Abstract
The aim of this study was to determine the in-plane shear properties of polyester satin fabric by the pull-out method and analytical relations were developed to calculate the shearing properties.
After the yarn in the fabric was pulled from the top ravel region, before the start of the crimp extension stage, it was found that fabric shear strength and rigidity increased when the number of pulled ends increased. In addition, when the fabric dimensions increased, fabric shear strength and rigidity increased. Also, the shear rigidity values in untreated fabric were high compared to that of treated fabric due to the effect of softening agent on the fabric structure.
It was observed that fabric sample dimensions and the number of pull-out ends as well as the fabric treatments influenced fabric shear strength and rigidity. The shear jamming angles were found to be based on the number of pulled ends. Fabric local shearing properties could be identified by pulling the yarn ends in various regions of the fabric. This could be important for the handling of the fabric during formation. The results generated from this study showed that polyester fabric shear could be measured by the yarn pull-out test.
Keywords
Introduction
Shearing allows dry fabric to be formed into complex shapes. 1 A simple shear device fixed to a tensile tester was developed to measure the simple shear in a fabric. Shear force-angular deformation before the development of local wrinkles and internal yarn-to-yarn friction in the fabric structure were identified. It was observed that the largest shear angular deviation was obtained when wrinkles appear. 2 The energy loss of the total work carried out indicated large frictional losses at yarn cross-over points at high normal stresses. It was also found that rectangular specimens were better than square specimens due to the latters’ tendency to have wrinkling during shearing. 3 On the other hand, it was observed that hysteresis occurs when the direction of shear was reversed due to it overcoming the frictional forces that exist in the intersection region between the warp and weft. Frictional forces always oppose the applied shearing force. 4
A shear tester (KES-F) based on the simple shear test principle was developed. 5 Another method used for measuring fabric shear was by bias-extension where a rectangular fabric sample was cut at 45° in the principal yarn directions and uniaxial tensile load was applied to identify the shear angle. 6 – 9 On the other hand, a fixture was developed in the bias-extension method, called the picture-frame (or trellis-frame) to conduct the shear test on a square fabric sample where the shear lock limit was reached. 10 There were inconsistencies between the fabric properties measured in simple shear and by bias-extension due to factors including the specimen geometry, thread properties and variation in normal stress during bias-extension.1,7
Fabric shear behavior was found to depend on applied tension, specimen size and fabric sett. Buckling due to specimen size affected the fabric’s shear rigidity.11,12 It was pointed out that the limits of shear were usually determined geometrically. For a wide range of conventional fabrics, the shear limit was defined by the side-by-side contact of one set of yarns. 13 By using the picture-frame shear test method, a microstructural analysis was carried out in high modulus fiber based fabrics to investigate shear locking on the basis of a geometrical approach and the maximum packing fiber fraction. 14
An edge-clamped fabric holding fixture was developed. However, transverse tension applied to the fabric through a spring-mounted sliding edge clamp prevented the measurement of the fabric’s simple shear.15,16 A similar fixture was used to conduct a fabric pull-out test in which small fabric dimensions were chosen (length 51 mm× width 7 mm) to prevent shear deformation and transverse tension induced by pull-out force. 17
The aim of this study was to determine the in-plane shear properties of polyester satin fabric by the pull-out method and to interpret the shear behavior of this fabric based on the generated data and developed analytical model.
