Özge
Edebali
a,
Anna
Goellner
b,
Marek
Stiborek
a,
Zdeněk
Šimek
a,
Melis
Muz
b,
Branislav
Vrana
a and
Lisa
Melymuk
*a
aRECETOX, Faculty of Science, Masaryk University, Kotlarska 2, 61137 Brno, Czech Republic. E-mail: lisa.melymuk@recetox.muni.cz
bUFZ Helmholtz Centre for Environmental Research, Department of Exposure Science, Permoserstr. 15, 04318 Leipzig, Germany
First published on 24th March 2025
Textiles play an important role in the accumulation of harmful chemicals and can serve as a secondary source of chemical pollutants in indoor environments, releasing these chemicals back into indoor air, as well as a vector from which indoor pollution can be released by laundering to wastewater systems. Among harmful indoor pollutants, aromatic amines (AAs) are particularly concerning due to their mutagenic and carcinogenic properties, but have received limited attention in non-occupational indoor environments. We have characterized the distribution of 19 AAs between cotton, wool, and polyester textiles and air. Chamber exposure experiments were conducted under controlled laboratory conditions to quantify textile–air distributions of AAs and identify key parameters impacting the distribution. The mass-normalized textile/air distribution coefficients (KTA) of AAs for polyester, cotton, and wool range from 5.28 to 9.52 log units (L kg−1). The findings suggest that cotton generally exhibits higher distribution coefficients than polyester and wool for most analytes. Overall, the results show a strong positive relationship between octanol–air distribution coefficients (KOA) and KTA values. The consistent uptake capacity of all tested textiles for AAs highlights the potential for textiles to play a key role in AA indoor distributions.
Environmental significanceAromatic amines (AAs) are chemicals of concern due to their mutagenic and carcinogenic properties. Understanding their sources is essential to reduce environmental levels. Textiles play a key role in indoor environments as they can act as sinks for semi-volatile compounds and a transport medium to outdoors via laundering. We quantify the distribution coefficients of AAs between different types of textiles and air, which can help understand the importance of textiles in human exposure to AAs and in their transport from indoor to outdoor environments. |
Textile structure and chemical properties influence their sorptive capacities.5,6 Textile fibres can be classified as natural (e.g., cotton and wool), semisynthetic (e.g., rayon), and synthetic (e.g., polyester) materials. Cotton and wool fibres have large, irregular surfaces and a porous structure. Synthetic fibres like polyester have smoother, more uniform surfaces.4 The sorption behaviour varies with fabric type, with natural fibres generally having a higher affinity for polar semi-volatile organic compounds than nonpolar synthetic fibres.6,7 For example, natural textiles absorb more cigarette smoke and gain significantly more weight than synthetic materials like polyester primarily due to the particulates in the smoke.8,9 Noble5 measured the change in textile weight during exposure to cigarette smoke, finding the greatest weight gain for rayon, linen, wool, and cotton, while polyester gained the least. Cotton, for example, absorbed about ten times more smoke than polyester. Smoke absorption and moisture regain are correlated, with fabrics that absorb more moisture also tending to absorb more smoke.5 Differences in the surface area-normalized sorption of polybrominated diphenyl ethers to cotton and polyester were attributed to both micro-surface differences in textile properties and differences in chemical affinity due to textile compositions.10
Textiles have been shown to be key matrices impacting secondary emissions of chemicals back to the indoor environment, as well as vectors through which chemicals can be transferred to outdoor environments.11 For example, nicotine, a major alkaloid in tobacco smoke, rapidly sorbs to surfaces, including clothing, skin, and hair, contributing to third-hand smoke exposure.12 Won et al.2 found that carpets can absorb and gradually re-emit volatile organic compounds, thereby changing peak indoor air concentrations.
Moreover, recent attention has been given to the transfer of chemicals from indoor environments to outdoor surface waters via wastewater discharges13 and washing of textiles is a key component of this transfer. Saini et al.4 investigated the transfer of phthalates, brominated flame retardants, and organophosphate esters from indoor air to cotton and polyester and subsequent release to water during washing, identifying the importance of laundry discharges in transferring plastic additives from indoor to outdoor environments.
