Abstract
This study examines the improvement of Interlaminar Fracture Toughness (IFT) of multilayered 3D glass/epoxy textile composites when through thickness reinforcement is introduced. Three stitching techniques have been examined: Modified Lockstitch (ISO-301), Single-yarn Orthogonal-stitch (ISO-205) and Double-yarn Orthogonal-stitch (ISO-205). It was found that the use of class ISO-205 manual-type stitched reinforcement significantly enhanced the Mode I-IFT, GIC measured using a Double Cantilever Beam technique. Furthermore, in every case, the use of class ISO-205 stitching and high stitch densities offer a significant improvement of 74.5 % on Mode I-IFT against interlaminar delamination.
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1 Introduction
Fibre reinforced textile composite materials generally comprise a number of layers of 2D textile fabrics. Because of their weak through thickness mechanical properties, they suffer significant interlaminar delamination when exposed to out of plane loading [1, 2]. As part of the research into the in-plane mechanical properties of multilayered textile composites, numerous studies have been carried out by researchers in recent years [3, 4].
To provide through thickness reinforcement, braiding, knitting, 3D weaving, and stitching have been used to improve the interlaminar crack (delamination) resistance of multilayered composites. Among these reinforcement techniques, researchers have concluded that stitching is an effective reinforcement technique to limit crack propagation and to minimise delamination within multilayered textile composites [3–10]. The awareness of stitching as a technique for through thickness reinforcement has increased rapidly during the last three decades.
In this study, class ISO-205, a Single-yarn Orthogonal-stitch (SOS) and a Double-yarn Orthogonal-stitch (DOS) technique have been used to obtain through thickness reinforcement and these differ from the stitching techniques that have been previously utilised for this task; Modified Lockstitch (ISO-301), Lockstitch(ISO-301) and Chain Stitch (ISO-101) as reported by Morales in 1990 [11]. These commonly-used reinforcement stitching techniques are shown in Fig. 1, and were subsequently re-examined by Dransfield [3].
Both the lockstitch and the modified lockstitch require two constituent threads. The needle thread is inserted through the top of the fabric via the sewing needle, even as the under-thread is supplied from beneath the fabric via a bobbin. The two stitch yarns are first interlaced and then pulled into position in the middle of the fabric layers in the through thickness direction throughout the configuration of the balanced lockstitch. This formation damages the fabric fibres around the stitch loop and may trigger a high stress concentration point [11]. To avoid this problem the lockstitch is generally modified when used for textile composite preforms by diminishing the tension of the bobbin yarn (by loosening the bobbin-case spring), and also by increasing of the needle yarn, by increasing the pressure applied on the needle thread by the tension-disc adjuster. This readjustment of the stitch balance brings the interlace point to the top surface of the preform [11, 13]. Thus, the geometry of the lockstitch may be modified to ease the stress concentration and to address the problem stated above; this stitch form is almost universally used in composite applications. This stitching technique usefully halves the number of small-radius loops in the sewing thread from two per stitch to just one.
In contrast to these two stitch forms, the ISO-101 chain stitch is intralooped and only involves one yarn to complete the stitch formation process. It is very similar in structure to the weft knitting process, as it uses one single stitch yarn constantly making loops around itself [11]. Nevertheless, because small radius loops of 360° are required in the formation of every stitch and these are held during stitching by an under-bed looper, the flexibility demanded of the stitching yarn for this stitch geometry makes it inconvenient for advanced fibre yarns such as carbon, Kevlar and glass [3].
The alternative SOS and DOS techniques which have been used in this study are structurally simpler than the traditionally-used lockstitching techniques and moreover the theoretical stitch formation does not require any angles to be made in the yarn of greater than 90°. In practice, because of the flexibility and compressibility of the fabric layers being sewn, the bending of the stitching yarn is further minimised in radius. The orthogonal seam can therefore be created using high-performance (stiff) fibre yarns. Further critical characteristics of the SOS and DOS techniques are that an equal distance is left between successive needle penetration points and the stitching yarn is laid on both sides of the fabric preform; therefore the fabric is stabilised with even tensions applied above and below.
