Faisal T.
Adams
*a,
McNeill
Bauer
a,
Clément
Levard
b and
F. Marc
Michel
a
aDepartment of Geosciences, Virginia Polytechnic Institute and State University, Blacksburg, VA 24061, USA. E-mail: fadams@vt.edu
bAix Marseille Univ, CNRS, IRD, INRAE, Coll France, CEREGE, Aix-en-Provence, France
First published on 21st February 2024
Interest is growing in nanoparticles made of earth abundant materials, like alumino(silicate) minerals. Their applications are expanding to include catalysis, carbon sequestration reactions, and medical applications. It remains unclear, however, what factors control their formation and abundance during laboratory synthesis or on a larger industrial scale. This work investigates the complex system of physicochemical conditions that influence the formation of nanosized alumino(silicate) minerals. Samples were synthesized and analyzed by powder X-ray diffraction, in situ and ex situ small angle X-ray scattering, and transmission electron microscopy. Regression analyses combined with linear combination fitting of powder diffraction patterns was used to model the influence of different synthesis conditions including concentration, hydrolysis ratio and rate, and Al:
Si elemental ratio on the particle size of the initial precipitate and on the phase abundances of the final products. These models show that hydrolysis ratio has the strongest control on the overall phase composition, while the starting reagent concentration also plays a vital role. For imogolite nanotubes, we determine that increasing concentration, and relatively high or low hydrolysis limit nanotube production. A strong relationship is also observed between the distribution of nanostructured phases and the size of precursor particles. The confidences were >99% for all linear regression models and explained up to 85% of the data variance in the case of imogolite. Additionally, the models consistently predict resulting data from other experimental studies. These results demonstrate the use of an approach to understand complex chemical systems with competing influences and provide insight into the formation of several nanosized alumino(silicate) phases.
Synthetic imogolite has been researched for use in catalysis, gas adsorption, and polymer nanocomposites among other applications due to its tunable size, hydrophilicity, high surface area and aspect ratio, and functionalized surface.1–5 Both imogolite (Al2SiO3(OH)4) and proto-imogolite are aluminosilicate nanominerals that typically occur together in varying proportions, and although the primary distinguishing factor between them is their morphologies, they are both suggested to possess the same “imogolite-like local structure” (ILS).6 These aluminosilicates are composed of gibbsite-like sheets of aluminum hydroxide (Al(OH3)) with isolated silica (SiO4) tetrahedra occupying the center position of the six-membered rings formed by the Al octahedra.7
Imogolite forms high aspect ratio nanotubes that are 2–3 nm in diameter and can extend up to several μm in length,8,9 while proto-imogolite is said to possess a “rooftile” shape,10 eventually transforming into imogolite nanotubes in solution. The curvature observed in the particles is believed to be due to strain resulting from the size disparity between the silica tetrahedra and the lacunar sites of the gibbsite-like sheets. This discrepancy causes different types of curvature, resulting in the formation of tubes and spheres in one and two dimensions, respectively.6 The exact transformation method is still under discussion although an oriented aggregation-based growth is the foremost conclusion.6,11 Other secondary phases have been observed during the synthesis of these nanoparticles, specifically Al-(oxy)hydroxides and amorphous silica.12–14
