AUTEX Research Journal, Vol. 4, No4, December 2004 © AUTEX
ABRASION RESISTANCE OF COTTON/FLAX FABRICS:
COMPUTER SIMULATIONS OF FABRIC WEAR GEOMETRY
3D
1
N.G. Koltysheva, S.V. Lomov , N.N. Truevtzev
St. Petersburg State University of Technology and Design, B.Morskaya 18, 191011 St. Petersburg,
Russia – [email protected]
1
current affiliation: Department MTM, Katholieke Universiteit Leuven, Belgium –
[email protected]
Abstract
Geometrical models constructed using WiseTex software are used to describe the abrasion
resistance of flax/cotton two-layered fabrics. Good agreement with experimental observations is
found.
Keywords
abrasion, geometrical models, woven fabrics
Introduction
Purely natural textile materials are in vogue nowadays. Two-component footwear fabrics, combining a
cotton and a flax layer without a chemical bond, are a perfect example of the advantages which can
be gained by using these materials. The flax sits in the outer, ‘heavy-duty’ layer, and the cotton inside,
forming the hygienic liner of the textile footwear.
One of the important properties which determines the quality of a footwear fabric is its abrasive
resistance. The paper presents an approach to modelling the change of the fabric geometry induced
by abrasive wear. Our interest is focused on the change in the surface filling factor and the fabric
thickness with the progressive wear of the fabric. The rate of this change indicates the rate of abrasion
and allows qualitative assessment of the fabric’s resistance to wear.
A full quantitative model of abrasion must include a mechanical description of the wear process. The
approach we use is purely geometrical. However, we show that this simplified model comprises the
important generic features of wear, and can even be predictive to a certain extent.
The geometrical modelling is based on WiseTex textile modelling software [3,4], and the earlier
version of this model, CETKA software [5,6].
Similar models have been presented also in [1,2] although concerned with different problems.
1. Materials
Three types of cotton-flax fabrics were used in this study (Figure 1). All the fabrics have the following
common features:
− The same flax (92 tex in warp, 97 tex in weft) and cotton (155 tex) yarns are used.
− The weave has two layers.
− Flax yarns are used in the outer (face) layer of warp, and in both weft layers; cotton yarns form
the inner (back) layer of warp.
− The flax yarns stay almost circular in the fabric, the cotton yarn is flattened (compression
coefficient 0.6).
The models of the fabrics were created with WiseTex software. Figure 2 illustrates the qualitative
adequacy of the models. The twill pattern on the face of the fabric is well represented by the
computer-generated image. The roughness of the surface, important to the abrasive resistance, is
also featured in the models. Upper flax warp yarns are well over the upper flax weft, creating a rough
surface with ‘hills’ and ‘valleys’.
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Figure 1. Flax/cotton fabrics. Weaves (face/bottom): 1 – plain/plain; 2 – basket/twill; 3 – plain/twill
Figure 2. Face (top) and back (bottom) of fabric 3. Photos and WiseTex simulations
The comparison with the specified and measured fabric parameters (areal density, thickness, yarn
crimp) shows good correspondence between the computed and experimental values. This allows the
models to be used for the further study of the fabrics’ internal geometry and changes in wear.
2. Virtual ‘Microtoming’
To model the abrasion wear, the sections of the fabrics were created using the WiseTex tools (Figure
3). The sections were made parallel to the fabric surface at the depth step of 1% of the fabric
thickness, and the relative area S of the sectioned yarns (surface filling factor) was computed for each
section. Figure 3 shows the dependence of S on the position of the section.
At the beginning, the graphs for fabrics 1 and 3 coincide. The sections in this region include the yarns
of the upper warp only, which are of the same weave pattern (plain) and of the same geometry for
these fabrics. The basket weave in the face of fabric 2 creates a higher surface in the sections in this
region.
When the section goes deeper in the sample, it starts to include warp cotton yarns of the bottom layer.
The rate of the increase in S is higher for fabric 1, because it has a plain weave for the bottom layer,
as opposite to the weft-effect weaves of the fabrics 2 and 3.
A sharp minimum at the depth of 60% for samples 2 and 3 is explained by the transition of the
sections from the top to the bottom weft yarns. For fabric 1 this effect is shaded by the presence of
large sections of the plain-woven warp yarns.
For the depth of over 60%, the graph for fabric 1 goes lower than that for fabrics 2 and 3. This can be
explained by the weft-effect of the back layer weaves of the former fabrics.
Using the computed data, the mass distribution of the fibrous material through the fabric thickness can
be derived. We assume that:
− the density of the fibrous assemblies are the same in all the yarns;
− the volume of fibres between the two neighbouring sections is proportional to S.
With these two assumptions, the mass distribution curve would follow the S~h curves of Figure 3.
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0.02
0.018
0.016
0.014
S
0.012
1
2
3
0.01
0.008
0.006
0.004
0.002
0
1
11
21
31
41
51
61
71
81
91
h, %
Figure 3. Relative yarn surface at the fabric sections vs. the section depth
3. Experiment in abrasive wear
An experimental study of the abrasive wear of the flax/cotton fabrics has been performed on the IM3M rig. The load of 10 N and sand paper was used. After each 200 rotations the rig was stopped, the
fibrous dust removed and the sample weighed.
Using the mass distribution curves, the data of the mass loss of the samples was transformed into the
dependency of the fabric thickness on the number of rotations of the abrasive disk (Figure4).
Reduction of thickness, %
45
40
35
30
3
25
2
20
1
15
10
5
0
0
500
1000
1500
2000
2500
3000
3500
Rotations
Figure 4. Reduction of the thickness of the fabrics vs number of rotations of the abrasive disk
A reasonable assumption of the criterion of a fabric’s full disintegration would be the onset of the
destruction of warp/weft yarns in all the layers. The geometric modelling predicts this onset to start at
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the reduction of thickness of 35…40% (Figure5), which is in good agreement with the experimental
observations.
damaged flax
weft yarns,
layer 1
completely
damaged flax
warp yarns,
layer 1
onset of damage in cotton
warp yarns, layer 2
Figure 5. Damage pattern of fabric 3, thickness reduction of 40%
4. Conclusions
The geometrical WiseTex modelling of two-layered flax/cotton fabrics provides a tool for ‘virtual
microtoming’ the fabrics. The dependencies of the area of fibrous material in a section on the section
depth and the yarn damage pattern in the sections proved to be a useful instrument for assessing the
resistance of the fabrics to abrasive wear, and for explaining the phenomena observed in the wear test
with the abrasive disk.
Acknowledgments
This work was done within the scope of the NATO project SfP 973658-FLAX. The work by S.V. Lomov
in The Catholic University of Leuven was carried out as part of the following projects: ‘Development of
unified models for the mechanical behaviour of textile composites’ (GOA/98/05), funded by the
Flemish Government through the Research Council of the Catholic University of Leuven, ‘Advanced
numerical techniques in R&D on processing and properties of textiles and textile composites’ (IWT000148), funded by the Flemish Government, and ‘Technologies for Carbon Fibre Reinforced Modular
Automotive Body Structures’ (TECABS, Brite-Euram), funded by the European Commission. The
authors are grateful to Prof. I. Verpoest, Catholic University of Leuven, for permission to use WiseTex
software in this study.
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