abrasion resistance of cotton/flax fabrics - Autex Research Journal

abrasion resistance of cotton/flax fabrics - Autex Research Journal abrasion resistance of cotton/flax fabrics - Autex Research Journal

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AUTEX Research Journal, Vol. 4, No4, December 2004 © AUTEX ABRASION RESISTANCE OF COTTON/FLAX FABRICS: 3D COMPUTER SIMULATIONS OF FABRIC WEAR GEOMETRY N.G. Koltysheva, S.V. Lomov 1 , N.N. Truevtzev St. Petersburg State University of Technology and Design, B.Morskaya 18, 191011 St. Petersburg, Russia – mtvm@sutd.ru 1 current affiliation: Department MTM, Katholieke Universiteit Leuven, Belgium – Stepan.Lomov@mtm.kuleuven.ac.be 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’. http://www.autexrj.org/No4-2004/0125.pdf 182

AUTEX <strong>Research</strong> <strong>Journal</strong>, Vol. 4, No4, December 2004 © AUTEX<br />

ABRASION RESISTANCE OF COTTON/FLAX FABRICS: 3D<br />

COMPUTER SIMULATIONS OF FABRIC WEAR GEOMETRY<br />

N.G. Koltysheva, S.V. Lomov 1 , N.N. Truevtzev<br />

St. Petersburg State University <strong>of</strong> Technology and Design, B.Morskaya 18, 191011 St. Petersburg,<br />

Russia – mtvm@sutd.ru<br />

1 current affiliation: Department MTM, Katholieke Universiteit Leuven, Belgium –<br />

Stepan.Lomov@mtm.kuleuven.ac.be<br />

Abstract<br />

Geometrical models constructed using WiseTex s<strong>of</strong>tware are used to describe the <strong>abrasion</strong><br />

<strong>resistance</strong> <strong>of</strong> <strong>flax</strong>/<strong>cotton</strong> two-layered <strong>fabrics</strong>. Good agreement with experimental observations is<br />

found.<br />

Keywords<br />

<strong>abrasion</strong>, geometrical models, woven <strong>fabrics</strong><br />

Introduction<br />

Purely natural textile materials are in vogue nowadays. Two-component footwear <strong>fabrics</strong>, combining a<br />

<strong>cotton</strong> and a <strong>flax</strong> layer without a chemical bond, are a perfect example <strong>of</strong> the advantages which can<br />

be gained by using these materials. The <strong>flax</strong> sits in the outer, ‘heavy-duty’ layer, and the <strong>cotton</strong> inside,<br />

forming the hygienic liner <strong>of</strong> the textile footwear.<br />

One <strong>of</strong> the important properties which determines the quality <strong>of</strong> a footwear fabric is its abrasive<br />

<strong>resistance</strong>. The paper presents an approach to modelling the change <strong>of</strong> the fabric geometry induced<br />

by abrasive wear. Our interest is focused on the change in the surface filling factor and the fabric<br />

thickness with the progressive wear <strong>of</strong> the fabric. The rate <strong>of</strong> this change indicates the rate <strong>of</strong> <strong>abrasion</strong><br />

and allows qualitative assessment <strong>of</strong> the fabric’s <strong>resistance</strong> to wear.<br />

A full quantitative model <strong>of</strong> <strong>abrasion</strong> must include a mechanical description <strong>of</strong> the wear process. The<br />

approach we use is purely geometrical. However, we show that this simplified model comprises the<br />

important generic features <strong>of</strong> wear, and can even be predictive to a certain extent.<br />

The geometrical modelling is based on WiseTex textile modelling s<strong>of</strong>tware [3,4], and the earlier<br />

version <strong>of</strong> this model, CETKA s<strong>of</strong>tware [5,6].<br />

Similar models have been presented also in [1,2] although concerned with different problems.<br />

1. Materials<br />

Three types <strong>of</strong> <strong>cotton</strong>-<strong>flax</strong> <strong>fabrics</strong> were used in this study (Figure 1). All the <strong>fabrics</strong> have the following<br />

common features:<br />

− The same <strong>flax</strong> (92 tex in warp, 97 tex in weft) and <strong>cotton</strong> (155 tex) yarns are used.<br />

− The weave has two layers.<br />

− Flax yarns are used in the outer (face) layer <strong>of</strong> warp, and in both weft layers; <strong>cotton</strong> yarns form<br />

the inner (back) layer <strong>of</strong> warp.<br />

− The <strong>flax</strong> yarns stay almost circular in the fabric, the <strong>cotton</strong> yarn is flattened (compression<br />

coefficient 0.6).<br />

The models <strong>of</strong> the <strong>fabrics</strong> were created with WiseTex s<strong>of</strong>tware. Figure 2 illustrates the qualitative<br />

adequacy <strong>of</strong> the models. The twill pattern on the face <strong>of</strong> the fabric is well represented by the<br />

computer-generated image. The roughness <strong>of</strong> the surface, important to the abrasive <strong>resistance</strong>, is<br />

also featured in the models. Upper <strong>flax</strong> warp yarns are well over the upper <strong>flax</strong> weft, creating a rough<br />

surface with ‘hills’ and ‘valleys’.<br />

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AUTEX <strong>Research</strong> <strong>Journal</strong>, Vol. 4, No4, December 2004 © AUTEX<br />