Pseudo-boehmite is a poorly crystalline and hydrated aluminum oxyhydroxide (γ-AlOOH), studied for its influences spanning from radiolysis in nuclear material storage and waste sites15,16 to health applications, where it is one of the oldest and most commonly used adjuvants in vaccines.17 It is formed under similar conditions to its more crystalline counterpart, boehmite, from aluminum ion precursors hydrothermally aged at alkaline conditions, and has a double-sheet structure of aluminum octahedra forming nanosized wires, platelets or rafts.18,19 Alternatively, amorphous silica nanoparticles (SiO2) possess localized structures of 2-membered to 8-membered siloxane rings, and are arguably the most commonly produced of all synthetic nanosized materials.20 This nanoparticle has found widespread industrial use in food and cosmetics, as well as biotechnological applications in cancer therapy and enzyme immobilization.21,22
Several synthesis investigations have reported a mixture of 2 or more of these nanoparticles occuring12,13 and others have discussed isolated conditions impacting their formation,23,24 yet there has been no holistic study of the influence synthesis conditions have on the resulting phase distribution of these materials. Experimental studies of imogolite and proto-imogolite, or allophane ((Al2O3)(SiO2)1.3–2·2.5–3H2O), formation have tested separately the effects of starting concentration, pH, and elemental ratios on the various morphologies.25–28 Others have suggested that excess silica to aluminum in the starting solution will suppress imogolite formation due to the limited capacity for silica polymers in the inner tube. Excess silica may be accommodated by silica polymers residing in the larger interiors of spherical allophane and/or by the increased number of reactive surface sites on proto-imogolite fragments.7 Another study suggested that imogolite is not favored at hydrolysis ratios less than 1.5 due to differences in imogolite and proto-imogolite stabilities at different pH and OH:
Al ranges.24 Taken together these prior studies suggest that alumino(silicate) nanoparticle formation may be influenced by two or more competing factors. The presence of various mixtures of nanosized and/or nanostructured phases provides an additional challenge for quantifying them into separate phases, especially using relatively accessible scattering-based approaches like X-ray diffraction.
This paper attempts to describe which key variables including concentration, elemental Al:
Si ratio, hydrolysis ratio and speed of base addition impact the formation of these different nanosized minerals. The influence of these conditions on some precursor particle sizes and their compounding effect on nanotube formation is also described. Systematic synthesis experiments were combined with in situ and ex situ analytical characterization and multivariate linear regression analysis to determine the quantitative influence each factor had on final phase abundance. This is the first study designed to unravel the competing effects of these different synthesis variables, as well as to probe the role of precursor particle size on imogolite formation using experimental data. This study also employs a unique approach29 to quantify the distribution of nanoparticle mineral phases via linear combination fitting of laboratory powder X-ray diffraction data. The results are important for greater understanding of alumino(silicate) synthesis, where individual variables can be isolated and understood for their effect on the system. The framework of the study can be adapted and utilized for other chemical processes where competing effects complicate the products of a system.
The majority of the other products of the different synthesis experiments did not result in a single pure phase but contained a mixture of the different endmembers instead. Qualitative evidence for these mixtures was provided by pXRD, which showed combinations of distinct pXRD peaks for imogolite, proto-imogolite, pseudo-boehmite and/or amorphous silica all present in a single sample (Table 1).
Concentration (M) | NaOH addition (mL min−1) | Al![]() ![]() |
Hydrolysis ratio | Imogolite (%) | Proto-imogolite (%) | Am. silica (%) | Ps. boehmite (%) |
---|---|---|---|---|---|---|---|
0.005 | 10 | 1 | 2 | 100.0 | 0.0 | 0.0 | 0.0 |
0.005 | 5 | 1 | 2 | 90.9 | 0.0 | 0.0 | 9.1 |
0.005 | 10 | 2 | 2 | 19.7 | 0.0 | 3.8 | 76.5 |
0.005 | 2 | 2 | 3 | 9.7 | 16.9 | 8.6 | 64.8 |
0.005 | 2 | 1 | 3 | 8.4 | 0 | 2.7 | 88.9 |
0.005 | 2 | 2 | 2 | 100 | 0 | 0 | 0 |
0.005 | 5 | 1.5 | 2 | 100 | 0 | 0 | 0 |
0.005 | 5 | 2 | 3 | 0 | 27 | 3 | 70 |
0.005 | 10 | 1.5 | 3 | 0 | 59.8 | 2.8 | 37.4 |
0.005 | 10 | 1 | 3 | 0 | 74 | 10.3 | 15.7 |
0.005 | 5 | 1 | 0.5 | 6.6 | 87.5 | 5.9 | 0 |
0.005 | 2 | 2 | 0.5 | 33.8 | 52.4 | 6.6 | 7.2 |
0.005 | 10 | 2 | 1 | 89 | 5 | 0 | 6 |
0.005 | 10 | 2 | 0.5 | 50.6 | 38.9 | 0 | 10.5 |
0.005 | 2 | 1 | 1 | 15.6 | 73.9 | 0 | 10.5 |
0.01 | 5 | 1 | 2 | 32.4 | 67.6 | 0.0 | 0.0 |
0.01 | 2 | 1.5 | 2 | 20.2 | 79.8 | 0.0 | 0.0 |
0.01 | 2 | 1.5 | 3 | 0 | 29.2 | 9.8 | 61 |
0.02 | 10 | 1.5 | 1 | 9.6 | 48.9 | 29.4 | 12.1 |
0.05 | 5 | 2 | 2 | 23.7 | 76.3 | 0.0 | 0.0 |
0.05 | 5 | 2 | 3 | 6 | 0 | 1.4 | 92.6 |
0.05 | 10 | 1.5 | 0.5 | 0 | 78.8 | 21.2 | 0 |
0.05 | 10 | 1 | 0.5 | 0 | 77.3 | 22.7 | 0 |
0.05 | 5 | 1 | 3 | 0 | 90 | 10 | 0 |
0.1 | 5 | 2 | 3 | 10.5 | 0 | 0 | 89.5 |
0.1 | 10 | 1 | 0.5 | 0 | 36.4 | 63.6 | 0 |
0.1 | 10 | 2 | 0.5 | 0 | 70.1 | 29.9 | 0 |
0.1 | 10 | 2 | 2 | 0.0 | 96.0 | 4.0 | 0.0 |
0.1 | 2 | 1 | 1 | 0 | 92.6 | 7.4 | 0 |
0.1 | 10 | 1 | 2 | 0.0 | 96.4 | 3.6 | 0.0 |
0.1 | 5 | 1 | 1 | 0 | 82.2 | 17.8 | 0 |
0.1 | 0.5 | 2 | 1 | 0 | 84.1 | 15.9 | 0 |
0.1 | 10 | 1.5 | 3 | 0 | 32.5 | 0 | 67.5 |
0.125 | 10 | 2 | 1 | 0 | 56.5 | 43.5 | 0 |
0.125 | 2 | 1.5 | 1 | 0 | 72 | 28 | 0 |
0.125 | 5 | 2 | 1 | 0 | 77.5 | 22.5 | 0 |
0.125 | 1 | 2 | 1 | 0 | 85 | 15 | 0 |
0.125 | 2 | 1 | 1 | 0 | 58.3 | 41.7 | 0 |
0.125 | 2 | 2 | 1 | 0 | 79.9 | 20.1 | 0 |
0.125 | 5 | 1.5 | 3 | 0 | 86.2 | 13.8 | 0 |
0.125 | 2 | 2 | 2 | 0.0 | 90.4 | 9.6 | 0.0 |
0.125 | 10 | 1.5 | 3 | 0 | 50.5 | 7.3 | 42.2 |
0.125 | 10 | 1 | 3 | 0 | 93 | 7 | 0 |
0.125 | 5 | 1 | 3 | 0 | 94 | 6 | 0 |
0.15 | 2 | 2 | 3 | 5.8 | 0.1 | 3 | 91.1 |
0.15 | 5 | 2 | 1 | 0 | 91.6 | 8.4 | 0 |
0.15 | 5 | 1 | 1 | 0 | 60.7 | 39.3 | 0 |