1.1 The Effects of Stitching on the Mechanical Properties of Multilayered Composites
The stitching technique as a through thickness reinforcement for multilayered textile composite structures has been mainly used by researchers in their experimental studies [8–10, 14, 15]. To stitch the laminates, especially high strength yarns frequently made of carbon, Kevlar, and glass have been used. Many studies have shown that stitching is the most effective through thickness reinforcement technique for composite preforms, even if many studies differ from each other with reference to fabric structure, fibre orientation, resin type, stitch density, direction of stitching, stitching yarn, stitch tension, and stitch patterns utilised. To limit interlaminar delamination and to achieve high delamination resistance many experimental studies on multilayered textile composite materials using the Double Cantilever Beam technique (DCB) test method have been carried out. These studies show that stitching the laminates results in a conspicuous enhancement of the Mode I-IFT, GIC in comparison with unstitched composite laminates [1, 3–10, 13, 16]. The researchers have stated that the introduction of through thickness stitching has increased the Mode II-IFT performance of multilayered textile composites and likewise the Mode I-IFT is also enhanced [1, 17–20].
Most studies confirm that stitching the laminates had not altered the impact damage resistance even though through thickness stitching has been shown to improve impact damage resistance [21]. Liu’s findings [22] show that stitching enhances the interlaminar strength and diminishes the damage area. The delamination resistance was inspected with respect to the effectiveness of various stitch patterns and across a variety of stitch densities. Liu pointed out [22] that stitching impedes the propagation of delamination and reduces the delamination area in accordance with the increase of stitch density.
Sharma and Shankar [19] concluded that stitching of laminates did not have a significant effect on the impact damage resistance, but decreased the damage area and increased the compression strength after impact, whilst Kang and Lee [23] found that the impact resistance properties had been improved by stitching the textile composite laminates.
Some studies show that stitching enhances or has no effect on flexural strength [1]. According to Kang and Lee [23], the tensile and flexural properties of woven laminate composites were improved by stitching. However, Mouritz [14] found that the stitching of glass reinforced polymer (GRP) laminates lessened the flexural properties. Moreover, it was found that these reductions were caused by the damage introduced by the stitching process, creation of resin-rich areas at the stitch holes, breakage of glass fibres, and also stitch interlacements. Even though stitching increased the elastic modulus, it did not affect the flexural and yield strengths [14].
In this study, the MLS, SOS and DOS stitching techniques have been used for the through thickness reinforcement of glass fibre fabric preforms. In total, five different stitch densities have been applied to multilayered preforms using these three stitching techniques. Hence, the effect of different stitching techniques and different stitch densities have been examined for stitched glass/epoxy composite specimens and compared to unstitched (UNS) composite specimens.
2 Experimental
2.1 Materials and Preparation of Preform Panels
In this study, it was chosen to use 8 layers of 2×2 twill weave structure made from E-glass fabric supplied by Sigmatex Ltd UK [24], having an a real weight of 876 g/m2 and with 2.54 g/cm3 E-glass fibre density [25] and this was integrated into a single preform panel to provide a test specimen thickness between 3 and 5 mm, in accordance with the ASTM D5528–01 standard test method [26]. All fabric layers were laid in the warp direction with dimensions of 390 mm (width) x 320 mm (length). The stitching process was performed (and will be explained in detail in the following section) after layering the eight plies of fabric. Following the completion of the stitching process, 12 extra layers of unidirectional (UD) E-glass fabric supplied by Formax with 498 g/m2 +/− 5 % fabric density and 2.54 g/cm3 E-glass fibre density [25] was used to obtain an increment for the final thickness of the test specimens. Even though international standards were followed wherever appropriate, this modification was made because, during initial testing of the trial set of composite specimens, the test malfunctioned; part of the test specimens fractured before the delamination part of the process had been completed. It was realised that the standard (ASTM) thickness of the trial set of test specimens was inadequate for the delamination process to be completed. It was found that for all the DCB test specimens, either the top or bottom arm bent severely without the first stitch being broken. Additionally, many of the loading hinges became detached as shown in Fig. 2, although this problem did not effect the entire range of composite test specimens used in this work.
Supplementary UD E-glass fabric plies were added to both sides of the pre-prepared preform panels; 6 plies of UD were added on top and six plies beneath. Therefore, the thickness of the test specimens was almost doubled (with a commensurate increase in stiffness) in order to gain a final thickness of the test specimens which allowed the test to be accomplished correctly [26]. The preform panel fabric specifications are given in Table 1.
2.2 Through Thickness Reinforcement - the Stitching Process
Following the preparation of preform panels, the Mode I-DCB test specimens were marked with the dimensions as required by the DCB testing standard in 25 mm (width) x 125 mm (length) on the preform panels. While marking the test specimens, 62 mm was retained as the working length for the stitching area and 63 mm of the specimens were separated by inserting Teflon film to separate the initial delamination length (a 0 ) of the test samples. To reinforce the preform panels the through thickness stitching method was introduced in the z-direction. Five different stitch densities were created by using a number of different stitch lengths: 20, 10, and 5 mm, inserted vertically in a single column through the length of the specimen; the yarns are specified in Table 2. Stitch patterns of: 10 × 10 and 5 × 5 mm were also inserted vertically and horizontally in two columns as shown in Table 4. The different stitch types being compared in the experimental work were inserted into the preform panel at the marked needle insertion points, so that the three stitching techniques could be compared in an unbiased fashion. The first stitching technique to be inserted was the commonly used MLS, the second technique was SOS, and the third was DOS.