Aromatic amines (AAs) are a broad compound group known to be hazardous to human health and the environment, but in indoor environments largely associated with occupational exposure.14 They are used in rubber, azo dyes, pesticides, plastics, pharmaceuticals, cosmetics, and textiles, and can be produced in cigarette smoke and by high-temperature cooking of protein-rich foods such as meats and fish.15–17 Certain AAs are classified as carcinogens or potential carcinogens for humans18 and are contributors to both acute toxicity19,20 and mutagenicity in surface waters.21 There is growing awareness of the potential for these chemicals to be important indoor contaminants in non-industrial indoor environments, including in homes.14,22 AAs can accumulate in textiles through direct contact with indoor sources such as tobacco smoke, cooking, foods, and hair dyes,14 as well as through deposition of airborne particles, dust, or contaminated air. Given the importance of indoor textiles in the uptake and release of chemicals from tobacco smoke, which includes AAs, we hypothesize that indoor textiles can play an important role in the distribution of AAs in indoor environments, as well as their release to outdoor environments via laundry wastewater. However, little is known about the sorptive behaviour of AAs to textiles, which is necessary to understand their role in the accumulation and retention of these compounds.
This study investigates the sorptive distribution of AAs between three textiles (wool, cotton, and polyester) and air, providing insights into their indoor fate. To determine the distributions of AAs between textiles and air, we designed a chamber exposure study using primary AAs and three types of textiles. Initial laboratory work focused on developing techniques for dosing and extraction of AAs to textiles. Subsequent laboratory exposure experiments were conducted to determine the textile–air distribution coefficients (KTA) of AAs.
The experimental apparatus consisted of a textile exposure chamber consisting of a three-litre glass cylinder with a flat bottom and a ground-joint flange lid (Fig. 1). The exposure chamber was designed with a threaded air inlet in the lid, implemented as a steel capillary pierced through a septum, and an air outlet at the bottom. The chamber operated in a flow-through setup, meaning it was not a closed system. We assumed that the dosing rate of the textile (in terms of air volume equivalent per unit of time) was significantly higher than the airflow rate. Consequently, the chamber conditions were maintained close to a textile/air distribution equilibrium. A wire mesh sheet was rolled up inside the chamber, serving as a framework to support a piece of the tested textile. A small fan inside the chamber was used to homogenize the air inside the chamber and minimize the air boundary layer at the surface of the textile. The chamber was kept at a constant temperature of 25 °C through an external thermostatic water circuit.
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Fig. 1 Scheme of apparatus used for measurement of KTA of AAs; 1- textile pieces before wrapping to the chamber mesh (Fig S1†), 2- glass chamber with a ground joint lid, mesh and airtight seal, 3- steel capillary pierced through a septum for air intake, 4- metal clamp, 5- small fan, 6- two glass tubes filled with Tenax adsorbent, in series, 7- air mass flow meter, 8- low volume air pump. |
Two glass tubes packed with Tenax® TA (Gerstel, Germany) were connected in series to the chamber outlet to trap AAs from the air extracted from the exposure chamber. Air was drawn from the apparatus through the Tenax tubes using a low-volume air pump connected to a digital air mass flow controller (Omega FMA-A2404, USA) adjustable in the 0–200 standard cubic centimetres per minute (sccm) range.
Three types of textile materials were tested: wool, cotton, and polyester. All textiles were white/undyed materials; detailed information is provided in ESI Fig. S2, Text S1 and Table S1.† The purchased textile fabrics were cut into larger sheets (27 × 32 cm; area of 864 cm2 each), pre-cleaned (cleaned in water in overhead tumbler) and dried (Text S1 and Fig. S3†). Textiles were then dosed with a mixture of 19 primary AA compounds (Table S2†). The dosing procedure in a rotary evaporator was selected after testing different dosing methods to ensure homogeneously dosed textile samples (Text S2 and Fig. S4–S7†). The selected AAs were diluted in acetone by spiking 1 mL of AA standard (for the spiked masses of each analyte see Table S3†) in approximately 200 mL of acetone in a round rotary evaporator flask and mixed by shaking for 5 minutes. Next, the textile sheet was added to the acetone-filled flask. The textile samples were dosed for 6 hours while turning on a rotary evaporator (270 rpm, 25 °C at normal pressure). Subsequently, acetone was evaporated (556 mbar, 40 °C) while continuing the flask rotation, a process taking 1 hour to achieve complete dryness. After dosing, the textile samples were stored in the closed rotary evaporator flask at 4 °C until they were transferred to the exposure chamber.