Figure 1. Flax/<strong>cotton</strong> <strong>fabrics</strong>. Weaves (face/bottom): 1 – plain/plain; 2 – basket/twill; 3 – plain/twill<br />

Figure 2. Face (top) and back (bottom) <strong>of</strong> fabric 3. Photos and WiseTex simulations<br />

The comparison with the specified and measured fabric parameters (areal density, thickness, yarn<br />

crimp) shows good correspondence between the computed and experimental values. This allows the<br />

models to be used for the further study <strong>of</strong> the <strong>fabrics</strong>’ internal geometry and changes in wear.<br />

2. Virtual ‘Microtoming’<br />

To model the <strong>abrasion</strong> wear, the sections <strong>of</strong> the <strong>fabrics</strong> were created using the WiseTex tools (Figure<br />

3). The sections were made parallel to the fabric surface at the depth step <strong>of</strong> 1% <strong>of</strong> the fabric<br />

thickness, and the relative area S <strong>of</strong> the sectioned yarns (surface filling factor) was computed for each<br />

section. Figure 3 shows the dependence <strong>of</strong> S on the position <strong>of</strong> the section.<br />

At the beginning, the graphs for <strong>fabrics</strong> 1 and 3 coincide. The sections in this region include the yarns<br />

<strong>of</strong> the upper warp only, which are <strong>of</strong> the same weave pattern (plain) and <strong>of</strong> the same geometry for<br />

these <strong>fabrics</strong>. The basket weave in the face <strong>of</strong> fabric 2 creates a higher surface in the sections in this<br />

region.<br />

When the section goes deeper in the sample, it starts to include warp <strong>cotton</strong> yarns <strong>of</strong> the bottom layer.<br />

The rate <strong>of</strong> the increase in S is higher for fabric 1, because it has a plain weave for the bottom layer,<br />

as opposite to the weft-effect weaves <strong>of</strong> the <strong>fabrics</strong> 2 and 3.<br />

A sharp minimum at the depth <strong>of</strong> 60% for samples 2 and 3 is explained by the transition <strong>of</strong> the<br />

sections from the top to the bottom weft yarns. For fabric 1 this effect is shaded by the presence <strong>of</strong><br />

large sections <strong>of</strong> the plain-woven warp yarns.<br />

For the depth <strong>of</strong> over 60%, the graph for fabric 1 goes lower than that for <strong>fabrics</strong> 2 and 3. This can be<br />

explained by the weft-effect <strong>of</strong> the back layer weaves <strong>of</strong> the former <strong>fabrics</strong>.<br />

Using the computed data, the mass distribution <strong>of</strong> the fibrous material through the fabric thickness can<br />

be derived. We assume that:<br />

− the density <strong>of</strong> the fibrous assemblies are the same in all the yarns;<br />

− the volume <strong>of</strong> fibres between the two neighbouring sections is proportional to S.<br />

With these two assumptions, the mass distribution curve would follow the S~h curves <strong>of</strong> Figure 3.<br />

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AUTEX <strong>Research</strong> <strong>Journal</strong>, Vol. 4, No4, December 2004 © AUTEX<br />

0.02<br />

0.018<br />

0.016<br />

0.014<br />

S<br />

0.012<br />

0.01<br />

0.008<br />

0.006<br />

0.004<br />

0.002<br />

1<br />

2<br />

3<br />

0<br />

1 11 21 31 41 51 61 71 81 91<br />

h, %<br />

Figure 3. Relative yarn surface at the fabric sections vs. the section depth<br />

3. Experiment in abrasive wear<br />

An experimental study <strong>of</strong> the abrasive wear <strong>of</strong> the <strong>flax</strong>/<strong>cotton</strong> <strong>fabrics</strong> has been performed on the IM-<br />

3M rig. The load <strong>of</strong> 10 N and sand paper was used. After each 200 rotations the rig was stopped, the<br />

fibrous dust removed and the sample weighed.<br />

Using the mass distribution curves, the data <strong>of</strong> the mass loss <strong>of</strong> the samples was transformed into the<br />

dependency <strong>of</strong> the fabric thickness on the number <strong>of</strong> rotations <strong>of</strong> the abrasive disk (Figure4).<br />