2.2.1 Modified Lockstitch (MLS)
The commonly-used MLS (ISO-301) stitch technique was applied to the preform panels in the through thickness direction, as the first stitching procedure to be performed on an ADLER: KL267 type sewing machine. This sewing machine is designed to create a standard lockstitch seam using heavy gauge thread and is particularly well-suited to use in the automotive and upholstery industrial sectors [12]; the needle thread tension was increased and the bobbin thread tension decreased so that it would generate a modified lock-stitch. For the needle yarn, nylon 6.6 of 0.5 mm diameter was used as a top thread which was implemented to lock the stitches on the surface of the laminate. For the bobbin yarn, 0.6 mm diameter E-glass was used as the bottom thread which was implemented for through thickness reinforcement inside the laminates as is shown in the sketch in Fig. 3 which illustrates the cross section of the MLS stitch geometry.
2.2.2 Single-yarn Orthogonal-stitch (SOS)
The “Single-yarn Orthogonal-stitch” (ISO-205) is an alternative stitch geometry which has been named the SOS technique. It was applied to the preform panels as through thickness reinforcement by hand [12] at this stage. The SOS technique was applied with precisely defined stitch lengths using single 0.6 mm diameter E-glass yarn with identical stitch spacing to that of the MLS technique as illustrated in Fig. 4 which shows the cross section of the SOS stitch geometry.
2.2.3 Double-yarn Orthogonal-stitch (DOS)
The “Double-yarn Orthogonal-stitch” (ISO-205) offers an alternative stitch geometry and was named the DOS technique. This was applied by hand [12] using twin 0.6 mm diameter E-glass yarns for stitching the preform panels as through thickness reinforcement. The stitches were inserted in defined steps precisely following the method used to generate the SOS technique. The DOS technique has an altered stitch pattern in comparison with the MLS and SOS techniques; this is particularly apparent in the vertically and horizontally stitched specimens with two columns as is illustrated in the sketch in Fig. 5 which demonstrates the cross section of the DOS stitch pattern.
2.2.4 Comparison of SOS and DOS techniques versus MLS technique
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The alternative SOS and DOS techniques which have been applied in this work are structurally simpler than the conventionally-used modified lock-stitching technique and of considerable significance is the fact that the theoretical stitch formation does not require any angles to be made in the yarn that are greater than 90°.
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The seam is devoid of intra-looping or interlacement, both of which techniques unavoidably introduce small radius curves which reduce the performance of textile threads.
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In practice, because of the flexibility of the fabric layers being sewn, the bending of the stitching yarn is further degraded in radius. These orthogonal seams are therefore well-suited to being generated using advanced stiff fibre yarns.
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The main and common fundamental characteristic of SOS and DOS stitch geometries are that an equal space is left between two successive needle entry points and the stitching yarn is laid evenly on both sides of the fabric preform to prevent fabric deformation at the needle penetration points, as occurs when applying the commonly-used stitching methods.
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This novel stitching technique generates different stitch geometry; therefore, it positions the stitching fibre on both sides of the fabric and thus the fabric is stabilised equally during stitch insertion.
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And the most vital difference between these two alternative stitching techniques is when using the different stitch patterns, in particular vertically and horizontally when stitching two column specimens which feature two parallel columns of stitching shown in Fig. 6.
The nylon 6.6 yarn with a fibre density of 1.14 g/cm3 [27] was supplied by Oxcel and E-glass yarn with a fibre density of 2.54 g/cm3 [25] was supplied by PPG Textile [28]. All specifications of the stitching yarns are collated in Table 2. The tensile test [29] was examined for both nylon 6.6 and E-glass yarns to compare the mechanical characteristics of the stitching yarns. All mechanical characteristics of the stitching yarns are collated in Table 3.