Principle of experiment
Shear force-angle relationship
We can use the simple shear relations to calculate the shear angle. As,
Shear angle can be defined as,
In addition, shear rigidity from the simple shear can be considered1,
Then, shear rigidity can equal to
Specific shear rigidity can be defined as
Materials and methods
Woven fabrics
Continuous filaments of polyester air-entangled textured yarn (Advansa, Turkey) were used to produce the woven fabrics. The linear density of this yarn was 33.33 tex and it has 68 filaments in a cross-section. It also has 10/10 cm entanglement. The woven fabrics were designed as 1/4 satin weave. The warp and filling densities of the fabrics were 38 ends/cm and 18 ends/cm, respectively. The weight of the fabric unit area was 247 g/m2. The warp and filling crimp ratios were 22.18% and 11%, respectively. The fabric thickness was 1.06 mm. The fabrics were produced by an air-jet weaving machine (Picanol Omni Plus-800, Belgium). Fabrics were treated with non-ionic softening agent (Ceralube SVN liq, Clariant Ltd., Switzerland). The solution, which included 50 g/L softening agent, applied to the fabric by padding method. The pick-up rate was 100%. Treated fabrics were dried under laboratory conditions. Crimp measurement was performed using a Tautex digital instrument (James H. Heal Co., UK) according to ISO 7211-3. The fabric thickness measurement was performed using an R&B cloth thickness tester (James H. Heal Co., UK) according to ISO 5084. The fabric weight measurement was performed based on ISO 6348 using an Ohaus Adventurer™ Pro AV812 (Ohaus Corp. USA) digital balance.
In-plane shear test by pull-out method
Pull-out test was conducted to determine fabric shear in the frayed edge of the plain fabric structure. For this reason, a pull-out fixture was developed. Figure 1 shows the fixture with the fabric during the shear test by the pull-out method in the testing instrument. Figure 2 shows schematic views of the fabric and yarn pulled-ends for fabric shear by the pull-out test, before and after the test. The fixture consists of a base to hold the testing instrument; a sliding frame to adjust the position of the yarn end to be pulled from the testing instrument; and a fabric holder with screws to apply the required pressure to both edges of the fabric sample via a metal plate.
18
Fabric from both edges was clamped under no pre-tension. In this set-up, fabric shear (fabric displacement) was defined as ‘displacement that is received under the applied tensile load on single (one yarn) or multiple yarn ends (two, three, four or five) in the fabric just before the crimp extension starts’ and crimp extension was defined as ‘yarn length that is received under the applied tensile load on a single yarn end in the fabric structure due to interlacement’. The maximum fabric shear displacement (fabric displacement) was measured during pull-out testing on the yarn pulled region as seen schematically in Figure 2. Shear force was received by testing instrument. In addition, shear angle was calculated based on shear displacement. Shear rigidity was also calculated based on simple shear principles. Fabric crimp interchange during pull-out test was ignored due to clamped fabric edges. The yarn slippages in warp and weft directions in the fabric interlacement regions were not considered for simplification purposes. The testing instrument used was the Instron 4411 and the testing speed was 100 mm/min.
Pull-out fixture with fabric sample on the tensile testing instrument. Schematic views of the fabric and yarn pulled-ends for fabric shear by the pull-out test; initial fabric position before fabric shear by pull-out test (left), fabric shear before crimp extension starts (right).

Pull-out test dimensions of softening treated and untreated polyester woven fabric samples
Results and discussion
Shear force-angle results
Fabric shear by the yarn pull-out test on polyester fabric samples was carried out. The test results on untreated and treated satin fabrics are presented in Tables 2–3 and 4–5, respectively. Figure 3 shows the shear force-angle curve for shearing the weft in the fabric during the applications of tensile pulling force to the warp yarns.
Woven fabric shear force-angle curve in warp direction of fabric part A and B before crimp extension stage. (fabric: polyester untreated fabric; pulled ends: 5 yarns; fabric width and length: 30 × 30 cm). Shear results of untreated satin fabrics by pull-out test for various fabric dimensions to warp direction Shear results of untreated satin fabrics by pull-out test for various fabric dimensions to weft direction
Fabric shear resulting from the yarn pull-out test was observed. Based on these results, the shear force-angle curve was defined and is shown in Figure 3. When the pulled yarn reaches the point just before where the crimp extension stage starts, this is defined as the maximum shear force-displacement. As seen in Figure 3, there are two regions in the fabric, called A and B, in maximum shear force-displacement. The yarn pulled region is at the center of the fabric. The A and B regions of the fabric are considered equal. In this case, the shear force-displacement curves seen in regions A and B are equal to each other but, they are in opposite regions in the coordinate system. The tensile base pulled forces and equivalent fabric displacements were recorded. Then, fabric displacement was converted to angular displacement by using equation 3. The shear force-angle curves obtained from the yarn pull-out test appeared to be similar to those in the simple shear and bias-extension shear methods. The initial position of the curves was proportional, but after that it showed a slight non-linear behavior in which there was slight shear angle rotation compared to the increasing level of shear force. The curve was also wavy due to micro-slippage between yarn sets at the interlacement region.