0.15 | 2 | 2 | 1 | 0 | 85.4 | 14.6 | 0 |
0.15 | 0.5 | 2 | 1 | 0 | 84.7 | 15.3 | 0 |
0.15 | 5 | 1.5 | 2 | 0.0 | 85.3 | 14.7 | 0.0 |
0.15 | 1 | 2 | 1 | 0 | 91.2 | 8.8 | 0 |
0.15 | 10 | 1.5 | 3 | 0 | 76.5 | 0 | 23.5 |
0.16 | 10 | 1 | 1 | 0 | 54.9 | 45.1 | 0 |
0.16 | 10 | 1.5 | 1 | 0 | 74.1 | 25.9 | 0 |
0.16 | 2 | 2 | 1 | 0 | 75.6 | 16.4 | 8 |
0.175 | 0.5 | 2 | 1 | 0 | 65.1 | 34.9 | 0 |
0.175 | 0.5 | 1 | 1 | 0 | 61.1 | 38.9 | 0 |
0.175 | 2 | 1 | 1 | 0 | 36.6 | 63.4 | 0 |
0.175 | 5 | 1 | 1 | 0 | 53.7 | 46.3 | 0 |
0.175 | 10 | 1.5 | 3 | 0 | 45.7 | 27.1 | 27.2 |
0.175 | 2 | 1.5 | 1 | 0 | 72.3 | 27.7 | 0 |
0.175 | 5 | 2 | 1 | 0 | 83.8 | 16.2 | 0 |
0.175 | 2 | 2 | 1 | 0 | 87.6 | 12.4 | 0 |
0.175 | 10 | 2 | 3 | 0 | 79.1 | 0 | 20.9 |
0.185 | 2 | 2 | 1 | 0 | 38.4 | 61.6 | 0 |
0.185 | 2 | 1 | 1 | 0 | 48 | 52 | 0 |
0.185 | 5 | 1.5 | 3 | 0 | 100 | 0 | 0 |
0.2 | 2 | 2 | 1 | 0 | 79.6 | 20.4 | 0 |
0.2 | 2 | 2 | 3 | 0 | 25.7 | 2.6 | 71.7 |
0.2 | 10 | 1 | 0.5 | 0 | 26.3 | 73.7 | 0 |
0.2 | 10 | 1.5 | 0.5 | 0 | 39 | 61 | 0 |
0.2 | 10 | 1.5 | 1 | 0 | 72.8 | 27.2 | 0 |
0.2 | 10 | 1 | 3 | 0 | 93 | 7 | 0 |
0.2 | 10 | 1 | 2 | 0.0 | 100.0 | 0.0 | 0.0 |
This binary regression was used to determine the concentration at which imogolite nanotubes are likely to occur. A subset of the data in Table 1 obtained using that concentration cutoff was then analyzed with a multivariate regression to determine factors affecting the proportion. The proportion of imogolite is modeled with the following relationship:
![]() | (1) |
In eqn (1), IM represents the resulting proportion of imogolite as a percentage, conc refers to the initial Al solution concentration (M), H corresponds to the hydrolysis ratio (mol mol−1), rate is the rate of base addition (ml min−1) and cat is the cation ratio (mol mol−1). The negative coefficient for concentration implies increased imogolite proportion with lower concentrations, while the quadratic relationship for the amount of base added implies decreased proportion at relatively low and high OH:
Al ratios. We also observe a complex relationship between the hydrolysis ratio, rate at which the base is added, and the cation ratio as indicated here by the interaction terms and visualized in the ESI (Fig. S2†). The overall model was found to be significant, with a p-value less than 0.0001, and an adjusted R2 of 0.85, meaning it explains 85% of the variance in the data. The starting concentration and hydrolysis ratio were both considered statistically significant factors, with confidence >99.99%. Cation ratio was significant, by virtue of its interaction with the rate at which base is added, at >95% confidence. The imogolite proportions predicted in the model were compared to the experimentally measured counterparts based on the initial synthesis conditions, and the resulting plot is shown in Fig. 4a.
The Root Mean Square Error (RMSE) is 0.65, meaning the model can predict the imogolite proportion to within ±0.3%, after correcting for the cube root transformation. The Durbin–Watson (DW) statistic for the residuals of this model is 2.95, and we therefore fail to reject the null hypothesis that the residuals are independent at a p-value of 0.05. A plot of the model predicted values and their corresponding residuals as observed in Fig. 4 was used to check for adherence of the results to modeling assumptions.