2.3 Fabrication of Composite Panels and Test Specimens
The three steps of vacuuming, resin infusion and curing were carried out on the dry preform panels to fabricate the composite panels. In order that the 63 mm upper and lower unstitched parts of the test samples should stay separated during and after resin infusion, a non-adhesive Aerovac-A6000 ETFE release film (thickness 20 μm) was laid into the midplane of the preform panel according to the test standard before commencing the vacuuming process. Bisphenol A epoxy resin (Araldite LV 564 with a density of 1.15 g/m3) and hardener (Aradur XB 3486 with a density of 0.95 g/m3), were mixed in the proportion of 100:34 to infuse the preform panel as prescribed by the suppliers, Huntsman International LLC [30]; further preparation before infusion included gas extraction. The composite panels were cured in a Thermo-Scientific Heraeus Oven (T20P) at a temperature of 80 °C for 8 h subsequent to the infusion process. Following the curing of the preform panel, the test specimens were cut into separate pieces of 25 mm width and 125 mm length. Metal loading hinges with dimensions of 25 mm (width) x 13 mm (length) were mounted at the end of the test specimens to prepare them for DCB testing.
3 Test Methods
The unstitched and stitched composite specimens’ Mode I-IFT performances were evaluated by performing DCB tests using an Instron model-8862 machine equipped with a 100 kN load cell. Figure 7 demonstrates a DCB test specimen dimensions and configuration. The test conditions were prescribed by test standard ASTM D5528-01 [26]. The prepared DCB test specimens were held in the tensile testing machine by clamping the loading hinges in the jaws. The test specimens were initially loaded at a constant cross-head speed of 5 mm/min for the first 5 mm of crack extension to provide initial crack growth under stable conditions. The aim of the initial loading is to observe if unsteady crack growth from the insert is apparent. When the crack length reached 3 to 5 mm, the specimens were un-loaded at a constant cross-head speed of 10 mm/min and the ends of the cracks were pinpointed to check the difference in crack lengths on both edge sides of the specimens. Subsequently, the DCB composite test specimens were re-loaded at the same loading speed of 5 mm/min until the incremental crack growth extended along the entire length of the specimen (50 to 60 mm). The test specimens were then un-loaded at a constant cross-head speed of 10 mm/min to finish the DCB test. During loading, the onset of delamination crack growths was visually observed and captured using an optical microscope on the edges of the test specimens and crack lengths were noted. When crack growth was observed, at the same time, the load and displacement data were recorded digitally.
3.1 Calculation of GIC
The Mode-IFT, GIC - energy release rates were calculated by using modified beam theory (MBT) [26]. The equation is as follows:
Where: P is the Load (N), δ is the load point displacement, b is the specimen width, a is the delamination length, and Δ is determined experimentally by generating a least squares fit plot of the cube root of compliance, C1/3, as a function of delamination length. The initiation GIC-NL (NL-Deviation from Linearity) and propagation GICP values were calculated for all composite specimen groups and were used for generating a Delamination Resistance Curve (R-Curve). The R-Curve shows the relationship between the delamination length, a (mm) and the Mode I-IFT, GIC (kJ/m2).
4 Results
In total sixteen composite specimen groups were prepared for the DCB test and each type of group comprising five specimens to be tested is named in Table 4. These groups of stitched and unstitched test specimens varying in respect of stitch densities and stitching techniques were investigated and compared with each other. The average dimensions of DCB test specimens and their VF (%) are shown in Table 5.
All the fracture toughness values were calculated by using collected data from DCB testing. The overall test results are presented in the form of load–displacement curves with the help of each particular crack growth point and are displayed in the form of R-Curves with the help of GIC values and the delamination length at each particular point. The load–displacement curves and R-curves were classified as UNS-MLS, UNS-SOS, and UNS-DOS. The aim of doing this comparison was to indicate the efficiency of the stitched composites against the unstitched composites, and after eliminating the unstitched specimens, to identify the most effective stitching technique.
4.1 Load–displacement Curves
UNS; as shown in Fig. 8 the unstitched sample group, A1 (0) has been included as a reference and compared with groups stitched using the MLS, SOS, and DOS techniques. The NL displacement point appears after 4.8 mm. Sample group A1 (0) has the lowest maximum load and displacement, these being approximately 311.2 N and 12.9 mm respectively. The load reached a maximum level and remained around this maximum level for a while, and then crack propagation slowly decreased without jumping. The crack growth progressed easily and specimens were delaminated with relative ease through the entire specimen length. Hence the load–displacement curve has a smooth shape. The gradient in the linear region for sample group A1 (0) was bigger than that for all the MLS groups.