Prepared textiles (27 × 32 cm) were dosed with AAs and pre-cut into 2 cm2 pieces to ease subsampling of textiles during the chamber experiments with limited disturbance to the experimental setup. Before placing the textile rectangles into the chamber, six subsamples of 2 cm2 were collected from each piece to assess the dosing homogeneity. Subsequently, the AA-dosed textile piece, wrapped around the wire mesh, was placed into a glass cylindrical chamber. The chamber was closed, and the experiments were initiated. Two durations of experiments were performed: 8-hour and 24-hour exposures. For the 24-hour experiments, triplicate data were collected over three days with a constant airflow of 67 sccm through the chamber. Similarly, the 8-hour experiment was conducted with a higher airflow of 200 sccm, keeping the total sampled air volume constant (96 L). The measurement of AA concentration in the freshly spiked textile samples versus textile samples exposed in the chamber confirmed that the sampling did not decrease the AA concentration in the textile by more than 1%. After each experiment, the air pump was stopped, and the Tenax tubes were transferred to separate vials and stored in the freezer for subsequent AA analysis. The chamber was opened, and nine 2 cm2 textile pieces were removed with tweezers, placed into vials and stored for AA analysis. This procedure was repeated for each textile type, with triplicate experiments conducted for both 24-hour and 8-hour durations.
An Agilent 6495A Triple Quadrupole Mass Spectrometer (Agilent Technologies, Santa Clara, CA) with a mass resolution of 0.7 amu (FWHM, autotune) and mass accuracy of 0.1 amu from 5 to 1000 m/z was used to quantify AAs. The ion source parameters were set as follows: gas temperature of 280 °C, gas flow at 15 L min−1, nebulizer pressure at 25 psi, sheath gas temperature at 380 °C, sheath gas flow at 12 L min−1, capillary voltage of 3000 V (positive mode), and nozzle voltage of 300 V. The instrument operated in ESI-positive dynamic multiple reaction monitoring (dMRM) mode. For MS/MS analysis, two transitions were monitored for each analyte. Collision energies for the [M + H]+ precursor ions of both target analytes and ISTDs are provided in Table S4.† Agilent MassHunter Workstation Software, LC/MS Data Acquisition (version B.08.00) for the 6400 Series Triple Quadrupole, was used for dMRM data acquisition, while AA quantification was performed using Agilent MassHunter Quantitative Analysis software, version B.07.01 for QQQ.
Surrogate standards d8-benzidine (Dr Ehrenstorfer™, LGC Group, USA) and d3-o-anisidine (A2S Analytical Standard Solutions, France), 100 ng per sample, were added to each sample before extraction to monitor the recoveries of AAs. Surrogate recoveries ranged from 65% to 87% for textile samples and from 81% to 118% for Tenax tubes (Tables S6 and S7†). Laboratory blanks (3 samples from each pre-cleaned textile material) were spiked with surrogate standards, and target AAs were below detection limits in all blanks.
Each textile subsample was weighed. The nine AA concentrations in textile subsamples were averaged for each replicated experiment. The textile/air distribution coefficient of each AA in each experiment, KTA (L kg−1), was calculated as the ratio:
![]() | (1) |
Uncertainties in KTA values were also estimated (Text S3†). Since only one Tenax sample was used per experiment, the uncertainty in the air concentrations was calculated by incorporating sources of uncertainty in the measurement: the error from the flow controller, repeatability of Tenax analysis, and extraction recoveries of AA from Tenax. For textiles, the standard deviation of the nine textile subsamples was taken to indicate uncertainty. Calculated KTA values were compared across replicates and exposure durations (one-way ANOVA test; α = 0.05) to determine if the differences in the mean KTA values were statistically significant.