Reduction <strong>of</strong> thickness, %<br />

45<br />

40<br />

35<br />

30<br />

25<br />

20<br />

15<br />

10<br />

5<br />

0<br />

0 500 1000 1500 2000 2500 3000 3500<br />

Rotations<br />

3<br />

2<br />

1<br />

Figure 4. Reduction <strong>of</strong> the thickness <strong>of</strong> the <strong>fabrics</strong> vs number <strong>of</strong> rotations <strong>of</strong> the abrasive disk<br />

A reasonable assumption <strong>of</strong> the criterion <strong>of</strong> a fabric’s full disintegration would be the onset <strong>of</strong> the<br />

destruction <strong>of</strong> warp/weft yarns in all the layers. The geometric modelling predicts this onset to start at<br />

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AUTEX <strong>Research</strong> <strong>Journal</strong>, Vol. 4, No4, December 2004 © AUTEX<br />

the reduction <strong>of</strong> thickness <strong>of</strong> 35…40% (Figure5), which is in good agreement with the experimental<br />

observations.<br />

damaged <strong>flax</strong><br />

weft yarns,<br />

layer 1<br />

onset <strong>of</strong> damage in <strong>cotton</strong><br />

warp yarns, layer 2<br />

completely<br />

damaged <strong>flax</strong><br />

warp yarns,<br />

layer 1<br />

Figure 5. Damage pattern <strong>of</strong> fabric 3, thickness reduction <strong>of</strong> 40%<br />

4. Conclusions<br />

The geometrical WiseTex modelling <strong>of</strong> two-layered <strong>flax</strong>/<strong>cotton</strong> <strong>fabrics</strong> provides a tool for ‘virtual<br />

microtoming’ the <strong>fabrics</strong>. The dependencies <strong>of</strong> the area <strong>of</strong> fibrous material in a section on the section<br />

depth and the yarn damage pattern in the sections proved to be a useful instrument for assessing the<br />

<strong>resistance</strong> <strong>of</strong> the <strong>fabrics</strong> to abrasive wear, and for explaining the phenomena observed in the wear test<br />

with the abrasive disk.<br />

Acknowledgments<br />

This work was done within the scope <strong>of</strong> the NATO project SfP 973658-FLAX. The work by S.V. Lomov<br />

in The Catholic University <strong>of</strong> Leuven was carried out as part <strong>of</strong> the following projects: ‘Development <strong>of</strong><br />

unified models for the mechanical behaviour <strong>of</strong> textile composites’ (GOA/98/05), funded by the<br />

Flemish Government through the <strong>Research</strong> Council <strong>of</strong> the Catholic University <strong>of</strong> Leuven, ‘Advanced<br />

numerical techniques in R&D on processing and properties <strong>of</strong> textiles and textile composites’ (IWT-<br />

000148), funded by the Flemish Government, and ‘Technologies for Carbon Fibre Reinforced Modular<br />

Automotive Body Structures’ (TECABS, Brite-Euram), funded by the European Commission. The<br />

authors are grateful to Pr<strong>of</strong>. I. Verpoest, Catholic University <strong>of</strong> Leuven, for permission to use WiseTex<br />

s<strong>of</strong>tware in this study.<br />

References<br />

1. Szosland J., Air Permeability <strong>of</strong> Woven Multilayer Composite Textiles, Fibres & Textiles in<br />

Eastern Europe, vol.7, No.1(24), 1999, pp.34-37.<br />

2. Szosland J., Identyfication <strong>of</strong> Structure <strong>of</strong> Inter-Thread Channels in Models <strong>of</strong> Woven Fabrics,<br />

Fibres & Textiles in Eastern Europe, vol.7, No.2(25), 1999, pp.41-45.<br />

3. Lomov, S.V., Huysmans, G., Verpoest, I. Hierarchy <strong>of</strong> textile structures and architecture <strong>of</strong><br />

fabric geometric models. Textile <strong>Research</strong> <strong>Journal</strong>, vol.71, No.6, 2001, 534-543.<br />

4. Lomov, S.V., Huysmans, G., Luo, Y., Parnas, R.S., Prodromou, A., Verpoest, I., Phelan, F.R.,<br />

Textile composites: Modelling strategies, Composites A, vol. 32, No.10, 2001, 1379-1394.<br />

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AUTEX <strong>Research</strong> <strong>Journal</strong>, Vol. 4, No4, December 2004 © AUTEX<br />

5. Lomov S.V., Truevtzev N.N. A s<strong>of</strong>tware package for the prediction <strong>of</strong> woven <strong>fabrics</strong><br />

geometrical and mechanical properties, Fibres & Textiles in Eastern Europe, vol.3, No.2,<br />

1995, 49-52.<br />

6. Gusakov, A.V. and S.V. Lomov, Parametric studies <strong>of</strong> the internal structure <strong>of</strong> 3D woven<br />

<strong>fabrics</strong>. Fibres & Textiles in Eastern Europe, 6, No.2, 1998, 60-63.<br />

∇∆<br />

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