MLS; for the MLS groups: B1 [20], C1 [10], D1 [5], E1 (10 × 10), and F1 (5 × 5), the NL displacement points are close to each other and appear near the maximum load point. The crack propagation proceeded steadily as shown in Fig. 8, throughout the full specimen length. While the crack behaviour was similar in all the groups made using the MLS technique, the crack propagation behaviour was different from that of the UNS group. All the MLS groups show similarity in behaviour of delamination and crack propagation and in respect of the gradient in the linear region, but amongst these groups, the gradient for sample group F1 (5 × 5) was smaller than the others. When they reached the maximum load, they rapidly decreased with sharp jumping at each individual stitch point. Hence, these groups’ load–displacement curves have a characteristic jagged shape and the average maximum load and displacement values were variable. In general, sample groups B1 [20], C1 [10], and D1 [5] which were stitched in one column have low values of load and displacement. Amongst these groups, B1 [20] and C1 [10] have the lowest maximum average load of 311.6 N with displacements of 16.3 and 17.0 mm respectively. And group D1 [5] demonstrates the highest maximum average load and displacement. This difference seems to be influenced by featuring the shortest stitch length. However, sample groups E1 (10 × 10) and F1 (5 × 5) which were stitched in two columns have high values of load and displacement, and among these two groups; the F1 (5 × 5) has the highest maximum average load of 375.4 N with a displacement of 26.6 mm, and it is characterised by having the shortest stitch length and also by the number of columns of stitching in the specimen; this is the densest reinforcement stitching used in this work.
SOS; as shown in Fig. 9, in general, all the SOS groups: G1 [20], H1 [10], I1 [5], J1 (10 × 10) and K1 (5 × 5), the NL displacement points are quite close to each other and appear near the maximum load point. They show similar behaviour in respect of delamination and crack propagation. It can be seen that the load and displacement values increase in line with reducing stitch length and with an increased number of columns of stitches. When they reach a maximum load, they suddenly decrease sharply at each stitching point. Hence, all the SOS groups’ load–displacement curves exhibit a jagged shape. The gradient in the linear region for all the SOS groups was similar; furthermore, it shows similarity to the UNS composite group. Among sample groups G1 [20], H1 [10], and I1 [5] which were stitched in one column through the specimen length; I1 [5] has the highest maximum average value of 341.9 N with the value of 14.6 mm displacement. This performance seems to be influenced considerably by having the smallest stitch length. However, amongst the groups of J1 (10 × 10), and K1 (5 × 5) which were stitched in two columns through the specimen length, K1 (5 × 5) has by a considerable margin the highest value of maximum average load, 365.4 N, with a displacement of 15.6 mm.
DOS; as illustrated in Fig. 10, in general, for the all DOS groups: L1 [20], M1 [10], N1 [5], O1 (10 × 10) and P1 (5 × 5), the NL displacement points are close to each other and appear near the maximum load point, and test specimens show similarity in respect of their delamination and crack propagation behaviour. When they reached their maximum load, they decreased sharply at each stitching point. Hence, the load–displacement curves for all the DOS groups have a jagged shape. The gradient in the linear region for the L1 [20], N1 [5], O1 (10 × 10), and P1 (5 × 5) were similar and also show similarity with the UNS composite group. Among all the DOS groups the gradient of M1 [10] in the linear region was smaller than the others. Sample groups L1 [20], M1 [10], and N1 [5] have similar values of maximum average load and displacement, and among these groups, N1 [5] has the highest maximum average load of 323.0 N with a displacement value of 20.8 mm. The particular characteristic of these three groups is that they were stitched in one column through the specimen length. However, sample groups O1 (10 × 10), and P1 (5 × 5) were stitched in two columns through the specimen length, and of these, P1 (5 × 5) has by a considerable margin, the highest value of maximum average load 417.9 N with a displacement of 27.5 mm. It can be stated that the maximum average load values increase with reducing stitch length and with an increased number of columns of stitches.
4.2 R-Curves and GIC - Energy Release Rates
UNS; as shown in Fig. 11 the initiation GIC-NL points for the sample group A1 (0) appeared later than the other MLS specimens and the crack propagation GICP was continuous and stable. Therefore, crack growth proceeded relatively easily and specimens were smoothly delaminated throughout the entire specimen length. Hence, group A1 (0) has a low GICP value of 1.82 (kJ/m2).
