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Optical-related properties and characterization of some textile fibers using near-infrared spectroscopy

  • Alsaid Ahmed Almetwally EMAIL logo and Heba M. Elfowaty
Published/Copyright: March 2, 2024

Abstract

When light falls on the fiber surface, it is absorbed, reflected, or refracted. These three phases of incident light determine, to a great extent, the behavior of lustre of major textile fibers. This article sheds light upon the behavior of some textile fibers, namely, polyethylene terephthalate, cotton, viscose, bamboo, tencel, and modal fibers, in terms of their reflectance percentages in the ultraviolet regions. Also, the direct and indirect band-gap energies of the used textile fibers were also investigated. The findings of this study revealed the significant differences among these used textile fibers in relation to their optical properties. Also, the chemical composition of the used textile fibers was easily identified using near-infrared spectroscopy. Finally, the findings of this study revealed that the used textile fibers are considered good insulators.

1 Introduction

Nowadays, textile fibers are determined, identified, and characterized using four main methods: visual inspection, solubility testing, flame testing, and microscopy [1,2]. Visual inspection is considered a subjective method. In contrast, solubility and flame testing methods are destructive. Thus, microscopic examination of textile fibers became the simplest, most efficient, and most reliable testing method in many industries including chemical, plastics, polymer, agriculture, pharmaceutical, and textile industries [3]. The application of near-infrared (NIR) technology in the textile industry includes the determination and identification of fiber type and blend content, fiber maturity, micronaire value, size pick-up, moisture content, heat-set temperature, etc. [4,5,6].

When diffuse NIR reflectance spectroscopy was combined with the soft independent modeling of class analogy (SIMCA) method, it was discovered to be an efficient, quick, multivariate, and non-destructive method for classifying various textile fibers. This promising technique does not require any sample pretreatment and settings on the manufacturing process, fiber origin, dye pattern, or dye content [3]. Jinfeng et al. [7] integrated the NIR spectra with pattern recognition approache that include principal component analysis (PCA), linear discrimination analysis (LDA), and SIMCA to characterize and identify polypropylene and polylactic acid, wool, and cashmere fibers.

Yongliang et al. [8] investigated the relationship between NIR spectra and micronaire values, which were measured using high volume instrument (HVI) from a total of 381 cotton samples that were harvested from crops in 2011 and 2012. Their results disclosed that the difference between micronaire values measured and predicated using HVI and NIR, respectively, was accepted to a great extent. Therefore, they stated that the development of an effective and robust NIR model can be used to rapidly assess the micronaire values of cotton fibers. It was also reported that linen content in linen/viscose blended yarn was measured conveniently using NIR spectroscopy [9]. Thomasson et al. [10] used an FTIR instrument to characterize cotton fiber quality, including its micronaire value. At fixed polarization, they discovered that the different wavelengths of the laser caused a slight variation in the scatted light among the cotton samples. By contrast, with a fixed wavelength and varying polarization, a notable variation was detected, assuring that the polarization can be used to differentiate among cotton fiber samples.

It should be noted that the characteristics of textile fibers, especially cotton and polyester, and their blends in the form of spun yarns or knitted fabrics were researched in various studies [11,12,13,14,15,16,17,18].

This article aims to identify and characterize some cellulose textile fibers such as viscose, bamboo, tencel, and modal fiber in comparison with Egyptian cotton and PET fibers using NIR analysis. Also, the direct and indirect band energies of these fibers were compared.

2 Experimental

2.1 Materials

Throughout this study, six different kinds of textile fibers were used. Of these, four types are regenerated cellulosic fibers, namely viscose, bamboo, tencel, and modal fibers. The rest are Egyptian cotton of type Giza 86 and polyethylene terephthalate (PET) textile fibers. The longitudinal and cross-sectional views of the textile fibers are shown in Figures 1 and 2, respectively. Also, the particulars of the Egyptian cotton fibers (Giza 86) are listed in Table 1, and the dimensions of the remaining used fibers are tabulated in Table 2.