Figure 4 shows the shear force-angle curve for shearing the weft and warp in the untreated polyester satin fabrics during the application of tensile pulling force applied on the warp and weft yarns, respectively. Figure 5 shows the shear force-angle curve for shearing the weft and warp in the treated polyester satin fabrics during the application of tensile pulling force applied on the warp and weft yarns, respectively.
Shear force-angle curves of untreated polyester satin fabrics. a) Pulled ends: 1–5, pulled direction: warp, fabric width: 5 cm, fabric length: 20 cm. b) Pulled ends: 1–5, pulled direction: warp, fabric width: 30 cm, fabric length: 20 cm. c) Pulled ends: 1–5, pulled direction: weft, fabric width: 5 cm, fabric length: 20 cm. d) Pulled ends: 1–5, pulled direction: weft, fabric width: 30 cm, fabric length: 20 cm. Shear force-angle curves of softening agent treated polyester satin fabrics. a) Pulled ends:1–5, pulled direction: warp, fabric width: 5 cm, fabric length: 20 cm. b) Pulled ends:1–5, pulled direction: warp, fabric width: 30 cm, fabric length: 20 cm. c) Pulled ends:1–5, pulled direction: weft, fabric width: 5 cm, fabric length: 20 cm. d) Pulled ends:1–5, pulled direction: weft, fabric width: 30 cm, fabric length: 20 cm.

In Figure 4(a) and (b), the shear force-angle curves for shearing the weft by 1–5 pulled yarn ends in untreated narrow and wide fabrics were presented, respectively. In Figure 4(c) and (d), the shear force-angle curves for shearing the warp by 1–5 pulled yarn ends in untreated narrow and wide fabrics were also presented, respectively. It was observed that the shear force-angle curves and the number of pulled ends were proportional. When the number of pulled ends increased, shear force-angle curve also increased. It was also seen that the shear force-angle curves were wavy due to micro-slippage occurred yarn-to-yarn at the interlacement regions.
In Figures 5(a) and 4(b), the shear force-angle curves for shearing the weft by 1–5 pulled yarn ends in treated narrow and wide fabrics were shown, respectively. In Figures 5(c) and 4(d), the shear force-angle curves for shearing the warp by 1–5 pulled yarn ends in untreated narrow and wide fabrics were shown, respectively. It was observed that the shear force-angle curves and the number of pulled ends were slightly proportional. When the number of pulled ends increased, the shear force-angle curve also increased. It was also seen that the shear force-angle curves were wavy due to micro-slippage occurring yarn-to-yarn at the interlacement regions. In addition, fabric sample dimensions and chemical treatments affect the fabric shear obtained from the yarn pull-out method.
Effects of sample dimensions and the number of pull-out ends
The warp and weft shear force-angle results for various fabric length and widths, and the number of pull-out ends in untreated and treated fabrics are presented in Figures 6 and 7, respectively. Figure 8 also shows relationship between warp and weft shear force-angle and the number of pulled ends for various fabric width/length ratios in untreated and treated fabrics.