MLS; Fig. 11 gives R-Curves and Fig. 12 illustrates initiation GIC-NL and propagation GICP values. Whilst the GIC-NL values are varied for all the MLS specimens, only the GIC-NL of sample group C1 [10] appeared similar to those of the unstitched sample group A1 (0), yet they still showed higher GIC-NL values than those of A1 (0) group. The GIC-NL values for sample group B1 [20], and D1 [5] appeared similar to one another, likewise, the GIC-NL points for sample group E1 (10 × 10) and F1 (5 × 5) also appeared similar to one another. Amongst the specimens tested, B1 [20], C1 [10] and D1 [5] which were all stitched in one column, D1 [5] demonstrated the highest GICP figures with the value of 2.81 (kJ/m2), by showing gradual crack growth. However, sample group B1 [20] has the lowest GIC-NL and GICP value amongst the all MLS groups, with the value of 1.42 (kJ/m2) and 1.67 (kJ/m2) respectively, as it was stitched with the longest stitch length (20 mm). Group D1 [5] is 54.4 % higher than the unstitched group A1 (0) and 68.3 % higher than group B1 [20]. It can be concluded that the concentrated stitch density has improved the Mode I-IFT. Groups of samples E1 (10 × 10) and F1 (5 × 5), were stitched in two columns, and both showed gradual crack growth and their GICP values are almost identical to one another. The propagation points of F1 (5 × 5) showed a higher degree of dispersal and this group has the highest GICP with the value of 3.54 (kJ/m2). They produced a better fracture toughness, greater than any of the other MLS groups. F1 (5 × 5) is 94.5 % higher than the unstitched samples group A1 (0) and 26 % higher than group D1 [5]. It can be concluded that the concentrated stitch density and also the number of columns of stitching have significantly improved the Mode I-IFT. In general, the standard deviation (S.D.) values of initiation and propagation are small. But, in particular sample groups D1 [5], E1 (10 × 10), and F1 (5 × 5) show the largest deviations for the initiation values. Table 6 gives the initiation GIC–NL and the average propagation GICP values for the UNS and MLS groups along with the standard deviations (S.D.) and coefficient of variation (C.V.).
The SEM photomicrographs in Fig. 13 shows the cross-section of F1 (5 × 5) along the crack propagation path of the specimen after testing. This specimen was stitched in two columns with the highest stitch density. As this group has more stitches in two columns than the other groups, it presented the highest fracture toughness value of all the MLS groups. For this heavily stitched specimen, during DCB testing, the nylon 6.6 yarn which was originally on its top surface was pulled down into the body of the laminate by the stitch legs of the E-glass yarn in the through thickness direction. As can be seen in Fig. 13, most stitches remained unbroken, but more fibre damage was created in the midplane of the sample. It can also be seen that there are resin-rich areas at the interlacement points of the stitching yarns on the surface of the specimen and at the separation points of the E-glass yarn’s stitching legs on the upper surface of the bottom part of the fractured specimen.
SOS; Fig. 14 gives the R-Curves and Fig. 15 illustrates crack initiation GIC-NL and propagation GICP values. As can be seen in Fig. 14, in general, the crack growths of all the SOS composite samples demonstrate similar behaviour on the R-curve and they have similar GIC-NL initiation values, and also relatively similar GICP propagation values. Among the sample groups G1 [20], H1 [10], and I1 [5] which were stitched in one column through the specimen length, I1 [5] has the highest GICP with a value of 2.18 (kJ/m2). Furthermore, amongst the all composite specimen groups to which the SOS technique was applied, G1 [20] has the lowest GIC-NL and GICP with a value of 1.34 (kJ/m2) and 1.81 (kJ/m2) respectively; and it has the longest stitch length at 20 mm. Sample group I1 [5] has 19.8 % higher Mode I-IFT values than the A1 (0) group and 20.4 % higher than G1 [20] group which has the longest stitch length. It can therefore be concluded that a higher stitch density bestows much improved Mode I-IFT figures. Likewise, considering the sample groups J1 (10 × 10) and K1 (5 × 5) which were stitched in two columns through the specimen length; K1 (5 × 5) has the highest GIC-NL and GICP figure with the value of 1.80 (kJ/m2) and 2.36 (kJ/m2) respectively. The slope of the crack propagation points rises slightly, and the R-curve plateau demonstrates a rise that is smaller than any of the other SOS specimens. Sample group K1 (5 × 5) is 29.7 % higher in respect of its Mode I-IFT results than the A1 (0) group and 8.3 % higher than the I1 [5] group. It is clear that the high stitch density and also the increased number of columns of stitching give significantly improved Mode I-IFT figures. The S.D. values of initiation and propagation were, in general, very small. But, in particular sample groups H1 [10], J1 (10 × 10), and K1 (5 × 5) show the largest deviations for the initiation values. Table 7 illustrates the initiation GIC–NL and the average propagation GICP values for the UNS and SOS groups together with the standard deviations (S.D.) The SEM images in Fig. 16 show a cross section of the crack propagation path of K1 (5 × 5) after DCB testing. The specimen was stitched in two columns using the SOS technique. As can be seen, delamination continues throughout the main body of the specimen without destroying the stitches. The stitch geometry in the thickness direction remained unaltered. The crack propagation was decelerated by the stitching. But along the crack propagation path, as might be expected, midplane distortion and matrix cracks can be seen. Figure 16a–d shows stitching points along the length of the composite specimen.