Figure 1 
                  Longitudinal views of the used textile fibers.
Figure 1

Longitudinal views of the used textile fibers.

Figure 2 
                  Cross-sectional views of the used textile fibers.
Figure 2

Cross-sectional views of the used textile fibers.

Table 1

Particulars of the Egyptian cotton (Giza 86)

Value
Upper half mean length 33.8 mm
Length uniformity 87.1%
Short fiber content 5.6%
Tenacity 45.3 g/tex
Micronaire value 4.31 (µg/in.)
Spinning consistency 206
Maturity ratio 82%
Table 2

Dimensions of textile fibers used in this study

Dimensions Types of textile fibers
Cotton Polyester Viscose Bamboo Tencel Modal
Diameter (µm) 14.6 11.6 10.3 12.5 10.2 10.8
Perimeter (μm) 45.9 36.5 32.4 39.3 32.1 33.9
Area (μm2) 118.5 122.7 101 86.3 97.1 75.4
Mean length (mm) 33.8 38 38 38 39 38
Linear density (denier/dtex) 2.3/2.6 1.5/1.6 1.2/1.3 1.7/1.9 1.1/1.3 1.3/1.4

Since the fibers investigated in this study are mainly cellulose and PET fibers, it should be noted that cellulose fibers (cotton, viscose, bamboo, tencel, and modal) are essentially made up of cellulose and have C–C, C–H, and O–H groups. These cellulose fibers differ from each other in terms of the percentage content of alpha-cellulose, hemicellulose, pectin, lignin, ash, etc. PET fiber contains both ester bonds (CO–O) and C–H. The chemical compositions of cellulose fibers in terms of cellulose, hemicellulose, pectin, lignin, and PET fiber are illustrated in Figure 3.

Figure 3 
                  Chemical compositions of cellulose and PET fibers.
Figure 3

Chemical compositions of cellulose and PET fibers.

2.2 Methods

First, all types of textile fibers under study were processed on a carding machine to convert them into a form of carded sliver. From each fiber type, a carded sliver of count 0.12 Ne with a weight of 4.9 g/m was produced. All carded slivers were placed in a standard environment, i.e., temperature of 20 ± 2°C and relative humidity of 65 ± 2% for a full day.

From each fiber type, 0.54 g was taken and pressed using a hydraulic press under a pressure of approximately 127 MPa in the form of a circular disc of 0.2 cm thickness and 1.5 cm diameter and then mounted in the sample holder of the measuring instrument.

It was reported that the best tool for evaluating the optical characteristics of textile fibers is ultraviolet–visible (UV-VIS) diffuse reflectance spectroscopy [19]. In order to acquire the NIR reflectance spectra of the textile fibers under study, a spectrometer of type JASCO V-770 (Jasco Co., Japan) was used. The spectra were collected using wavelength ranges between 190 and 2,500 nm with a specified resolution of 0.5 nm and 32 scans. For each fiber sample, three spectra were obtained, and their average was calculated. It should be noted that the used range wavelength covers UV–VIS–NIR bands.

Two types of reflection occur when electromagnetic radiation is directed onto the surface of a solid powder: specular reflection and diffuse reflection (DR). The specular reflection is direct radiation from the powder sample surface, and according to Snell’s reflective law, the angles of incidence and reflection are equal. DR is the radiation that penetrates the powder sample and scatters (after several reflections, refractions, and diffractions in all directions due to nanostructured mass) as well as wavelength-dependent absorption within the nanomaterial.

The standard approach for determining the optical characteristics of powder is to use a UV–Vis spectrophotometer to detect DR [20,21].

