-point bending was studied. The beams were made of unidirectional carbon/epoxy facings and various core materials including PVC closed-cell foams, a polyurethane foam and an aluminum honeycomb. Various failure modes including facing wrinkling, indentation failure and core failure were observed and compared with analytical predictions. It was established that the initiation, propagation and interaction of failure modes depend on the type of loading, constituent material properties and geometrical dimensions. 2013 Article Mechanical behavior and failure of sandwich structures / Е. Gdoutos // Автоматическая сварка. — 2013. — № 10-11 (726). — С. 107-111. — Бібліогр.: 11 назв. — англ. http://dspace.nbuv.gov.ua/handle/123456789/103236 620.192.7:62-112.81 en Автоматическая сварка Інститут електрозварювання ім. Є.О. Патона НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
topic Пленарные доклады Международной конференции
Пленарные доклады Международной конференции
spellingShingle Пленарные доклады Международной конференции
Пленарные доклады Международной конференции
Gdoutos, Е.
Mechanical behavior and failure of sandwich structures
Автоматическая сварка
description The failure behavior of composite sandwich beams under three- and four-point bending was studied. The beams were made of unidirectional carbon/epoxy facings and various core materials including PVC closed-cell foams, a polyurethane foam and an aluminum honeycomb. Various failure modes including facing wrinkling, indentation failure and core failure were observed and compared with analytical predictions. It was established that the initiation, propagation and interaction of failure modes depend on the type of loading, constituent material properties and geometrical dimensions.
format Article
author Gdoutos, Е.
author_facet Gdoutos, Е.
author_sort Gdoutos, Е.
title Mechanical behavior and failure of sandwich structures
title_short Mechanical behavior and failure of sandwich structures
title_full Mechanical behavior and failure of sandwich structures
title_fullStr Mechanical behavior and failure of sandwich structures
title_full_unstemmed Mechanical behavior and failure of sandwich structures
title_sort mechanical behavior and failure of sandwich structures
publisher Інститут електрозварювання ім. Є.О. Патона НАН України
publishDate 2013
topic_facet Пленарные доклады Международной конференции
url http://dspace.nbuv.gov.ua/handle/123456789/103236
citation_txt Mechanical behavior and failure of sandwich structures / Е. Gdoutos // Автоматическая сварка. — 2013. — № 10-11 (726). — С. 107-111. — Бібліогр.: 11 назв. — англ.
series Автоматическая сварка
work_keys_str_mv AT gdoutose mechanicalbehaviorandfailureofsandwichstructures
first_indexed 2025-07-07T13:30:09Z
last_indexed 2025-07-07T13:30:09Z
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fulltext 10710-11/2013 UDC 620.192.7:62-112.81 MECHANICAL BEHAVIOR AND fAILURE Of SANDWICH STRUCTURES E. GDOUTOS School of Engineering, Democritus University of Thrace, GR-671 00 Xanthi, Greece. E-mail: egdoutos@civil.duth.gr The failure behavior of composite sandwich beams under three- and four-point bending was studied. The beams were made of unidirectional carbon/epoxy facings and various core materials including PVC closed-cell foams, a polyure- thane foam and an aluminum honeycomb. Various failure modes including facing wrinkling, indentation failure and core failure were observed and compared with analytical predictions. It was established that the initiation, propagation and interaction of failure modes depend on the type of loading, constituent material properties and geometrical dimensions. 