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Comments on “Boron and lithium isotopic signatures of nanometer-sized smectite-rich mixed layers of bentonite beds from Campos Basin (Brazil)” by N. Clauer, L. B. Williams, and I. T. Uysal

Published online by Cambridge University Press:  01 January 2024

J. M. Wampler*
Affiliation:
Department of Geosciences, Georgia State University, P.O. Box 3965, Atlanta, GA 30302, USA
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Abstract

Type
Letter
Copyright
Copyright © The Author(s), under exclusive licence to The Clay Minerals Society 2022

To investigate the initial stages of illitization in marine bentonites, fine-clay subfractions of Santonian bentonite samples from the Campos Basin, offshore Brazil, were examined by X-ray diffraction, K-Ar, and Rb-Sr methods (Clauer et al., Reference Clauer, Środoń, Aubert, Uysal and Toulkeridis2020) and by chemical and isotopic analyses of B and Li (Clauer et al., Reference Clauer, Williams and Uysal2022). Only three subfractions of fine clay from each of two bentonite samples were available for the latter study, so the results were characterized as preliminary information “thought to be of help for future studies” (Clauer et al., Reference Clauer, Williams and Uysal2022, p. 73). A few substantial differences in boron content and isotopic composition among the six subfractions were found, but there was little variability in lithium content and isotopic composition. In the absence of information about B and Li in the bulk bentonites and their host rocks, and because of the presence of some detrital illite in one of the samples (sample A1, Clauer et al., Reference Clauer, Środoń, Aubert, Uysal and Toulkeridis2020), these B and Li analyses add little toward understanding the character of the fluid environments in which the original volcanic ash was transformed into the now-present smectite-rich interstratified illite-smectite (I-S). Nevertheless, in a rather long discussion of the results, Clauer et al. (Reference Clauer, Williams and Uysal2022) addressed many possibilities that could account for their observations, but they drew no clear conclusions about the origin of the illite beyond those drawn earlier by Clauer et al. (Reference Clauer, Środoń, Aubert, Uysal and Toulkeridis2020).

Critical evaluation of Clauer et al.’s (Reference Clauer, Williams and Uysal2022) isotopic study of B and Li is hindered by mistakes in the presentation of results and by inconsistencies between the text and the tabulated data (Online Resource 1). Most of these mistakes are of little consequence because they are not difficult to recognize and because no useful inferences were drawn from them. A few such mistakes in the Conclusions section are of more concern because misinformation there might be unrecognized and repeated by others.

More serious than the simple mistakes and inconsistencies are some assertions that are not supported by the results. Clauer et al. (Reference Clauer, Williams and Uysal2022, p. 75) initially recognized that, for each of the two bentonite samples, δ7Li did not vary beyond analytical uncertainty among the three size fractions studied. Yet, in the second half of the final paragraph of the Discussion, variations in δ7Li are described and discussed as if there were no analytical uncertainty in the values. Consider the final sentence, about supposed variations in δ7Li among the three fine-clay subfractions of sample B1:

The zigzaging variation in the δ7Li of the three B1 fractions with the lower value for the intermediate fraction is probably due to the dominant volcanic original reference in the coarser fraction combined with a variable impact of external pore fluids during further crystallization of the fine crystals. (p. 81)

If a measured quantity varies only within the range of its analytical uncertainty, asserting probable causes for those variations is unwarranted.

Consideration of analytical uncertainty is also essential to recognize another misinterpretation of results:

The δ11B remains almost constant in the A1 fractions relative to a continuously increasing K content with size, strongly suggesting that the illite content in the smectite-type interlayers is related to crystal size. This constant δ11B relative to an increasing K content indicates that the fluids had to remain identical in composition and at an almost constant temperature during illite growth; the K increase following the overall crystal growth. (p. 80)

The constancy of δ11B in the A1 subfractions does not require that temperature was almost constant during illite growth. The values of δ11B for the illite in the A1 subfractions are not known. The authigenic-illite content of the subfractions is <10% (Clauer et al., Reference Clauer, Williams and Uysal2022, Table 1), so temperature-dependent variation among subfractions in δ11B of the authigenic illite would not likely have caused variation in the subfraction δ11B values beyond the analytical uncertainty, which was ±1‰ at the 95% confidence level according to the typical precision for δ11B shown in Table 2 of Clauer et al. (Reference Clauer, Williams and Uysal2022). Specifically, not more than a 3‰ difference in δ11B (Williams et al., Reference Williams, Środoń, Huff, Clauer and Hervig2013, Fig. 8A) between the first- and last-formed authigenic illite would be expected if the illitization temperature range was from 60°C to 95°C and fluid δ11B did not change. Corresponding differences in δ11B among subfractions would have been far less than 3‰, however, because authigenic illite was diluted by much more-abundant smectite and because authigenic illite in the several fine-clay subfractions would have differed in average crystallization temperature by much less than 35°C.