DOS; Fig. 17 gives R-Curves and Fig. 18 illustrates initiation GIC-NL and propagation GICP values. All the GIC-NL points appeared similar to one another by varying the initiation values for the DOS specimens. As demonstrated in Fig. 17, among the groups comprising L1 [20], M1 [10] and N1 [5] which were all stitched in a single column through the specimen length, L1 [20] and M1 [10] show similar performances in respect of their R-curves. Conversely, N1 [5] shows more dispersed propagation points than these two groups. In the column-wise comparison, the lowest GICP value belongs to the L1 [20] group and the highest GICP value belongs to the N1 [5] group, being 1.94 (kJ/m2) and 2.56 (kJ/m2) respectively. The propagation values increase progressively and it can be said that the increment depends predominantly on the increase in stitch density. Sample group N1 [5] is 40.7 % higher than the A1 (0) group and 32 % higher than the L1 [20] group. It may be concluded that the higher the stitch density, the higher is the Mode I-IFT figures. Between sample groups O1 (10 × 10), and P1 (5 × 5) which were stitched in two columns, both showed gradual crack growth, but their GICP values differ significantly from one another. The propagation points of group P1 (5 × 5) showed a higher degree of scatter and these specimens return the highest GICP figure of all the DOS groups with a value of 3.64 (kJ/m2). Sample P1 (5 × 5) is 100 % higher than the A1 (0) sample and 42.2 % higher than the N1 [5] sample. It should be noted that the conspicuously high GICP value probably derives from the high stitch density, the number of columns and furthermore, particularly depends on the use of the DOS technique. Hence, the P1 (5 × 5) sample group produced a greater Mode I-IFT than all the other sample groups. The S.D. values for the initiation and propagation values were small in general. But, in particular the P1 (5 × 5) group shows the largest deviations for the initiation values. Table 8 shows the initiation GIC–NL and the average propagation GICP values for the UNS and DOS sample groups with their standard deviations (S.D.) and coefficient of variation (C.V.).
The SEM image in Fig. 19 shows the cross section of the crack propagation path of sample P1 (5 × 5) after testing. The specimen was stitched in two columns with the DOS technique. As the specimen was stitched with a double E-glass yarn and in addition was stitched with the highest stitch density, this specimen group demonstrates improved fracture toughness by resisting delamination. Figure 19a–e shows delamination at each stitch point in the midplane.
5 Discussions
Correlation has been used as a statistical analytical tool to reveal the relationship, if any, between two or more variables. A correlation is a measure of the linear relationship between variables [31] and the correlation coefficient measures the strength and direction of the relationship between two variables as shown in Table 9.
In this study, the UNS group was taken as a reference to help compare the various stitching techniques. The different stitching geometries have been classified as MLS, SOS, and DOS techniques. The differing stitch forms and differing stitching techniques were compared with each other, and detailed examination showed the effect of stitching and also the effectiveness of each stitching technique by observing the IFT individually for Mode I. It was found that the variables, stitching technique, stitch density and the number of columns of stitching, have an effect on the GICP value, and the correlation was further examined to expose the relationship between the variables. To reveal the relationship between the variables, correlation was applied between the number of stitches per unit width and the GICP values, and between the stitch density per unit area and the GICP values. To calculate the stitches per unit width (m) and the stitch density per unit area (m2), the average dimensions of Mode I-DCB specimens were used. For the DCB specimens the average width, 0.0248 m and the average stitched area length, 0.0644 m was used as shown in Table 10.
5.1 Correlation Between Stitches per Unit Width and GICP
As shown in Fig. 20 for the UNS-MLS property, a strong relationship (r = 0.8) between stitches per unit width and GICP can be detected. However, in particular, the GICP values for the groups in which the stitch type was applied vertically in a single column are more widely spread than those of the other groups. The general trend is that the GICP values increase with an increase in the number of stitches per unit width. For the UNS-SOS property, the analysis shows a strong relationship (r = 0.7) between stitches per unit width and GICP. The general trend is that the GICP values increase with an increase in the number of stitches per unit width as for the MLS technique. Similarly to the previous correlations, a strong relationship (r = 0.8) between the number of stitches per unit width and GICP is found for the UNS-DOS property. The general trend is that the GICP values increase with an increase in the stitches per unit width as with the MLS and SOS techniques. It should be noted that the reason for the strong relationship between the number of stitches per unit width and the GICP values is convincingly associated with the intensive stitch density, the number of columns of stitching and furthermore, particularly depends on the use of the DOS stitch formation.