Relationship between shear force/angle and the number of pulled ends for various fabric lengths in untreated polyester satin fabric. a) Pulled direction: warp, b) Pulled direction: weft (fabric width: 30 cm). Relationship between shear force/angle and the number of pulled ends for various fabric widths in untreated polyester satin fabric. a) Pulled direction: warp, b) Pulled direction: weft (fabric length: 20 cm). Relationship between shear force/angle and the number of pulled ends for various fabric width/length ratios in untreated and softening agent treated polyester satin fabric. a) Pulled direction: warp, b) Pulled direction: weft.


Shear results of softening treated satin fabrics by pull-out test for various fabric dimensions to warp direction
Shear results of softening treated satin fabrics by pull-out test for various fabric dimensions to weft direction
As seen in Figure 8 and Tables 2–5, when the number of pull-out ends in untreated and treated fabric increased, the shear force-angle values generally increased in each fabric width/length ratio. In addition, when the fabric width/length ratios increased, the shear force-angle values slightly increased. On the other hand, the shear force-angle values in untreated fabric were high compared to that of treated fabric due to the effect of softening agent on the fabric structure.
Effects of pull-out end position
Shear force-angle values for various pull-out end positions in the fabric sample can be calculated by means of following relations.
If the various regional shear angles were θ1 ≠ θ2 ≠ θ3 ≠ ……≠ θ
n
, and applied forces on the pulled yarn distance in the fabric width were w1 ≠ w2 ≠ w3 ≠ ……≠ w
n
, and the generated shear displacements were d1 ≠ d2 ≠ d3 ≠ ……≠ d
n
, then the following relations can be proposed to calculate the regional shear force-angle values:
Figure 9 shows the schematic views of the tensile pull-out yarn end positions from different fabric regions. The shear force-angle curve for each region can be defined based on the data generated from the tensile testing instruments. From the data, regional shear rigidity can also be calculated. The regional shear force-angle and rigidity values in the woven fabric can be especially important, if the fabric is transformed into varying complex geometrical shapes where local fiber fraction and porosity in the fabric could be affected. More research efforts will be spent to define the fabric’s local shearing properties and these will be published separately.
Schematic view of pull-out yarn end positions from different regions of woven fabric during pull-out test to find fabric local shear (left) and top portion of various regional shear displacements and angles (right).
Shear rigidity results
Fabric shear rigidity on polyester fabrics was found to be based on the relationships defined in the analytical model sub-section of the text. The fabric shear rigidity results are presented in Tables 2–5. The shear rigidity results for various fabric length and widths and the number of pull-out ends in untreated polyester fabrics are presented in Figures 10 and 11, respectively. Figure 12 shows the relationship between shear rigidity and the number of pulled ends for various fabric width/length ratios in untreated and treated polyester plain fabrics.
Relationship between shear rigidity and the number of pulled ends for various fabric lengths in untreated polyester satin woven fabric. a) Pulled direction: warp, b) Pulled direction: weft, (fabric width: 30 cm). Relationship between shear rigidity and the number of pulled ends for various fabric widths in untreated polyester satin woven fabric. a) Pulled direction: warp, b) Pulled direction: weft, (fabric length: 20 cm). Relationship between shear rigidity and the number of pulled ends for various fabric width/length ratios in untreated and softening agent treated polyester satin fabric. a) Pulled direction: warp, b) Pulled direction: weft.


As seen in Figures 10–11 and Tables 2 and 3, when the number of pull-out ends in untreated fabrics increased, the shear rigidity values increased in each of the fabric length. Generally, long fabric showed slightly high shear rigidity compared to that of the short fabric. On the other hand, when the number of pull-out ends in untreated fabrics increased, the shear rigidity values increased in each of the fabric widths. However, no significant differences were found between wide and narrow fabric with regard to shear rigidity values.
As seen in Figure 12, when the number of pull-out ends in untreated and treated fabrics increased, the shear rigidity values increased in each of the fabric width/length ratios. In addition, when the fabric width/length ratios increased, the shear rigidity values decreased in each of the pull-out ends. This indicated that fabric sample dimension and the number of pulled ends greatly influenced the fabric shear rigidity. On the other hand, the shear rigidity values in untreated fabric were high compared to that of treated fabric due to the effect of softening agent on the fabric structure.