11 Ref., 2 Tabls, 4 figures. K e y w o r d s : investigation of failure behavior, three-point bending, sandwich beams, carbon-epoxy facing, various core materials, strength-to-weight ratio 1. Introduction Sandwich structures consisting of strong and stiff facings and light weight cores offer improved stiffness and strength to weight ratios compared to monolithic materials. Under flexural loading the facings carry al- most all of the bending, while the core takes the shear loading and helps to stabilize the facings. facing ma- terials include metals and fiber reinforced composites. The latter are being used in advanced applications due to the large strength-to-weight ratio. The core mate- rials mainly include honeycombs, foams and wood. Possible failure modes of sandwich structures in- clude tensile or compressive failure of the facings, debonding at the core/facing interface, indentation failure under concentrated loads, shear core failure, wrinkling of the compression face and global buck- ling. Recently, the authors have performed a thorough investigation of the failure behavior of sandwich beams with facings made of carbon/epoxy composite material and core made of foam materials [1-6]. In the present work, failure modes were investi- gated experimentally in sandwich beams under four- point and three-point bending. failure modes ob- served and studied include core failure, face sheet wrinkling and indentation failure. 2. Materials and Specimens The sandwich beams were fabricated from 8-ply unidirectional carbon/epoxy (AS4/3501-6) facings and various core materials. The facings were bonded to the core with an epoxy adhesive (Hysol EA 9430). The assembly was cured at room temperature. The facings and core had a thickness of 1 and 25.4 mm, respectively. Beam specimens 25.4 mm wide and of various lengths were cut from the sandwich plates. Tables 1 and 2 give some characteristic properties of the sandwich constituent materials. 3. Experimental Procedure Special test fixtures were fabricated to provide three- and four-point bending for beams of various lengths. five span lengths of 10.2, 20.3, 25.4, 40.6 Ta b l e 1 . Properties of balsa wood, aluminum and foam-filled honeycomb, and polyurethane materials Property Balsa Wood CK57 Aluminum Honeycomb PAMG 5052 foam filled Honeycomb Style 20 Polyurethane fR-3708 Density, r kg/m3 (lb/ft3) 150 (9.4) 130 (8.1) 128.3 (8) 128.3 (8) In-plane long. comp. elast. mod., E1c MPa (ksi) 129.5 (18.8) 9.5 (1.38) 24.1 (3.5) 38.5 (5.6) In-plane long. tens. elast. mod., E1t MPa (ksi) 93.6 (13.6) 4.5 (0.65) 1.3 (0.19) 416.6 (60.4) In-plane trans. comp. elast. mod., E2c MPa (ksi) 129.5 (18.7) 6 (0.87) 7.6 (1.1) 38.5 (5.6) Out of plane comp. elast. mod., E3c, MPa (ksi) 5394 (782.3) 2125 (308) 269.1 (39) 108.7 (15.8) Transverse shear elast. mod., G13, MPa (ksi) 58.7 (8.5) 579 (84) 8.5 (1.23) 10.3 (1.49) In-plane long. comp. strength, f1c MPa (ksi) 0.78 (0.11) 0.2 (0.03) 0.4 (0.06) 1.15 (0.17) In-plane long. tensile strength, f1t MPa (ksi) 1.13 (0.16) 1.63 (0.24) 0.48 (0.07) 1.1 (0.16) In-plane trans. comp. strength, f2c MPa (ksi) 0.78 (0.11) 0.17 (0.03) 0.32 (0.05) 1.15 (0.17) Out of plane comp. strength, f3c MPa (ksi) 9.6 (1.39) 11.8 (1.7) 1.35 (0.2) 1.74 (0.25) Transverse shear strength, f13 MPa (ksi) 3.75 (0.54) 3.45 (0.5) 0.75 (0.11) 1.4 (0.2) © E. Gdoutos, 2013 108 10-11/2013 and 76.2 cm were tested. In studying the effects of pure bending, special reinforcement was provided for the core at the outer sections of the beam to prevent premature core failures. Also, under three-point bend- ing, the faces directly under concentrated loads were reinforced with additional layers of carbon/epoxy to suppress and prevent indentation failure. Only in the case when the indentation failure mode was studied, there was no face reinforcement. The concentrated load was applied to the specimens with a cylinder of diameter of 25.4 mm (1 in.). Strains on the outer and inner (interface between facing and core) surfaces of the facings were record- ed with strain gages. Most gages were oriented along the axis of the beam, but some were mounted in the transverse direction to record transverse strains. Beam deflections were measured with a displacement trans- ducer (LVDT) and by monitoring the crosshead mo- tion. The deflection was also monitored with a course moiré grating (31 lines/cm). Longitudinal and trans- verse strains in the core were measured with finer moiré gratings of 118 and 200 lines/cm. The deforma- tion of the core was also monitored with birefringent coatings using reflection photoelasticity. 