Alva-Valdivia Luis Manuel*a,
Agarwal Amar
b,
Urrutia-Fucugauchi Jaimea and
Hernández-Cardona Arnaldo
c
aLaboratorio de Paleomagnetismo, Instituto de Geofísica, Universidad Nacional Autónoma de México, Ciudad de México, 04510, Mexico
bDepartment of Earth Sciences, Indian Institute of Technology Kanpur, Kanpur, 208016, India
cPosgrado en Ciencias de la Tierra, Instituto de Geofísica, Universidad Nacional Autónoma de México, Ciudad de México, 04510, Mexico
First published on 31st October 2023
We investigate the origin of the magnetite nanoparticle aggregates (MNAs) from the Peña Colorada iron-ore mining district (Mexico) to devise a nature inspired synthesis process. Three types of samples were used: natural MNAs recovered from the mine, concentrated magnetite microparticles as reference material, and thin berthierine films used to synthesize MNAs. The chemical, mineralogical, crystallographic and rock magnetic properties were determined by polarized microscopy, high-resolution transmission electron microscopy, electron microprobe, X-ray diffraction, Mössbauer spectroscopy, and thermomagnetic and hysteresis measurements. MNAs were synthesized in the lab with the following steps. We start with berthierine thin films, which are heated to temperatures between 495 and 510 °C leading to formation of numerous stable magnetite nanocrystals. They grow at a temperature above 650 °C. Space restrictions lead to the formation of dense MNAs. Smaller MNAs, <200 nm, with a Curie temperature of 650 °C, shows superparamagnetic behavior. While larger MNAs, >7 μm, show Curie temperature of 578 °C and ferromagnetic behavior. Based on present observations, we suggest that MNAs in the Peña Colorada iron-ore formed in a marine environment, where berthierine formation was accelerated by Fe-rich hydrothermal springs that supplied iron and increased the temperature. Most notably, our laboratory experiments mimicked natural conditions and were able to successfully nucleate and grow magnetite nanoparticles which developed into MNAs. These MNAs were similar to those recovered from the Peña Colorada iron-ore deposit. This study, thus, provides a nature inspired method for synthesis of magnetite nanoparticles and its aggregates.
Well established methods of synthesizing nanoparticles require hazardous chemicals and physical conditions such as extremely high temperature and pressure. Thus, nature inspired synthesis procedures need to be established and developed.3,7,8 To the best of our knowledge such methods for preparing magnetic nanoparticle aggregates (MNAs) have not yet been well established. Our study, thus, investigates the natural origin and genesis of MNAs found in the Peña Colorada iron-ore deposit. This iron-ore mine is located at the Pacific continental margin in southern Mexico (Fig. 1). It is the main iron-ore and pellet producer in Mexico. The main Fe-ore is magnetite, which is being mined since 1975.9 We identified natural magnetite nanoparticles that form dense MNAs. Within the MNAs, the open spaces are filled mostly with berthierine, (Fe, Mg, Al)6(Si, Al, Fe)4O10(OH)8, and in minor proportion by calcite, quartz, apatite, cryptocrystalline and colloidal silica, hematite, siderite, feldspar, pyrite, chalcopyrite, pyrrhotite, marmatite, galena, covellite, native gold and argentite.10,11
The MNAs were initially reported first during the mine exploitation activities in 1987.12,13 In these MNAs, magnetite nanoparticles are embedded in the berthierine matrix (Fig. 2).2,14,15 Smaller MNAs, <200 nm, with a Curie temperature of 650 °C, shows superparamagnetic behavior. While larger MNAs, >7 μm, show Curie temperature of 578 °C and ferromagnetic behaviour.2 These observations sparked interest in the formation and the magnetic properties of the MNAs, their mineralogical and textural relationships with berthierine, and its implications on the depositional environment.
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Fig. 2 SEM images showing intergranular nanostructured mineral formed by 22 μm to 5 μm MNA embedded in berthierine. |
Recent results16 showed a non-linear relation between agglomeration state and magnetic properties. The magnetization in agglomerated magnetite is more sensitive to temperature than the smaller individual dispersed particles.16–18 The present study, therefore, investigates the natural MNAs and compares their characteristics with reference magnetite and synthesized MNAs through laboratory experiments. The results underline the use of MNAs as a potential indicator of geological environment in which the iron ore was deposited and, provide a possible nature inspired methodology for preparation of MNAs for societal use.