Specific shear rigidity in untreated and treated fabrics was calculated based on the relationships defined in the analytical model sub-section of the text. The fabric specific shear rigidity results are presented in Figure 13. As seen in Figure 13, when the number of pull-out ends increased, the specific shear rigidity values generally increased. On the other hand, the specific warp shear rigidity of untreated fabric was higher than that of treated fabric. However, the specific weft shear rigidity of treated fabric was higher than that of untreated fabric.
Relationship between specific shear rigidity and the number of pulled ends for various fabric width/length ratios in untreated and softening agent treated polyester satin fabric. a) Pulled direction: warp, b) Pulled direction: weft (fabric width: 30 cm, fabric length: 10 cm, fabric width/length ratio: 3/1).
Shear jamming results
The warp and weft shear jamming results for various fabric widths and lengths, and the shear angle values in untreated and treated fabrics are presented in Figure 14. As seen in Figure 14, the warp shear jamming angle ranged from 2.54° to 17.74° for untreated fabric and 2.30° to 37.34° for treated fabric, in narrow fabric samples for various fabric lengths, whereas the shear jamming angle ranged from 1.93° to 15.20° for untreated fabric and 0.41° to 12.32° for treated fabric, in wide fabric samples for various fabric lengths. The weft shear jamming angle ranged from 2.42° to 17.97° for untreated fabric and 2.94° to 17.97° for treated fabric, in narrow fabric samples for various fabric lengths, whereas the weft shear jamming angle ranged from 1.55° to 13.90° for untreated fabric and 1.93° to 13.17° for treated fabric, in wide fabric samples for various fabric lengths. The difference between warp shear jamming angles was around 15.20° for untreated fabric and 35.04° for treated fabric, in narrow fabric sample for various fabric lengths, whereas the difference between shear jamming angles was around 13.27° for untreated fabric and 11.91° for treated fabric, in wide fabric sample for various fabric lengths. The difference between weft shear jamming angles was around 15.55° for untreated fabric and 15.03° for treated fabric, in narrow fabric sample for various fabric lengths, whereas the difference between shear jamming angles was around 12.35° for untreated fabric and 11.24° for treated fabric, in wide fabric sample for various fabric lengths. On the other hand, the maximum warp and weft shear angle value for untreated and treated fabrics in narrow fabric for various fabric lengths was high compared to that in wide fabrics.
Shear angle jamming for various fabric widths and lengths in untreated and softening agent treated polyester satin fabrics. a) Pulled direction: warp, b) Pulled direction: weft.
Conclusions
Polyester satin fabrics were tested to define fabric shear by the pull-out method and analytical relations were developed to calculate the fabric shear strength and shear rigidity.
Shear strength increased when the fabric width and length, and the number of pulled ends increased. It was found that the weft shear force-angle values were higher than the warp shear force-angle values. On the other hand, when the number of pull-out ends and fabric width, and length increased, the shear rigidity values generally increased. Also, the shear rigidity values in untreated fabric were high compared to that of treated fabric due to the effect of softening agent on the fabric structure. Hence, it was realized that fabric sample dimensions and fabric treatments as well as the number of pull-out ends influenced fabric shear strength and rigidity.
Shear jamming angles were found to be based on the number of pulled ends. The maximum and minimum shear angles in untreated and treated fabrics were generated by five ends and one end, respectively. On the other hand, fabric local shearing properties could be identified by pulling the yarn ends in various regions of the fabric which was especially important for fabric handling during formation. The results generated from this study showed that fabric shear could be measured by the yarn pull-out test.
Footnotes
Acknowledgements
The author thanks the Research Associate Mahmut Korkmaz for some testing and Miss Gaye Yolacan for preparing the fabric samples and some art works. The author also thanks Mrs Turkay Bilisik for her encouragement and inspiration in this research project.