4. Failure Modes A number of failure modes were recorded and studied in the composite sandwich beams subjected to three- and four-point bending. They include wrin- kling of the compression facing, core failure and in- dentation of the loaded face. These failure modes are discussed in the following sections. 4.1. Compression Facing Wrinkling Compression facing wrinkling failures were ob- served in sandwich beams under both four-point and three-point bending. fig. 1 shows moment ver- sus strain results for two different tests of sandwich beams with Divinycell H100 cores under four-point bending. Evidence of wrinkling is shown by the sharp change in recorded strain on the compression facing, indicating inward and outward wrinkling in the two tests. In both cases the critical wrinkling stress was σcr = 673 MPa. Wrinkling is a localized short-wave buckling of the compression facing. Wrinkling may be viewed as buckling of the compression facing supported by an elastic continuum, the core. The critical wrinkling stress according to Heath [7] is given by ( )cr 12 3 1 12 21 2 3 1 f c fcE Eh h   s =   - ν ν   (1) where , cfh h : facing and core thicknesses, respec- tively; 31,f cE E : facing and core moduli, respective- ly; ijν : Poisson’s ratio associated with loading in the i-direction and strain in the j-directio and the indices 1 and 3 refer to the in-plane and through-the-thickness directions, respectively. Equation (1) predicts the following value of the wrinkling stress cr 687MPa.s = This value is close to the experimental value of 673 MPa. In the case when shear is present in addition to bending, the influence of the transverse shear mod- ulus of the core, 13cG , must be taken into account. An expression given by Hoff and Mautner [8] has the form ( )cr 1/3 3 131 c cfc E E Gs = (2) where c is a constant usually taken as equal to 0.5, 0.6, or 0.65. Note that the critical stress in this expression depends only on the elastic moduli of the facing and core materials. In the relation above the core mod- uli are the initial elastic moduli if wrinkling occurs figure 1. facing wrinkling in sandwich beam under four-point bending (Divinycell H100 foam core; dimensions are in cm) Ta b l e 2 . Properties of carbon/epoxy facings, adhesive, and H100 and H250 PVC foams Property facing fM-73 Adhesive foam Core (H100) foam Core (H250) Density, r, kg/m3 1,620 1,180 100 250 Thickness, h, mm 1.01 0.05 25.4 25.4 Longitudinal Modulus, E1, MPa 147,000 1,700 120 228 Transverse Modulus, E3, MPa 10,350 139 403 Transverse Shear Modulus, G13, MPa 7,600 110 48 117 Longitudinal Compressive Strength, f1c, MPa 1,930 1.7 4.5 Transverse Compressive Strength, f3c, MPa 240 1.9 6.3 Transverse Shear Strength, f13, MPa 71 33 1.6 5.0 10910-11/2013 while the core is still in the linear elastic range. This requires that the shear force at the time of wrinkling be low enough or, at least, c csV A F< (3) where Ac is core cross sectional area and fcs the shear strength of the core. This is the case for long span beams under three-point bending. 4.2. Core Failure Core failures were observed in sandwich beams under three-point bending. The core carries primar- ily the applied shear loading. In short beams under three-point bending the core is mainly subjected to shear and failure occurs when the maximum shear stress reaches the critical value (shear strength) of the core material. In long-span beams the normal stresses in the core become of the same order of magnitude or even higher than the shear stresses. In this case, the core is subjected to a biaxial state of stress and fails according to an appropriate failure criterion. It was shown that failure of the core materials can be described by the Tsai-Wu failure criterion [9]. for a beam loaded under combined bending and shear, the foam is subjected to longitudinal normal stress, s1, and in-plane shear stress, t5 (t13). The Tsai-Wu crite- rion for this case takes the form 2 2 1 1 11 1 1f f ks + s = - (4) where 5 1 11 55 2 1 1 1 1 5 5 1 1 1 1, , , t c t c f f f k F F F F F F t = - = = = f1t, f1c = tensile and compressive strengths in the in- plane (1, 2) direction. f5 = shear strength on the 1-3 plane. In the above equations σ1, σ3 and τ5 are the normal and shear stresses referred to the principal material directions (in-plane is direction 1 and through-the- thickness is direction 3), f1c and f1t are the com- pressive and tensile strengths along the in-plane di- rection, f3c and f3t are the compressive and tensile strengths along the through-the-thickness direction and f5 (= f13) is the shear strength on the 1-3 plane. The state of deformation and failure mechanisms in the core were studied by means of moiré method. fig. 2 shows moiré fringe patterns in the core of a sandwich beam with Divinycell H250 core under three-point bending. The moiré fringe patterns corre- sponding to the horizontal and vertical displacements away from the applied load consist of nearly parallel and equidistant fringes from which it follows that the normal strains are zero, while the shear strain is nearly constant across the core thickness. This is valid only in the linear range. 4.3. Indentation Failure Indentation failure was observed in beams under three-point bending when no special reinforcement of the facing or the core was provided in the area un- der the load. fig. 3 shows the variation of the applied load with the displacement of the indenting roller for a 36 cm long beam under three-point bending. The displacement represents the sum of the global beam deflection and the local indentation, but it is more sen- sitive to the local indentation. Therefore, the propor- tional limit of the load-displacement curve is a good indication of initiation of indentation. In the present case the beam was made with a Divinycell H100 core. The load at initiation of indentation is 735 N. The peak load measured was Pmax = 1080 N. The indentation failure of the sandwich beam can be predicted by treating the loaded face as a beam resting on a foundation. for linear elastic behavior, the core is modeled as continuous distributed linear tension/compression springs. The stress s at the in- terface between core and facing is proportional to the figure 2. Moire fringe patterns corresponding to horizontal and vertical displacements in sandwich beam under three-point bending (12 lines/ mm; Divinycell H250 core) figure 3. Load versus deflection under load of sandwich beam under three-point bending (carbon/epoxy facings, Divinycell H100 core) 110 10-11/2013 local deflection, w kws = (5) where k is the foundation modulus given by [10] 3 1 3 30.64 .c c f f E E k h E = (6) for a long (assumed infinite) facing the deflection Pw under the load P is [10] 2P Pw kb λ = (7) where 1 3 1.18 c f f E h E λ = (8) and b is the width of the facing. Yield of the core under the load occurs when the interfacial stress s reaches the yield stress of the foam core. The critical load at initiation of core yield is cal- culated from Eqs. (5) to (8) and the yield condition as 1 31.70 f cy ys f c E P bh E = s (9) where yss is the yield stress of the core. As the load increases beyond the yield value, plas- tic deformation propagates through the core from the center to the ends of the facing. for a rigid-perfectly plastic foundation the local bending stress at the upper surface of the facing is given by [11] 2 2 2 9 . 16fl f ys P b h s = s (10) for a beam in three-point bending the global stress in the facing is ( )4fb f f c PL bh h h s = + (11) where ch is the thickness of the facing. Indentation failure occurs when the sum of the lo- cal and global bending stresses, andfl fbs s , reaches the compressive strength of the facing material. The load at initiation of indentation in fig. 3 is 735 N and agrees with the calculated value of 800 N from Eq. (9). The peak load measured is max 1080,P = while the calculated value is max 1310 .P N= The difference in the results may be attributed in the simplifying as- sumption of a rigid-perfectly plastic foundation. 