We also evaluated literature values for volume normalized textile–air distribution coefficient (Kvol) in comparison with the logKOA–log
Kvol relationship we obtained, using cotton fabrics as a comparison as cotton had the best data availability. We calculated volume-normalized data from our mass-normalized distribution coefficients data (Table S8†). The volume-normalized cloth–air partition ratio, Kvol, was calculated as:
Kvol = KTA × ρT | (2) |
Compound name | Abbr | Log![]() |
Polyester log![]() |
Wool log![]() |
Cotton log![]() |
---|---|---|---|---|---|
a —: Indicates that air concentration data was unavailable, preventing the calculation of KTA values. b AAs were quantified in only 18 out of 36 samples; samples <LOQ were not considered in the calculation. | |||||
Aniline | ANI | 4.94 | 5.28 ± 0.21 | 5.46 ± 0.20 | 5.53 ± 0.12 |
2-Aminopyridine | 2APY | 5.68 | 6.07 ± 0.13 | 6.44 ± 0.19 | 6.81 ± 0.23 |
o-Toluidine | OTLD | 5.91 | 5.36 ± 0.20 | 5.50 ± 0.20 | 5.48 ± 0.17 |
o-Anisidine | OANI | 6.15 | 5.91 ± 0.32 | 6.03 ± 0.20 | 6.14 ± 0.15 |
4-Chloroaniline | 4CHA | 6.25 | 6.18 ± 0.16 | 6.31 ± 0.21 | 6.13 ± 0.13 |
p-Cresidine | PCRE | 7.28 | 6.45 ± 0.28 | 6.31 ± 0.19 | 6.47 ± 0.17 |
3-Chloro-o-Toluidine | 3CHOT | 7.46 | 5.94 ± 0.16 | 6.03 ± 0.18 | 6.02 ± 0.11 |
4-Chloro-o-Toluidine | 4CHOT | 7.48 | 6.25 ± 0.16 | 6.26 ± 0.20 | 6.19 ± 0.12 |
2-Amino-4-nitrotoluene | 2A4NT | 7.59 | 7.97 ± 0.15 | 7.81 ± 0.29 | 8.07 ± 0.16 |
Benzidine | BNZD | 8.35 | 8.16 ± 0.72 | 8.58 ± 0.40 | 9.29 ± 0.16 |
o-Aminoazotoluene | OAAT | 8.46 | 9.22 ± 0.20 | — | 9.55 ± 0.19b |
1-Naphthylamine | 1NAPA | 8.47 | 7.58 ± 0.30 | 7.28 ± 0.25 | 7.39 ± 0.20 |
2-Naphthylamine | 2NAPA | 8.47 | 7.45 ± 0.31 | 7.59 ± 0.27 | 7.67 ± 0.22 |
p-Aminoazobenzene | PAAZB | 8.70 | 8.85 ± 0.24 | — | — |
3,3′-Dichlorobenzidine | 33DCB | 9.11 | 7.81 ± 0.40 | 8.00 ± 0.38 | 8.31 ± 0.14 |
o-Dianisidine | ODAN | 9.11 | 7.50 ± 0.16 | — | 9.51 ± 0.10b |
4,4′-Methylenebis(2-chloroaniline) | MBOCA | 9.15 | 9.52 ± 0.29 | — | 9.65 ± 0.14b |
2-Aminobiphenyl | 2AMB | 9.27 | 6.72 ± 0.16 | 6.79 ± 0.19 | 6.84 ± 0.12 |
4-Aminobiphenyl | 4AMB | 9.27 | 8.17 ± 0.19 | 7.91 ± 0.29 | 8.25 ± 0.14 |
For polyester textiles, the ANOVA results (Table S9†) indicated no significant difference between the three replicates within 8-hour and 24-hour experiments. The airflow did not significantly affect the measured KTA, indicating that textile/air equilibrium was consistently achieved for all compounds under both 8- and 24-hour conditions, thereby confirming that the experimental setup provided sufficient time for equilibrium to be established regardless of the airflow rate. Consequently, the KTA data for polyester textiles were averaged (Fig. 2A) across all experiments. For cotton and wool textiles, the ANOVA results (Table S9†) showed a significant difference between the first replicate and subsequent replicates, but no significant difference between the second and third replicates. Therefore, the data for the 24-hour and 8-hour experiments were averaged for these textile types, excluding the first replicates (Fig. 2B, and C). We hypothesize that the chamber system had not achieved equilibrium at the time of collection of the first replicates for wool and cotton, which may have been due to some solvent (acetone) retention in cotton and wool. Both fabrics have higher capacities for retaining liquid and it is possible that some solvent from AA spiking was retained in the textile, and subsequently evaporated into the chamber air and disturbed the equilibrium conditions. As a result, the data from the first replicates for cotton and wool were excluded.
log![]() ![]() ![]() | (3) |
log![]() ![]() ![]() | (4) |
log![]() ![]() ![]() | (5) |
The correlations obtained for these empirical relationships suggest that they may be used to interpolate the prediction of textile–air distribution for other structurally similar compounds, e.g., other primary AAs based on regression eqn (3)–(5).
