Open Access Article
Denis V.
Okhrimenko
a,
Marcel
Ceccato
b,
Sven
Tougaard
c,
Morten
Foss
b,
Eric
Pezennec
d and
Mette
Solvang
a
aROCKWOOL A/S, Denmark
bInterdisciplinary Nanoscience Center (iNANO), Aarhus University, Denmark
cUniversity of Southern Denmark, Denmark
dKnauf Insulation, Belgium
First published on 2nd June 2023
The article mentioned in the title of this comment paper reports on an investigation of the organic binder presence and distribution on stone wool fibres with surface sensitive techniques (X-ray photoelectron spectroscopy (XPS), QUASES XPS modelling, time-of-flight secondary ion mass spectrometry (ToF-SIMS) mapping) and attempts to correlate the results with fibre performance in in vitro acellular biosolubility tests. However, the study has assumptions, hypothesis and results that do not take into account the recognised science and regulations on biopersistence of stone wool fibres, limitations of the utilized surface sensitive techniques and modelling approach and it contains a contradiction with biosolubility experiments. In this comment article, we discuss these points, propose improved QUASES XPS modelling and present recent ToF-SIMS mapping results that reflect biosolubility behaviour of the stone wool fibres.
2 and Sauer et al., 2021.3 The starting point for their publications is the authors' view that hazard assessment of man-made vitreous fibres (MMVF) is solely based on biodurability measurements of naked fibres (i.e. without binder). Similar to the previous discussion,4 we would like to bring attention to the fact that in vitro acellular biodurability tests either on fibres with or without binder are not relevant for the hazard assessment and regulations on mineral wool fibres. Actually, MMVF hazard assessment includes investigation of fibre biopersistence via in vivo animal studies with typically nasal inhalation or intratracheal installations of fibres produced without binder5,6 (Note Q of the European Regulation (EC) No. 1272/2008 (CLP) (EC2008)) and epidemiological studies on workers, where the impact of fibres produced with binder is studied, both recognised at international and European level.7–13 Despite this, the papers1–3 attempted to find differences in the in vitro acellular behaviour of fibres with and without binder, using binder removal techniques that modify fibre chemistry,14,15 wettability and thus likely solubility.16,17 The paper1 explored the distribution of binder (presumably phenol-urea-formaldehyde, PUF) on stone wool fibres and tried to find a correlation between dissolution rate of stone wool measured in a simulated lung fluid (phagolysosomal simulant fluid, PSF) and the amount and thickness of organic material on the fibre surface. The article1 reports the use of surface sensitive techniques, such as X-ray photoelectron spectroscopy (XPS), time-of-flight secondary ion mass spectroscopy (ToF-SIMS) mapping and modelled XPS data with QUASES software.18 The general findings of the paper about organic matter obtained with XPS and QUASES XPS modelling are in line with previously published results on stone wool samples.19,20 However, we would like to stress several points concerning the assumptions and hypotheses in the publication,1 analytical techniques limitations in spatial resolutions and interpretation of results and as well present the newest results using QUASES XPS and ToF-SIMS on stone wool samples with PUF binder.
The authors1 state that they expect phenolic resin to be commonly used as a binder based on their finding of traces of nitrogen but no further information on the organic binder chemical composition is provided. In the paper the binder appears to be treated as a classic organic molecule without further differentiation of other binder components (such as oil, coupling agent etc.). We further note that providing SEM images (a standard technique for the study of microstructure on fibre surfaces) of the stone wool fibres would have been beneficial and would have enabled the distinction between micrometre size areas with binder and the rest of the surface.
23 (F3 sample, 3.6 wt% PUF binder, 0.1 wt% mineral oil) performed with the same ToF-SIMS settings as in Okhrimenko et al., 2022.16 The signal from fibre substrate (Al+, Fig. 1a, a1) is dominating over the signal from organic layer originated likely from PUF binder (C7H7+) and oil (C3H7+) in many areas on the fibre surface (Fig. 1b, b1, c and c1), indicating that PUF binder and mineral oil coverage is neither uniform nor complete.
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| Fig. 1 ToF-SIMS imaging results of F3 stone wool fibres (3.6 wt% PUF binder, 0.1 wt% mineral oil) from Barly et al., 2019:23 (a-a1) Al+; (b-b1) overlay of Al+ (red) and C7H7+ (green); (c-c1) overlay of Al+ (red) and C3H7+ (green) and (d-d1) overlay Al+ (red) and total intensity (green). The images (a–d) are obtained with Bi1+ ion source and other settings similar to those in Okhrimenko et al., 2022.16 The images (a1–d1) are obtained with Bi3++ ion source similar to Hirth et al., 2021.1 | ||
It is important to consider the influence of the ToF-SIMS mapping spatial resolution and other settings on the conclusions about binder distribution on the fibres. This would help to understand why fibres with different binders (PUF and SBB) and fibres without any binder perform similar in dissolution tests as found in.16,23 We also note that the journal number and year for the work by Barly et al., 2019
23 in the Notes and references of Hirth et al., 2021
1 are not correct.