5. Failure Mode Transition from the above discussion it is obvious that in- itiation of a particular failure mode depends on the geometrical characteristics, the material properties and the loading conditions of the beam. In the case of beams under three-point bending when reinforce- ment of the facings or the core is provided to sup- press indentation failure, the prevalent failure modes are facing wrinkling and core failure. for short spans, core failure occurs first and then it triggers facing wrinkling. for long spans, facing wrinkling can occur before any core failure. Thus, a curve for the critical load for core failure initiation versus span length is obtained. On the other hand, the critical load for fac- ing wrinkling as a function of span length can be pre- dicted from Eq. (2). fig. 4 shows curves of the critical load versus span length for initiation of failure by core failure and facing wrinkling for a sandwich beam with various core materials. The intersection of the curves defines the transition from core failure initiation to facing wrinkling initia- tion. Note that for core materials H250, balsa wood and aluminum honeycomb with increased through- the-thickness Young’s modulus the compressive fac- ing wrinkling failure curve is displaced, according to Eq. (2) to the right, and therefore, the critical length for failure mode transition from core failure to wrin- kling increases. Thus, as the through-the-thickness Young’s modulus of the foam increases, the critical length of the beam for failure mode transition from core failure to wrinkling, also increases. 6. Conclusions failure modes of composite sandwich beams de- pend on the type of loading, constituent material properties and geometrical dimensions. for sandwich beams made of unidirectional carbon/epoxy facings and PVC closed-cell foam cores failure modes ob- served and studied include core failure, compressive facing wrinkling and indentation failure. Experimen- tal results were compared with theoretical predictions whenever they were available. following initiation, interaction of failure modes takes place leading to catastrophic fracture. Thus, failure initiation by plastic deformation of the core degrades the supporting role of the core and precip- itates other failure modes, such as facing wrinkling. When core failure and stiffness degradation occur first, the critical wrinkling stress is substantially re- duced. Thus, catastrophic failure of a sandwich beam appears to be the result of initiation propagation and interaction of failure modes, as influenced by type of loading, constituent material properties and geometri- cal dimensions. figure 4. Critical load versus span length for failure initiation in sand- wich beams under three-point bending. Horizontal lines indicate core shear failure and curved lines indicate failure by compressive facing wrinkling 11110-11/2013 1. Daniel, I. M., Gdoutos, E. E., Wang, K.-A. et al. (2002) fail- ure modes of composite sandwich beams. Int. J. Damage Mech, 11, 309–334. 2. Gdoutos, E. E., Daniel, I. M., Wang, K.-A. (2002) Indenta- tion failure in composite sandwich structures. Exp Mech, 42, 426–431. 3. Daniel, I. M., Gdoutos, E. E., Wang, K.-A. (2002) failure of composite sandwich beams. Adv. Com. Letters, 11, 49–57. 4. Abot, J. L., Daniel, I. M., Gdoutos, E. E. (2002) Contact law for composite sandwich beams. Sandwich Struct. & Mater. 4, 157–173. 5. Gdoutos, E. E., Daniel, I. M., Wang, K.-A. (2003) Com- pression facing wrinkling of composite sandwich structures. Mech. Mater., 35, 511–522. 6. Gdoutos, E. E., Daniel, I. M., Wang, K.-A. (2000) failure of cellular foams under multiaxial loading. Comps. Part A, 33, 163–176. 7. Heath, W. G. (1969) Sandwich construction. Pt 2: The op- timum design of flat sandwich panels. Aircraft Engng, 32, 230–235. 8. Hoff, N. J., Mautner, S. E. (1945) The buckling of sand- wich-type panels. J. Aerosp. Sci., 12, 285–297. 9. Tsai, S. W., Wu, E. M. (1971) A general theory of strength for anisotropic materials. J. Comp. Mat., 5, 58–80. 10. Hetenyi, M. (1946) Beams on Elastic Foundation. The Uni- versity of Michigan Press. 11. Soden, P. D. (1996) Indentation of composite sandwich beams. J. Strain Anal., 31, 353–360. Received 08.04.2013