To study the changes in MNAs with variation in grain size and temperature we used mechanical and magnetic separations. For grain size analysis MNAs were separated into different sizes through a granulometric classification using a Warman-M8 cyclosizer equipment, sub-sieve sizer.2 This instrument classifies and separates the particles as a function of the size through centrifugal force under controlled conditions (water temperature, density of the dry sample, flux and time of feeding, etc.). MNA fractions were separated into size ranges: 56–30 μm, 30–22 μm, 22–15 μm, 15–10 μm, 10–7 μm and 7–0.1 μm. A few smaller MNAs, 2 to 15 nm in size, were also obtained. Then the effects of temperature on MNAs were analyzed using optical microscopy, differential thermal and gravimetric analysis (DTA-GTA), Xray diffractometry (XRD), electron microprobe (EPMA), and high-resolution transmission electron microscopy (HRTEM). Magnetic characterization was done by analysing the changes in magnetic susceptibility with frequency (χFD%) and high-temperature (thermomagnetic), and by investigating the changes in magnetisation with applied field (hysteresis).
Light microscopy was done on a Leica MZ 7.5 stereoscope microscope a Leica DMLP polarizing microscope. XRD was done with Bruker D-8 advance with Cu Kα and λ = 1.5418 Å radiation and graphite monochromator. Diffplus B-S software and international crystal powder diffraction (ICPD) database. Electron probe X-ray micro-analyses was done using JEOL JXA 8900-R with dispersive energy spectrometers of X-ray wavelength (WDS) standards SPI#02753-AB. DTA-GTA analyses using a Shimatsu ATR at room conditions with 70 mg sample under temperature from 19 °C to 1100 °C and an interval of 1 °C per minute. HRTEM was done with a JEOL 2010 FEG FASTEM.
χFD% and thermomagnetic measurements were done using a Bartington MS2 with an MS2W sensor, coupled to a furnace MS2WFP. Low and high frequency of 470 Hz and 4700 Hz were used for χFD% measurements, which are especially useful to distinguish ultrafine magnetite grain with superparamagnetic (SP) behavior. During thermomagnetic measurements the samples were heated in air from room temperature to 700 °C and then cooled back. The magnetic susceptibility is measured during the entire process of heating and cooling. Hysteresis was determined using small core-chips measured in a Princeton Instrument AGFM 2900 (MicroMag) employing a maximum applied field of up to 1.5 T.
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Fig. 3 HRTEM of material around the nanoparticles. The spheres of magnetite (Mt) enclosed in berthierine (B) and associated colloidal silica (Si) and gold inclusions (Au). |
The XRD spectrum analysis (Fig. 4) reveals intense magnetite peaks corresponding to (220) d = 3.00 Å, (311) d = 2.55 Å, (111) d = 4.90 and (222) with d = 2.43 Å. Berthierine peaks correspond to (001) with d = 7.12 Å and (002) with d = 3.55 Å. The magnetite peaks are irregularly shaped with wide base, indicating a significant contribution from nanometer-scale grains.2
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Fig. 4 XRD spectrum of the nanoscopic material around the nanoparticles showing characteristic peaks of magnetite (Mt), berthierine (B), feldspar (Fl) and quartz (Q). |
The Mössbauer spectrum of the intergranular material around the nanoparticles (Fig. 5), shows six spectra doublets, typical of magnetite. The Fe3O4 molecule is in two magnetic states: ferromagnetic state indicated by a sextuple spectrum, corresponding to the micrometric size magnetite aggregates >0.2 μm; and superparamagnetic state represented by a doublet spectrum corresponding to the MNAs of nanometer-scale <200 nm. The magnetic state of the MNAs depends strongly on their degree of compaction.
The chemical properties of the MNAs obtained by WDS multi-elemental analysis in selected fields (ESI Table 1†) reveals Fe3+ = 15.59 to 15.69 wt% and Fe2+ ions = 7.78 to 7.83 wt%, and elemental trace impurities (<0.2 wt%) of Mn, Ca, Mg, Ti, Al, V, Si, Na and K.
