The paper deals with the modelling of the physical behaviour of woven structures imitating the textile fabrics. The model is based on a combined approach which presents longitudinal elastic properties of each yarn by a system of non-volumetric structural elements (springs), while the collision search and response algorithm works in a 3D space based on tight-fitting of the yarns by using oriented bounding boxes (OBB). The separation axis theorem (SAT) for collision detection between OBBs is performed. Collision response is performed by applying collision impulses to colliding nodes thus avoiding interpenetrations of the yarns. A simplified approach is applied in order to take into account the deformation of the cross-section of a yarn. It is assumed that the cross-sectional area remains constant all the time while its shape is elliptic with changing lengths of axes. Numerical examples of simulation of tension, warp and shooting-through the fabric are presented. 1. Indroduction The problematic of the computational models for simulation of the textile structures is defined mainly by the necessity to present the behaviour of the material in two different length scales. At the macro- scale one is inclined to regard a fabric as a continuous membrane. At the same time a textile fabric is not a continuum as at the micro-level its behaviour is de- fined by the contact interactions of the yarns in the woven structure. The dimension of this micro-struc- tural level is finite and may be very complex depend- ing upon the properties of the yarn and of the weave. The continua based approximations of the fabric beha- viour are always only rough approximations of the real fabric. Moreover, different continua-based models for modelling different situations (extension, warping, failure, etc.) may be necessary. Therefore the model- ling of the fabric by directly including the weave geometry and physical behaviour into the model is preferable. Implementations of the woven structure models can be performed by using the finite element method (FEM) computational environments such as LSDYNA, ABAQUS Explicit, DYTRAN, etc. The dimensionality of the obtained models is huge as each yarn has to be presented as the volumetric finite element structure. Moreover, in applications focused on the problem-specific area of the simulation of the physical behaviour of a fabric, significant model im- plementation efforts are necessary. Therefore the development of more efficient physically-based approximate models of a yarn structure is an important issue at the present time.
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