The residuals were assessed using the Shapiro–Wilks test, and we failed to reject the null hypothesis that the residuals are normally distributed at a p-value of 0.05. Normality of residuals was further confirmed, visually, using a Q–Q plot (not shown). For subsequent models, these checks are summarized in the ESI (Table S1†).
A similar approach was employed for the pseudo-boehmite model, which also exhibited a prevalence of zero values. The logistic regression for this phase showed that hydrolysis is the dominant factor determining the presence of pseudo-boehmite.
From the model for Fig. 3, we determine that hydrolysis ratios higher than 2.53 have >50% probability of producing pseudo-boehmite. Using that cutoff and performing the multivariate regression analysis on the resulting subset of data, the following model for the pseudo-boehmite proportion is obtained:
![]() | (2) |
In eqn (2), PB represents the resulting proportion of pseudo-boehmite as a percentage, conc refers to the initial solution concentration (M), and cat corresponds with the Al:
Si cation ratio (mol mol−1). The overall model is statistically significant with p-value = 0.0002. The statistically significant synthesis parameters are concentration (>99%) and cation ratio (>99.9%). Although the negative coefficient for concentration implies an inverse relationship with pseudo-boehmite proportion, and the positive value for cation ratio indicates increased proportion with increasing cation ratio, the presence of an interaction term implies there may be slight variations in the trends. These variations are visualized in the ESI (Fig. S3†). This model passes all feasibility tests of normality, autocorrelation, and residual trends. The fits and residual plots are shown in Fig. 4.
Proto-imogolite showed up in various quantities for most conditions used in Table 1. A multivariate regression was carried out on the entire dataset, producing the following model:
![]() | (3) |
Here, the percentage proportion of proto-imogolite is expressed as PI, while rate refers to the rate of base addition (mL s−1). The ubiquitous nature with which this particle occurs means there are complex trends even with individual synthesis parameters. Modeling the data requires the use of additional variables as observed in eqn (3). This model implies that slower base addition, and higher cation ratio promote proto-imogolite formation, however, the inclusion of interaction terms indicates variations in those trends (Fig. S4†). Both variables were found to be statistically significant, while the overall model was also significant with a p-value less than 0.0001. The model passes all feasibility tests while the resulting fit and residual trend are shown in Fig. 4.
Finally, the model developed for amorphous silica synthesis is described as:
![]() | (4) |
Eqn (4) implies that a relative increase in the concentration of starting reagents, as well as a relative decrease in the hydrolysis ratio are the key factors promoting proto-imogolite (PI) formation. Intuitively, lower Al:
Si ratios (expressed as cat in eqn (4)) suggest that as Si increases relative to Al, excess Si further contributes to the total amorphous silica proportion. The interaction term in this model indicates that higher initial concentrations significantly increase amorphous silica proportion at a hydrolysis ratio of 2 or less (Fig. S5†). Al concentration and hydrolysis ratio were the most important factors with >99.999% significance. The model passes all feasibility tests while the resulting fit and residual trend are shown in Fig. 4.