Thin berthierine films were separated from the ore fragments using a stereomicroscope. The films were annealed at 360, 495, 510, 570, 650 and 750 °C (Fig. 6), and the changes were characterized. Initially at the room temperature, the XRD pattern reveals distinct (001) and (002) peaks of berthierine, which have a d value of 7.18 Å and 3.55 Å, respectively. The XRD pattern also presents (311) and (222) magnetite peaks, with d value of 2.53 Å and 2.15 Å, respectively.
Exothermic reactions at 360 °C and 495 °C (Fig. 6) mark dehydration of magnetite nanoparticles and berthierine, respectively. Due to the dehydration, at 360 °C, the intensity of (001) and (002) berthierine peaks decreases (Fig. 8). Endothermic dehydration at 430 °C and 550–558 °C (Fig. 6) lead to loss of crystallinity. The berthierine samples, after heating up to 495–550 °C for 2 hours, lose their crystallinity and transform in an amorphous colloid.
Intense exothermic reactions at ca. 650 °C is owed to formation of new magnetite nanoparticles and growth of pre-existent magnetite nanoparticles to over 10 nm. These larger nanoparticles saturate the colloid favoring their contact and subsequent aggregation (Fig. 7). New magnetite nanoparticles are represented by novel XRD peaks in the spectra (Fig. 8a) compared to the original (Fig. 4). At 650 °C, the magnetite nanoparticles present zone edge oriented at [011], with interplanar distance d1 = 2.43 Å, d2 = 2.53 Å and d3 = 3.0 Å, and corresponding to (222) (220) and (311) planes, respectively (Fig. 9a). These interplanar distances are consistent with those reported for magnetite.20 HRTEM and FFT analyses of these nanoparticles reveals absence of crystal defects and significative structure transformation. This explain their resistance to oxidation and a high Tc.
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Fig. 7 HRTEM contrast Z images of a berthierine concentrate annealed at 650 °C. The semispherical magnetite nanoparticles (2 to 255 nm) are embedded in amorphous berthierine matrix. |
After the first annealing at 650 °C, we apply second annealing at the same (650 °C) temperature to explore the repeatability of the procedure (ESI Table 2†). XRD reveals similar results (Fig. 8c) and underlines the repeatability of the experiment.
Further annealing at 750 °C leads to oxidation of some magnetite to maghemite. The formation of maghemite is marked by a decrease in intensity of the (311) magnetite peak at 2θ angle of 35° (compare Fig. 8a with b). Newly formed maghemite is represented in HRTEM image by crystallites having interplanar distance d1 = 2.00 Å, d2 = 2.53 Å, d3 = 3.79 Å, corresponding to the (400), (311) and (210) planes, respectively (Fig. 9b and c). Magnetic interaction among magnetite nanoparticles results in aggregation of denser magnetite nanoparticles. Exothermic reactions at 750–780 °C mark transformation of magnetite to hematite nanoparticles.
In contrast, the MNAs (Fig. 10b) reveal four well defined exothermic reactions at 360 °C (exo-medium), 465 °C (exo-very small), 635 °C (exo-large) and 750 °C (exo-large). The first exothermic reaction, at 360 °C, is owed to partial oxidation and transformation (along the grain boundaries) of magnetite nanoparticles to maghemite (ESI Fig. 1a†). Although the phase change occurs over a wider temperature range 276 to 382 °C, it peaks at 360 °C and is accompanied with 1.14% weight loss. Transformation of magnetite to maghemite is slow process. It requires longer exposers at a specific temperature for oxidation to reach from the crust of the grain to its core. The second, slightly exothermic reaction at 485 °C is marked with a slight bump in the DTA curve. This reaction indicates starting of oxidation MNA core to maghemite.
The high exothermic reactions at 635 °C occur by transformation of the crust of MNAs, formed of maghemite, to hematite (γ-Fe2O3 → α-Fe2O3), while their core remains maghemite. The DTA curve shows wide amplitude in the interval 600 to 675 °C (Fig. 10b), supporting the loss of weight as showed in the GTA curve. Optical microscopy and XRD of MNAs annealed at 650 °C reveal a magnetite core, a surrounding layer of maghemite and outermost layer of hematite. The largest MNAs, thus, do not oxidize completely at 650 °C.