Tauc et al. [22] calculated the band-gap energy of amorphous semiconductors using optical absorption spectra in 1966. Later on, Davis and Mott developed Tauc’s proposal further [23,24]. The Tauc technique is dependent on the presumption that the absorption coefficient, α, based on the band-gap energy, can be expressed as follows:

(1) ( α × h ν ) = B ( h ν E g ) m ,

where ν is the frequency of the photon, h is the Plank’s constant, E g is the energy of the band-gap, and B is the constant. The m factor is 1/2 or 2 for direct and indirect transition band-gaps, respectively, depending on the nature of the electron transition [25]. Diffuse reflectance spectra are commonly used to calculate the band-gap energy. The observed reflectance spectra can be transformed to matching absorption spectra using the following Kubelka–Munk function, which was presented in 1931 [26]:

(2) F ( R relative ) = K S = ( 1 R ) 2 2 R .

The ratio of the sample-measured reflectance (R sample) to the measurement from a highly reflecting material (R standard, with reflectance approximately 100%) is used to calculate relative reflectance (R relative).

Here, R relative = R sample R standard , and K and S, respectively, are absorption and scattering coefficients [27]. In equation (1), by substituting F(R relative) instead of α, the following (equation (3)) was obtained:

(3) ( F ( R relative ) × h ν ) = B ( h ν E g ) m .

The energy band-gap is easily derived by plotting () against both (αhν)1/2 and (αhν)2.

3 Results and discussion

3.1 Reflectance values

When a light beam falls on a fiber surface, it is reflected, refracted, or absorbed, and the sum of their indices is equal to one. Reflectance values of the used raw fibers were measured using a NIR spectrometer in the UV–VIS and NIR regions. In the visible region, the reflectance spectrum uniquely describes the color of objects that are perceived by the human eyes.

Figure 4 shows the reflectance values of the used textile fibers in the UV–VIS region. It was detected that the percentage reflectance is gradually increasing until it reaches 85% at a wavelength of 400 nm for all textile fibers except for cotton fibers whose reflectance value reaches 50% at the same wavelength. Thereafter, the reflectance reaches a plateau at 90% reflectance starting from the wavelength of 400 nm, while cotton fiber is still increasing steadily until it reaches 80% at a wavelength of 880 nm. In the UV light (wavelength is less than 400 nm), the difference between cotton fibers and their counterparts of the remaining textile fibers in terms of their reflectance value is more pronounced. In the visible region, it can be concluded from Figure 4 that viscose fiber is associated with a high reflectance value, followed by bamboo, modal, and tencel fibers, respectively. In contrast, polyester and Egyptian cotton fibers have the lowest percentage of reflectance values. In the range of wavelength of 400–700, the reflectance spectra of all fibers except for cotton are overlapped, while the reflectance spectrum of cotton fiber was overlapped with bamboo and tencel fibers in the range of 900–1,000.

Figure 4 
                  The percentage reflectance of the used textile fibers in the UV–VIS region.
Figure 4

The percentage reflectance of the used textile fibers in the UV–VIS region.

Due to its significant superiority, NIR spectroscopy can be used to characterize, identify, and classify different textile fibers. Using the relationship between the vibrations of the characteristic groups and the corresponding wavelengths, quick identification and classification of the used textile fibers can be realized.

The NIR region starts from 900 to 2,500 nm, which has an overtone of stretching and vibrational modes of mid-infrared MIR, in which the FTIR measurement takes place. Figure 5 shows the NIR spectra of the used textile fibers. From this figure, it can be seen that the greatest variation was detected in the regions of 1,200–1,600 and 1,900–250 nm, respectively. The main bands are located at wavelengths of 1,460, 1,920, 2,100, 2,270, and 2,350 nm. The band located at a wavelength of 1,200 nm is associated with the second overtone of C–H stretching vibrations with a methyl group in cellulose. In contrast, the first overtone of O–H stretching vibration is the cause of the broadband located at a wavelength of 1,460 nm. The sharp band assigned at a wavelength of 1,924 nm is due to O–H asymmetric stretching and O–H deformation from free-absorbed water. The band located at a wavelength of 2,110 nm is due to the combination of O–H stretching and O–H deformation, which corroborates that all O–H groups are involved in hydrogen bridges. Both bands at 2,270 and 2,350 nm are from polysaccharides or cellulose derivatives [28,29,30,31].