Concentration (M) | NaOH addition (mL min−1) | Al![]() ![]() |
Hydrolysis ratio | Mean diameter (nm) | Median diameter (nm) |
---|---|---|---|---|---|
0.005 | 2 | 1 | 3 | 8.2 | 2.8 |
0.005 | 2 | 2 | 3 | 8.6 | 3.2 |
0.005 | 10 | 1 | 2 | 1.16 | 1.2 |
0.005 | 10 | 2 | 2 | 1.2 | 1.2 |
0.005 | 2 | 2 | 2 | 1.1 | 1 |
0.005 | 10 | 2 | 2 | 1.2 | 1.2 |
0.005 | 5 | 1.5 | 2 | 1.04 | 1 |
0.01 | 2 | 2 | 3 | 7.3 | 2.8 |
0.05 | 5 | 2 | 3 | 3.8 | 1.6 |
0.05 | 10 | 1.5 | 0.5 | 1.0 | 1.0 |
0.05 | 10 | 1 | 0.5 | 1.6 | 1.6 |
0.1 | 0.5 | 2 | 1 | 1.5 | 1.4 |
0.1 | 2 | 1 | 1 | 1.6 | 1.5 |
0.1 | 5 | 1 | 1 | 1.8 | 1.8 |
0.1 | 5 | 2 | 3 | 4.0 | 1.6 |
0.1 | 10 | 1 | 0.5 | 1.0 | 1.0 |
0.1 | 10 | 2 | 0.5 | 1.2 | 1.2 |
0.125 | 1 | 2 | 1 | 1.8 | 1.8 |
0.125 | 2 | 2 | 1 | 1.5 | 1.4 |
0.125 | 5 | 2 | 1 | 1.7 | 1.6 |
0.15 | 0.5 | 2 | 1 | 1.9 | 1.4 |
0.15 | 1 | 2 | 1 | 1.1 | 1.1 |
0.15 | 2 | 2 | 1 | 1.7 | 1.8 |
0.15 | 2 | 2 | 3 | 1.6 | 1.6 |
0.15 | 5 | 1 | 1 | 1.6 | 1.5 |
0.15 | 5 | 2 | 1 | 3.6 | 1.6 |
0.175 | 0.5 | 1 | 1 | 1.5 | 1.6 |
0.175 | 0.5 | 2 | 1 | 1.6 | 1.6 |
0.175 | 2 | 2 | 1 | 1.3 | 1.2 |
0.175 | 5 | 1 | 1 | 1.6 | 1.6 |
0.175 | 5 | 2 | 1 | 1.7 | 1.5 |
0.175 | 10 | 2 | 3 | 1.8 | 1.2 |
0.185 | 5 | 1.5 | 3 | 2.0 | 1.2 |
0.2 | 10 | 1 | 3 | 2.4 | 1.2 |
A regression tree analysis was used to model the impact of input conditions on precursor particle size (Fig. 5a), and the subsequent role of that precursor size on the phase distribution of nanoparticles (Fig. 5b). To prevent overfitting, a minsplit of 5 was chosen during modeling, which corresponds to the minimum number of observations each terminal node must contain before a split is attempted.
We observed that the most significant input condition that determines precursor particle size is the amount of base added, followed by the initial Al concentration. At a hydrolysis ratio above 2.5, particles were mostly larger than ∼2 nm, and generally increased in size with decreasing concentration. From the second decision tree, we observe that the ∼2 nm cut-off indicates whether the system becomes predominantly Al-based (pseudo-boehmite) or aluminosilicate-based (proto-imogolite). Larger precursors (∼5 nm and bigger) correspond to a predominant pseudo-boehmite product at over 74%, while smaller (∼2 nm and smaller) particles resulted in proto-imogolite dominant products.
Tracking Dv(R) results in situ through the first hour of synthesis show the effect of pH during and after base addition on particle size. Throughout the pre-oven synthesis process, the size of precursor particles hovers around the same size, and there is no obvious increase in particle size with time. The mean distribution of particle sizes with time (Fig. S6†) confirms there is little to no particle growth until oven treatment.
Synthesis studies of an imogolite analogue discovered that at hydrolysis ratio values below 1.5, extensive tubular structures were unable to form, and significant structural defects were observed at values below 2.0.24 Our imogolite regression model supports that experimental result with imogolite proportion maximized close to OH:
Al of 2 and dropping off on either side of that value.
Additionally, increasing the initial concentration of reagents, specifically Al, leads to a lower proportion of imogolite. It has been suggested that an increase in concentration hinders imogolite proportion,36 and this effect has been attributed to the presence of Cl− ions commonly used in imogolite synthesis.37 Despite using electron microscopy with complementary XRD data, the authors of that study could not detect imogolite fibers when Cl− concentrations were above 50 mM. They also noticed that the use of diprotic bases, such as Ca(OH)2 that resulted in salts like CaCl2, returned relatively lower imogolite contents compared to monoprotic bases at similar cation concentrations. According to other studies, producing high concentrations of nucleated particles impede imogolite growth kinetics, especially the growth of longer tube structures.3,10 Our model agrees with the already established effects of concentration on imogolite proportion.