There is reason to expect that tetrahedral boron is somewhat more abundant in illitic layers of I-S than in smectitic layers, but no reason to expect that such enrichment would be sufficient to have caused a δ11B difference of more than 1‰ among the A1 subfractions. Consider a few quantitative examples for hypothetical bentonite size fractions having 10% illite in I-S. Let each subfraction contain 20% by mass of illite fundamental particles 2 nm thick (Nadeau, Reference Nadeau1999, Fig. 3), and let the rest be smectite particles 1 nm thick. Consider the smectite particles to be uniform in δ11B and the illite particles to have δ11B dependent only on their crystallization temperature. If the B content of the illite particles were twice that of the smectite particles, the maximum difference in δ11B between two size fractions would be only 1‰. To reach that maximum would require that all the illite particles in one size fraction crystallized at 60°C and all in the other fraction crystallized at 95°C—a constraint that would not be realized in a natural system. If the illite particles were distributed as they might be in a natural system, so that, for example, the average crystallization temperatures of illite particles in two size fractions differ by 20°C instead of by 35°C, the illite particles would need to be enriched in B by a factor greater than 5 to cause the difference in δ11B between two size fractions to be greater than 1‰.

No information is available for sample A1 about the enrichment of B in authigenic illite relative to smectite, nor is there information about the distribution of early formed and late formed authigenic illite among the fine-clay subfractions. Without such information, there is no basis to assert that illite in that sample grew at an almost constant temperature.

Similar concerns apply to the discussion of the constancy of δ7Li in the A1 subfractions:

The δ7Li of the three A1 fractions averages +9.6±1.6‰ (n=9) with a content of 112±15 μg/g. Both values are statistically within analytical uncertainty, suggesting again that the illite layers of the smectite-rich size separates formed in equilibrium with a chemically stable fluid, the initial crystals forming with a minimal change in the burial temperature. (p. 80)

Constancy of δ7Li among subfractions is less informative about illite growth than is constancy of δ11B, because temperature-dependent isotopic fractionation is somewhat less for Li than for B (Williams et al., Reference Williams, Środoń, Huff, Clauer and Hervig2013, Fig. 8B), because the analytical uncertainty for δ7Li is about twice that for δ11B (according to the typical 2σ precision for δ7Li shown in Table 2 of Clauer et al., Reference Clauer, Williams and Uysal2022), and because there is no expectation of enrichment of structural Li in illite relative to smectite. The Li isotopic compositions of the A1 subfractions surely were determined largely by the Li in the smectite; they tell nothing useful about the conditions under which the illite layers formed.

Failure to recognize that the measured boron isotopic compositions are not those of illite may be responsible for some assertions in the abstract that are not supported by results: “The δ11B of the few illitic tetrahedral sites from one of the samples remains quite constant, …”; “In the second sample, the δ11B of the illite layers from the two coarser fractions is indicative of an early volcanic origin, while the smaller size fraction also interacted with sedimentary fluids.”; “In turn, the information of the B and Li isotopic compositions and contents from studied mixed layers suggests a various origin for the few illite layers of the smectite-rich I-S that contain more B than the smectite layers that host more Li.” In recognition that the isotopic analyses do not tell the isotopic compositions of B and Li in the few illite layers of the studied bentonites, the message for future investigators should be that to use isotopic studies of B and Li to find conditions of initial illitization of smectite in marine bentonites would be a very demanding task.

Supplementary Information

The online version contains supplementary material available at https://doi.org/10.1007/s42860-022-00205-5.

Funding

Not applicable

Data availability

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Code availability

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Declarations

Conflicts of interest

The author declares that he has no conflict of interest.

References

Clauer, N., Środoń, J., Aubert, A., Uysal, I. T., & Toulkeridis, T. (2020). K-Ar and Rb-Sr dating of nanometer-sized smectite-rich mixed layers from bentonite beds of the Campos Basin (Rio de Janeiro State, Brazil). Clays and Clay Minerals, 68, 446464.CrossRefGoogle Scholar
Clauer, N., Williams, L. B., & Uysal, I. T. (2022). Boron and lithium isotopic signatures of nanometer-sized smectite-rich mixed-layers of bentonite beds from Campos Basin (Brazil). Clays and Clay Minerals, 70, 7283.CrossRefGoogle Scholar
Nadeau, P. H. (1999). Fundamental particles: an informal history. Clay Minerals, 34, 185191.CrossRefGoogle Scholar
Williams, L. B., Środoń, J., Huff, W. D., Clauer, N., & Hervig, R. L. (2013). Light element distributions (N, B, Li) in Baltic Basin bentonites record organic sources. Geochimica et Cosmochimica Acta, 120, 582599.CrossRefGoogle Scholar
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