In summary, the oxidation front moves slowly towards the interior of the MNAs with gradually increasing temperature from 380 °C to 750 °C (ESI Fig. 1b†). At 750 °C the core of the MNAs are transformed to maghemite, marked by the peak in the DTA-GTA spectrum (Fig. 7b). This is in contrast to the standard magnetite that oxidises to hematite at 615 °C. The oxidation of MNA core at 750 °C is accompanied by a gain in weight of 1.14%. Continued heating till 1100 °C causes complete transformation of MNAs to hematite and a weight gain of 8.18%.
Sample | Mr (μA m2) | Ms (μA m2) | Mr/Ms | Hc (mT) | Hcr (mT) | Hcr/Hc | M (mg) | Ms/M (mA m2 kg−1) |
---|---|---|---|---|---|---|---|---|
A-3n (base) | 0.1549 | 2.48 | 0.062 | 8.18 | 26.400 | 3.227 | 12.0 | 0.207 |
A-3n annealed at 650 °C | 0.0858 | 7.789 | 0.011 | 10.23 | 24.34 | 2.38 | 16.9 | 0.46 |
A-3n annealed at 750 °C | 0.6008 | 4.285 | 0.142 | 7.51 | 13.59 | 1.81 | 21.4 | 0.2 |
A-3n annealed at 650 °C (2nd run) | 0.0341 | 3.405 | 0.010 | 5.14 | 6.13 | 1.19 | 20.3 | 0.17 |
MNA samples with largest grain size, 56 to 19 μm, annealed at 380 °C, have maghemite at boundaries with magnetite at the core (Fig. 1a, ESI†). With increasing annealing temperature, maghemite proportions increase. This is evident in the heating branch of thermomagnetic curves, where the maghemite Tc, between 350–380 °C becomes more prominent with the with increasing heat treatment (Fig. 11).
This laboratory synthesis is analogous to enrichment of berthierine in marine environment, where, colloidal berthierine is constantly enriched with Fe from external sources such as marine chimneys that discharge Fe-rich brines. The increasing of temperature during the experiment mimics the temperature increase due to the hydrothermal pulses and works in favor of nucleation and growth of magnetite nanoparticles, which later form MNAs.
Firstly, the reference magnetite shows three well-defined exothermic reactions at 285 °C, 375 °C and 615 °C (Fig. 10a) during its complete change to maghemite and later to hematite, Fe3O4 → γ-Fe2O3 → α-Fe2O3. On the contrary, the MNAs reveal four well-defined exothermic reactions at 360 °C, 485 °C, 635 °C, 750 °C (Fig. 7b). The first two correspond to partial oxidation to maghemite and hematite, respectively, and the last two reactions (465 °C and 750 °C), perhaps to the complete oxidation. The MNAs start to lose weight from 200 °C to 727 °C and thereafter gain weight due to the growth of magnetite nanoparticles up to 1050 °C.
Secondly, the reference material presents a Tc of 580 °C, which agrees with the published Curie point for pure magnetite.30 Whereas, Tc of the MNAs is >650 °C, which may due to hematite.
To summarize, the thermal reactions in reference magnetite initiate at lower temperatures and progress rapidly, while in the MNAs thermal reactions initiate at higher temperatures and progress slowly according, demonstrating the heat resistance of MNAs.
In marine conditions, berthierine is formed by colloidal diagenetic processes. Supply of heat and iron from hydrothermal solutions coming out of marine chimneys31 could spark a series of reactions and physicochemical adjustments in composition to form the MNAs.
Most notably, our laboratory experiments that mimicked natural conditions and were able to successfully nucleate and grow magnetite nanoparticles which developed into MNAs. The MNAs were similar to those recovered from the Peña Colorada iron-ore deposit. This study provides a nature inspired method for synthesis of magnetite nanoparticles and its aggregates which do not require harmful chemicals and the starting material is also naturally derived.
The physical and chemical settings of the experiments allow the prediction of the environmental conditions for the formation of the natural magnetite nanoparticle aggregates. It is suggested that the magnetic nanoparticle aggregates at the Peña Colorada iron mine developed in shallow to a deep marine environment with redox conditions. This was facilitated by Fe rich hydrothermal source such as marine chimneys. Because of this, we propose that the MNAs act as genetic indicators and reveal the geological conditions of their formation.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d3ra04065h |
This journal is © The Royal Society of Chemistry 2023 |