The Al:
Si ratio was a significant factor in modeling all phases except pseudo-boehmite. At lower pH values and in the presence of excess Si associated with lower Al
:
Si ratios, we suspect the Si complexes in solution polymerize since there are fewer gibbsite-like-sheets with which to bond. Further, amorphous Si has been shown to inhibit imogolite growth, while polymerizing Si chains originating on tetrahedral sites and creating Si-rich local structure are known to occur for proto-imogolite.7 We observe these effects as the prevalent co-existence of appreciable amounts of amorphous silica and proto-imogolite in our pXRD patterns, while the reverse holds true for imogolite predominant versions of our samples.
None of the products containing pseudo-boehmite exhibited the sharp diffraction peaks associated with its crystalline phase, despite being aged for 7 days. Compared to other similarly aged products, this finding hints at the presence of alumino(silicates) as a method for controlling or inhibiting the crystallization of pseudo-boehmite nanoparticles.
Using the models derived for each nanoparticle phase, we produce phase maps as a function of input Al, H+ and Si concentrations (Fig. 6). These maps confirm that there are localized areas in the chemical space where the proportion of any particle is maximized, with overlapping regions elsewhere that produce mixed phase products. Imogolite is observed to occur within a relatively narrow region of synthesis space, consistent with commonly reported conditions in the literature. Proto-imogolite occurs over a wider range, which could be explained by the suggestion that it has variations in composition, and this agrees with the more varied examples from the literature. Pseudo-boehmite occurs at relatively higher Al concentrations and lower acidity, while amorphous silica predominates at high Si concentrations except at very low acidity.
![]() | ||
Fig. 6 Phase maps of imogolite, proto-imogolite, pseudo-boehmite and amorphous silica. Contours are derived from model predicted values, and the base addition rate was optimized for the formation of imogolite and pseudo-boehmite in each case. Hollow circles represent the experimental data obtained in this study, and the size of each circle correlates to the percent proportion of that nanoparticle. The colored “x” shows the position of reported input conditions from the literature.7,25,38,39 These studies reported single phase products, so we assume 100% proportion of that particle in the respective phase map. |
The first split in our decision tree, corresponding to the greatest difference in resulting phase occurs at threshold of 2.3 nm – below this mean particle size, proto-imogolite becomes the dominant phase in the system. We are unable to detect the proposed critical size for imogolite formation at this stage of the synthesis process, as both imogolite and proto-imogolite precursors have similar sizes. It is also possible that the growth needed to achieve this critical size occurs very early on in the aging step, but after the hydrolysis stage. Our Dv(R) plots show that a range of particle sizes occur after hydrolysis (Fig. S8†), and the distribution of particle sizes are expected to directly correlate with the distribution of phases.6 Simulated fits of proto-imogolite SAXS data using a mixture of proto-imogolite sizes has been shown to adequately fit the corresponding SAXS data, further highlighting the polydispersity in precursor particle sizes.40
Past studies suggested that the mechanism of growth involves the thermodynamic self-assembly of precursor particles,41 while others proposed a kinetic growth process where “seeds” of pre-existing nanotubes grow to longer lengths in the presence of precursor particles.42 More recent studies seem to agree with the notion of kinetically driven growth via aggregation of pre-formed sections, although it is less certain why particle growth slows down drastically after approximately 3 days of aging.
These models can help answer questions about nanoparticle formation, and address factors in a uniquely systems-based approach not yet employed in this field. This approach can be applied to a multitude of geochemical systems to produce predictive models about crystallization. Using these models, we can probe questions about what chemical and physical properties are most important during mineral or precursor formation, which can lead to insights about mechanisms and reactions.
Footnote |
† Electronic supplementary information (ESI) available: Additional experimental results and modeling details, including TEM images, interaction plots, pH data, model checks and their descriptions (PDF). See DOI: https://doi.org/10.1039/d4nr00473f |
This journal is © The Royal Society of Chemistry 2024 |