For the XPS results, no survey (wide-scan) spectra of the studied stone wool samples are presented. This does not allow to check the presence of additional chemical elements in the different stone wool samples that were compared. Complete survey spectra would have enabled the authors and the readers to get a first qualitative view of comparison between the samples. Moreover, it would be beneficial for the readers if it was acknowledged that both methods, XPS and ToF-SIMS, are extremely sensitive towards contaminations by adventitious carbon, which can originate from fibre storage and handling, as well as from apparatus in situ, and interfere with the performed analysis, reducing its representativity.
QUASES XPS modelling works the best if reference spectra are available, i.e. in this case this would be a spectrum of “naked” fibres without organic matter on their surface. In the absence of reference spectra, several models describing experimental XPS spectra are possible. The authors1 chose to simulate the surface layer in a similar way as in the study by Okhrimenko et al., 2018,20i.e. as a uniform carbon layer with thickness 1–3 nm on top of the fibres. While the approach of using the background of the Si and Al XPS peaks to determine the binder distribution can be relevant at the considered thicknesses (≤10 nm), we note that binder droplets can be thicker (30–50 nm) and they are “blind” spots for QUASES analysis.
With QUASES software version 7.5, the results from Okhrimenko et al., 2018
20 can be re-evaluated using the automation option. QUASES v.7.5 uses the simplex method to determine the combination of all structure parameters which gives the minimum root mean square, RMS, between the spectrum and the background in the desired energy range. Using the automated structure determination facility that varies the structure until the RMS deviation in the 1270 to 1310 eV energy range reaches a minimum, we observed an improved fit of the XPS spectra when the software applies the model where 20% of the fibre surface remained uncoated (Fig. 2a, RMS 8.3 × 10−4), compared to the previous fitting with a 4 nm thick uniform layer presented in Okhrimenko et al., 2018
20 (Fig. 2b, RMS 20.3 × 10−4). This reduction in RMS is substantial but it should also be supplemented by a visual inspection of the spectra: the fit in Fig. 2a is seen to be virtually perfect in the full energy range from 1270 to 1295 eV, whereas there are clear deviations in Fig. 2b in this energy range. Any other structural model also gives substantially worse fits to the background.
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| Fig. 2 XPS spectra QUASES fitting using model: (a) with 80% of the surface covered with 7.1 nm organic layer and 20% of the uncoated surface; (b) uniform organic layer of 4.0 nm thick (Okhrimenko et al., 2018).20 | ||
Presence of the organics-free areas correlates with ToF-SIMS mapping results presented in our work for PUF treated fibres and by Okhrimenko et al., 2022
16 for SBB treated fibres and also with the similar dissolution behaviour of the fibre material irrespective if binder was applied or not23 and which type of the binder was applied.16 To sum up, the realization in the paper1 analyses without reference to neither the substrate nor the binders and without proof of the goodness of the modelling (only one example provided with narrow energy range, 1225–1345 eV) and the fact that their XPS spectrum was recorded with a rather low signal to noise level does not allow to ensure the solidity of the results and the findings. In addition, we note that information about how the general background is accounted for in the analysed energy region would have been very helpful. In QUASES XPS this is done by subtracting a straight which is fitted to the spectrum on the high energy side of the region. However, if peaks are present in this region (which is clearly the case here as seen in Fig. 2), the slope of this line can be uncertain and this adds to the uncertainty of the analysis. We avoid this problem by including in the analysis all peaks on the high energy side in the full energy range.
The observed fibre (with binder) dissolution can be explained by the fact that the organic layer on the fibre surface is incomplete and inhomogeneous in reality and leaves bare surface available for dissolution, as we have just shown with the newest QUASES XPS modelling and ToF-SIMS results presented here for PUF- and recently for SBB-treated fibers.16
Therefore, Hirth et al., 2021
1 results confirmed that binder presence cannot affect the dissolution of the stone wool fibres. It was shown that it is the inorganic chemical composition of the fibre that is among of the prime factors in in vivo pathogenicity5,6 and for in vitro cellular24,25 and acellular26–28 dissolution rates. Besides that, experimental conditions16,28–30 (e.g. fluid flow rate to sample surface area ratio, fluid composition, temperature, pH, dynamic or batch experiment and sample preparation) are crucial for the determination of the dissolution rates in in vitro acellular studies.
1 are in contrast with the existing science and regulations on biopersistence of stone wool fibres and other MMVF fibres. The present authors hope that provided comments, the additional examples of QUASES XPS modelling approach and application of ToF-SIMS mapping technique would support a better understanding of the biosolubility of the stone wool fibres, accepted terminology and existing regulations on MMVF biopersistence.
Footnote |
| † Personal Communication 2019, F. Schulz, Fraunhofer Institute for Toxicology and Experimental Medicine ITEM Hannover, Germany. |
| This journal is © The Royal Society of Chemistry 2023 |