For compounds with logKOA above 8, cotton shows higher log
KTA values than wool or polyester, indicating a high capacity to sorb AAs. The higher sorptive capacity of cotton in comparison with the other two textile materials aligns with what has been noted by Borujeni et al.,8 who also identified that cotton had a high capacity to adsorb tobacco smoke compounds such as pyridine and nicotine, and those of Morrison et al.,3 who noted that cotton exhibited higher log
KTA for methamphetamine than polyester. Similar to our observations, Saini et al.4 found that cotton fabrics had higher partition coefficients than rayon for semi-volatile organic compounds (SVOCs), reinforcing the pattern that cotton consistently shows higher retention of chemicals across various studies. Fibres are often classified based on their origins into two main categories: natural fibres and synthetic fibres, which are derived from natural or synthetic polymers.25 Cotton, as a natural fibre, is hydrophilic due to its structure rich in hydroxyl groups that strongly attract and absorb water molecules.25,26 This high moisture absorbance increases cotton's ability to absorb airborne chemicals, especially polar molecules.12 The higher KTA observed for cotton textiles in our study, as well as in other studies, may be due to the hydrophilic nature of the textile fibres. In contrast, polyester is hydrophobic,27 with a smooth surface and a chemical structure that repels water, reducing its capacity to adsorb chemicals from the air. This limited adsorption might give polyester a lower capacity than cotton to interact with airborne chemicals. These contrasting properties are critical for understanding chemical interactions with textiles.
Further, even with the overall correlation with logKOA, individual AAs showed variations in log
KTA values across textiles, suggesting that the affinity of AAs can vary depending on the textile material-compound property combination. A few compounds had KTA values that were consistently more than one order of magnitude lower than the corresponding KOA. A notable example is 2AMB, with log
KTA values of ∼6.8 compared with log
KOA of 9.27; in contrast, 4AMB, which differs only in the position of the amino group, had log
KTA values of 7.9–8.2 (Table 1). This suggests weaker interactions of 2AMB with all textiles. 2AMB (ortho) and 4AMB (para) differ in chemical hydrogen bonding,28 and key structural characteristics that might influence their behaviour. In contrast, OAAT and MBOCA (for polyester and cotton) and BNZD (for cotton only) exhibited KTA values that were substantially higher than KOA (Table 1), indicating greater affinity for textiles than for pure organic matrices.
The literature has limited data on partitioning measurements between fabrics and air, making direct comparisons of the same compounds challenging. However, existing studies provide ranges for SVOCs such as novel flame retardants (NFRs) and phthalates, showing some consistency in partitioning behaviour across different compound groups. Other studies have linked fabric–air distribution to physical-chemical compound properties such as KOA, including for methamphetamine,3 PCBs,29,30 and phthalates.31,32 Morrison et al.32 also investigated textile–air partition coefficients for diethyl phthalate and di-n-butyl phthalate using a closed chamber experiment over 10 days. They observed that fabric–air partition coefficients of phthalates were strongly linked to KOA values, a trend also evident in our findings for AAs. Additionally, Saini et al.4,10 reported area normalized distribution coefficients for cotton and rayon fabrics for NFRs, PBDEs, and phthalates, showing that the distribution of chemicals was positively correlated with KOA, and consistent with the kinetic limitations of uptake.
The KTA values for AAs, phthalates,32 and PCBs30 showed strong positive relationships between logKOA–log
Kvol, as in our AA data (Fig. 4 and Table S10†). Variations in experimental design, including environmental conditions and fabric structure likely contribute to the differences in partition ratios and equilibration times observed in these studies. Additionally, differences in extraction methods may further contribute to these differences, even for the same chemicals.
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Fig. 4 Cotton textile Kvol for different compounds from literature; AAs (this study), PCBs [a],29 phthalates [b],32 phthalates [c],31 PCBs [d],30 methamphetamine [e].3 The regressions marked with an asterisk (*) indicate that at the 0.05 level, the slope is significantly different from zero. The statistical values for the linear regression analysis are provided in Table S10.† |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d5em00015g |
This journal is © The Royal Society of Chemistry 2025 |