Figure 5 
                  NIR spectra of the used textile fibers.
Figure 5

NIR spectra of the used textile fibers.

3.2 Absorbance

The average absorbance values of the used textile fibers versus the wavenumber are depicted in Figure 6. From this figure, it can be noticed that at the bands of 8,200 up to 4,000 cm−1, there exist identical wave fluctuations and spectra peaks for the used textile fibers. This means that most textile fibers, except for the PET fiber, have similar chemical structures. Differences in absorption intensity are linked to the molecular composition or found chemical groups, which can be used to further determine the blending ratios among these textile fibers. The used textile fibers also displayed a different variation trend of absorbance in the spectral range over 12,500 cm−1, which can be ascribed to their color differences. This result agrees with previous findings [32,33].

Figure 6 
                  Absorbance spectra of the used textile fibers.
Figure 6

Absorbance spectra of the used textile fibers.

3.3 Band-gap energy

The values of the direct and indirect band-gap energies of the used textile fibers are depicted in Figures 7 and 8, respectively. In these figures, the values of were plotted against both (αhν)2 and (αhν)1/2. Generally, the extrapolation of the tangent of the straight line segment of each (αhν)2 and (αhν)1/2 against at ordinate is equal to zero and can be used to determine the direct and indirect band-gap energies, respectively.

Figure 7 
                  Direct band-gap energy values of the used textile fibers.
Figure 7

Direct band-gap energy values of the used textile fibers.

Figure 8 
                  Indirect band-gap energy values of the used textile fibers.
Figure 8

Indirect band-gap energy values of the used textile fibers.

From Figure 7, it can be seen that the direct band-gap energies of the used textile fibers ranged between 5.31 and 5.43 eV, which means that these textile fibers are good insulators. It can also be seen that polyester fibers have the highest value of the direct band-gap energy; and cotton fiber has the lowest value. The values of the direct band-gap energies of the used textile fibers can be arranged in descending order from a high value to a low value of the direct band-gap energies as follows: polyester (5.43 eV) > viscose (5.4 eV) > modal (5.37 eV) > bamboo (5.35 eV) > tencel (5.33 eV) > cotton (5.31 eV).

The indirect band-gap energies of the used textile fibers are obtained by plotting () against (αhν)1/2 and are depicted in Figure 8. The extrapolation of the linear portion of each curve till its intersection with the x-axis, , will be used to estimate the value of the indirect band-gap energy. From these figures, it can be noted that the indirect band-gap energies of the textile fibers under study ranged between 3.52 and 4.04 eV. It was found that polyester and cotton fibers have high and low indirect band-gap energies, respectively. The values of the indirect band-gap energies of these textile fibers can be arranged from the high value to low one as follows: polyester (4.04 eV) > bamboo (3.86 eV) > viscose (3.68 eV) > modal (3.66 eV) > tencel (3.64 eV) > cotton (3.52 eV). It is surprising to note for all textile fibers that the direct band-gap energy is higher than the indirect band-gap energy.

4 Conclusion

The present study focuses on the characterization of six textile fibers of which one natural cellulose fiber, namely Egyptian cotton, and four regenerated cellulose (viscose, bamboo, Tencel, and modal) and PET fibers. The characterization and determination were conducted using UV–NIR spectroscopy, which proved its usefulness and efficiency. The direct and indirect band-gap energy of each fiber type was also estimated using the Munk–Kubelka equation. The findings of this study revealed that in the visible region, these textile fibers differ significantly in their reflectance and absorbance values. It was also estimated that the direct band-gap energy of the fibers was more than 3 eV, which means that these textile fibers are good insulators.

  1. Funding information: This article is based upon work supported by the Science, Technology & Innovation Funding Authority (STIFA) under grant number 43342.

  2. Conflict of interest: Authors state no conflict of interest.

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Received: 2022-02-16
Revised: 2022-07-14
Accepted: 2023-12-13
Published Online: 2024-03-02

© 2024 by the authors, published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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