Experimental and numerical analyses of textile reinforcement forming of a tetrahedral shape
Introduction
In Liquid Composite Moulding (LCM) processes, a resin is injected on a textile preform [1], [2], [3]. The shape of this preform can be complex. It can be obtained by a punch and die forming process from initially flat textile reinforcement. In case of double curved shapes, the forming process may be delicate because it needs in-plan deformations of the textile reinforcement and especially in-plane shear strains. A blank holder is then generally necessary in order to obtain a preform without defects (an especially with no wrinkles).
The experimental analysis and the numerical simulation of this forming process of the textile reinforcement are important in order to determine the conditions for a successful manufacturing of a preform (without defects). In addition they can determine the direction and the density of the fibres at any point on the preform after forming. Those directions are much depending on the forming process because shear angles between warp and weft yarns due to manufacturing can be large when the final shape is double curved. These directions condition the mechanical behaviour of the final solid composite, but also the filling of the resin in the case of a liquid moulding process [4], [5], [6].
The experimental devices for forming of textile preforms with deformation and loads measurements facilities are of main importance for the understanding of deformation modes and for the analysis of the defects that can occur during the forming. Concerning punch and die forming of textile preforms, several experimental forming system have been designed for hemispherical forming [7], [8], [9], [10], [11], [12], [13], [14], [15] (and extended hemispherical shape [16]). The hemispherical shape is much studied because it is rather simple, it is double curved and leads to large shear angles (about 45°). In the present paper an experimental device is presented for the forming of a tetrahedral shape which is those of corner fitting parts (or corner brackets). This shape is strongly double curved and is more difficult to form than an hemispherical part especially when the radius of curvature are small. It is shown that it is possible to manufacture this preform by punch and die forming thanks to a strong blank holder load and appropriate mechanical properties of the textile reinforcement (the thin interlock G1151® in the present work). There is no wrinkle in the tetrahedral part of the preform but many wrinkles in the plane zone due to the six blank holders. A main results given by this forming experiment concern the ‘locking angle’ This locking angle is commonly considered as the angle corresponding to the onset of wrinkling [17], [18], [19], [20]. It is shown that very large shear angle are necessary for the tetrahedral forming but there is no wrinkle in this zone. Conversely there are many wrinkles in other areas where the shear angle are much smaller.
A main interest of the experimental forming device is validation of numerical forming simulations. These simulations permit to avoid the trial–error approaches for the development of forming processes and they also compute the directions and densities of the fibres before the injection stage. There are many simulation methods that are developed today based on different approaches (see Section 3) and it is important to know their abilities and their limits. The tetrahedral forming device is used to validate the semi-discrete simulation approach presented in [21]. In this approach (that is briefly described in Section 3) a finite element is made up of woven unit cells. The tensile, in-plane shear and bending internal virtual work are directly computed from the nodal displacements and from the mechanical properties obtained by experimental tests specific to textile composite reinforcements. This finite element is a shell element because bending stiffness is important for wrinkling simulations. In order to improve the numerical efficiency, a rotation-free formulation is used [22], [23]. There are no rotation degrees of freedom but the curvatures are computed from the position of the neighbouring elements.
The numerical/experimental comparison concerns principally two points: the shear angles and the deformed shape, especially the shape of the wrinkles. The agreement is good. In particular, the simulation gives a realistic description of the wrinkles after forming. This is possible with the semi-discrete approach because the bending strain energy and the bending behaviour of the reinforcement (that is very specific) are considered. Some numerical analyses have been presented on onset of wrinkles [10], [13], but they do not depict the shape of the wrinkles because they are based on membrane approaches and neglect the bending stiffness that conditions the wrinkle shape. However in a forming process such as the tetrahedral forming presented in this paper, it is not possible to avoid all wrinkles. The numerical simulation must check that the process conditions insure that those wrinkles do not expand in the useful part of the preform. In that goal, the computation of the shape of the wrinkles after forming, as it is performed in the present study, is important.
Section snippets
Motivation
The development of one specific device able to preform woven textile reinforcement has two main objectives. First, such a device permit to experimentally analyze the possibilities to manufacture a double curved composite structure without defects in the useful part with a given textile reinforcement. The role of the blank holders, of the pretensions, of the speed of the tools…can be investigated. This is very useful because the composite forming processes do not benefit from so much experience
Different approaches for preforming simulations
To simulate draping of textile composite reinforcement, several packages are commercially available based on “kinematical models” [37], [38], [39]. This method is very fast but does not account for the mechanical behaviour of the woven reinforcement for possible sliding of the fabric with regard to the tools and for load boundary conditions. These points are very important in the case of preforming with punch and die. A complete physical simulation of a composite forming process needs a model
Comparison between forming simulations and forming experiments
The forming experiments have been described in Section 2. The geometry of the tools used in the simulations is given in Fig. 9. The tetrahedral punch is in green, the die is in blue and the six blank holders are in red. The fabric is the G1151® interlock fabric described in Section 2.3. The mechanical properties used in the present simulations for membrane and bending behaviour are given in Table 1. The pressure on the blank holder is 1 bar on 32 mm diameter pistons. This load is important since
Conclusion
An experimental device for textile composite preforming has been presented. It has been shown that a tetrahedral shape used for corner brackets can be formed by punch and die without wrinkles in the useful part. This forming process has been possible thanks to strong loads on the blank holders and because the G1151® reinforcement is well suitable to the forming that need large shear angles. This experimental device is of main importance in order to test and to validate the software’s used to
Acknowledgements
The work reported here has been carried out in the scope of the project ITOOL (European Commission), of the project LCM3M (ANR, French National Research Agency) and has been supported by EADS IW company.
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