5.2 Correlation Between Stitch Density per Unit Area and GICP
As can be seen in Fig. 21 a very strong relationship (r = 0.9) between stitch density per unit area and GICP can be detected for the UNS-MLS property. As a general trend the GIC-PROP values increase with an increase in the stitch density per unit area. The strong relationship between the stitch density per unit area and GICP values for the MLS technique seems to be significantly influenced by high stitch density and by the stitch formation technique. Similarly to the results for UNS-MLS, the calculations for the UNS-SOS property show a very strong relationship (r = 0.9) between the stitch density per unit area and GICP. It is clear that the strong relationship between the stitch density per unit area and the GICP values of the SOS technique is influenced by the stitch formation technique and is significantly influenced by high stitch density and by the number of columns of stitch lines. For the UNS-DOS property, a very strong relationship is indicated (r = 1.0) between the stitch density per unit area and GICP. There is a general trend that the GICP values rise with an increase in the stitch density per unit area, as for the MLS and SOS techniques. It should be noted that the reason for the strong relationship between the stitch density per unit area and the GICP values is convincingly associated with the intensive stitch density, the number of columns of stitching and furthermore, it particularly depends on the use of the DOS stitch geometry.
6 Conclusions
This investigation has shown the effect of inserting stitching into textile composites and has identified effective stitching techniques by observing the interlaminar delamination resistance of a number of laminated composite samples. Table 11 compiles an overall comparison of average Mode I-IFT, GICP values which derive from unstitched and stitched groups. As can be seen in Table 11 the UNS sample group A1 (0) returns the lowest average GICP values. The composite sample group K1 (5 × 5) using the SOS technique demonstrates the second highest average GICP values with a 29.7 % increment over the UNS results. And the composite group F1 (5 × 5) using the MLS technique has the third highest GICP values with a 50 % increment over the SOS results and a 94.5 % increment over the UNS results. Of all the stitching techniques used, composite group P1 (5 × 5) using the DOS technique notably returns higher GICP values with a 2.8 % increment over the MLS technique, and 54.2 % increment over the SOS technique and a 100 % increment over the UNS results. The reason for the high GICP values of the DOS technique, which is greater than for the MLS and SOS techniques seems to be influenced by the stitch formation technique and is significantly influenced by high stitch density and by the number of columns of stitch lines.
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It was found in every case that stitching through thickness reinforcement into composite laminates provides significant resistance against interlaminar cracking (delamination) and generates high GICP values under Mode I loading, the absolute values depending on the stitching technique employed, on the stitch density and on the number of columns of stitching in the composite specimen.
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The orthogonal-stitch (ISO-205) type DOS technique showed the best performance for Mode I-IFT. The reason for the excellent GICP capabilities of the DOS stitch form, which is greater than for the MLS and SOS stitch forms, seems to be significantly influenced by the stitch geometry.
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The delamination resistance of the orthogonal-stitch (ISO-205) clearly improves as the stitch density of the reinforcement is increased, as a consequence of reduced stitch length and decreased separation between adjacent seams.
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Among all of the stitching patterns used for Mode I, the 5 × 5 mm stitch pattern demonstrated very good performances with a 74.5 % increment over the UNS results. The reason for the high GICP capability of the 5 × 5 mm stitch pattern, which is greater than any of the other tested stitching formations under Mode I, seems to be significantly influenced by the high stitch density and by the number of columns of stitching. As the stitching has a good ability to prevent crack growth, short stitch length delays fast crack growths and increases the IFT. Hence, it may be concluded that the 5 × 5 mm stitch pattern produces the highest mechanical delamination resistance performance of all the tested stitch formations even though creating more fibre damage by increasing the number of stitch penetration points, producing more fibre distortions around the inserted stitching yarns while piercing the stitching needle into the preform panels, thus causing more resin rich regions in the specimens. These factors tend to compromise the tensile properties of the specimens, however, the inserted stitching thread acts to enhance the tensile properties, so research in this area is rendered complex [32, 33].
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Göktaş, D., Kennon, W.R. & Potluri, P. Improvement of Mode I Interlaminar Fracture Toughness of Stitched Glass/Epoxy Composites. Appl Compos Mater 24, 351–375 (2017). https://doi.org/10.1007/s10443-016-9560-x
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DOI: https://doi.org/10.1007/s10443-016-9560-x