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Search Results (37,013)

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20 pages, 8161 KiB  
Article
Research on Support Technology for Unstable Roof Roadway Under Abandoned Roadways in Ultra-Thick Coal Seam
by Xianyang Yu, Siyuan Lv, Yafei Luo, Pengchao Liu, Hao Fu and Yicai Zhou
Processes 2024, 12(12), 2886; https://doi.org/10.3390/pr12122886 (registering DOI) - 17 Dec 2024
Abstract
Due to the impact of disordered mining activities in previous years, numerous abandoned roadways exist in the second mining district of the 13# coal seam in Chejiazhuang Coal Mine. The stability of the new roadway roof was analyzed under various distributions of abandoned [...] Read more.
Due to the impact of disordered mining activities in previous years, numerous abandoned roadways exist in the second mining district of the 13# coal seam in Chejiazhuang Coal Mine. The stability of the new roadway roof was analyzed under various distributions of abandoned roadways above. It was determined that the ultimate stable thickness of the coal layer between the new and abandoned roadways is 4.0 m. When the thickness between the two is less than 4.0 m, the roof becomes unstable after excavation, posing a risk of collapse. Advanced grouting reinforcement is required to enhance roof stability before installing U-shaped steel arches. Mechanical experiments were conducted on the polymer grouting consolidation of fractured coal, showing a significant increase in residual strength compared to intact coal. Furthermore, the uniaxial compressive strength of the polymer grouting consolidation partially recovered. On average, the consolidation coefficient and recovery coefficient were 5.28 and 85.51%, respectively. Grouting increased the ductility of the fractured surrounding rock, enhancing its resistance to deformation and plasticity. A polymer grouting consolidation technology for supporting fractured surrounding rock under the unstable roof of abandoned roadways is proposed, along with the design of corresponding support schemes and parameters. Monitoring the results of mine pressure indicated that the surrounding rock remained stable after roadway excavation, validating the effectiveness of the support schemes and parameters. Full article
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Figure 1
<p>The engineering site in the Shanxi Provence of China.</p>
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<p>Roadway in Chejiazhuang Coal Mine with unstable roof.</p>
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<p>Stratigraphic column of 13# coal seam in Chejiazhuang Coal Mine.</p>
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<p>Mechanical model of roof rock beam of new roadway under abandoned roadway.</p>
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<p>Relationship between roof thickness and tensile stress in the midpoint of the lower layer of the rock beam.</p>
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<p>The cohesion of coal and fractured coal grouting consolidation.</p>
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<p>Calibrating the strain softening model for coal and fractured coal grouting consolidation (the test process of the mechanical parameters of coal and fractured coal grouting consolidation is introduced in <a href="#sec4-processes-12-02886" class="html-sec">Section 4</a>).</p>
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<p>Numerical simulation model and meshing.</p>
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<p>Plastic zone and fractured zone around abandoned roadway.</p>
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<p>Plastic zone and fracture zone of surrounding rock with roof thickness of 3.0 m.</p>
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<p>Plastic zone and fractured zone of surrounding rock with roof thickness of 3.5 m.</p>
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<p>Plastic zone and fractured zone of surrounding rock with roof thickness of 4.0 m.</p>
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<p>Plastic zone and fractured zone of surrounding rock with roof thickness of 4.5 m.</p>
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<p>Fracture coal grouting test’s flow chat.</p>
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<p>Grouting consolidation test equipment.</p>
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<p>Fractured coal grouting consolidation. (<b>a</b>) Fractured coal grouting consolidation; (<b>b</b>) fractured grouting consolidation.</p>
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<p>Interact coal and fractured coal grouting consolidation strength curve.</p>
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<p>Development of plastic zone and fractured zone in surrounding rock with polymer grouting (unstable roof).</p>
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<p>Support parameters for the roadway with an unstable roof under abandoned roadways (dimensions in the figure are given in millimeters (mm)). (<b>a</b>) A longitudinal section of the roadway (<b>b</b>) A cross-section of the roadway.</p>
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<p>Roadway’s surrounding rock displacement in monitoring site. (The red circle indicates the short anchor bolts installed in the surrounding rock. An L-shaped thick wire is welded to the nut of the bolt, which is used to observe the displacement of the surrounding rock in the roadway).</p>
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<p>Monitoring results of surface displacement in new roadway.</p>
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<p>The overall condition of the roadway after being supported.</p>
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15 pages, 2271 KiB  
Article
Determination of Methotrexate Using an Electrochemical Sensor Based on Carbon Paste Electrode Modified with NiO Nanosheets and Ionic Liquid
by Peyman Mohammadzadeh Jahani, Somayeh Tajik, Hadi Beitollahi, Fariba Garkani Nejad and Zahra Dourandish
Chemosensors 2024, 12(12), 266; https://doi.org/10.3390/chemosensors12120266 (registering DOI) - 17 Dec 2024
Abstract
In this paper, the application of NiO nanosheets (NiO NSs) for the detection of methotrexate (MTX) is described. The NiO NSs were synthesized using a hydrothermal method. The electrocatalytic activity of two modifiers, ionic liquid (IL) and NiO NSs, was examined on a [...] Read more.
In this paper, the application of NiO nanosheets (NiO NSs) for the detection of methotrexate (MTX) is described. The NiO NSs were synthesized using a hydrothermal method. The electrocatalytic activity of two modifiers, ionic liquid (IL) and NiO NSs, was examined on a carbon paste electrode (CPE) in relation to MTX, utilizing voltammetry methods such as cyclic voltammetry (CV), linear sweep voltammetry (LSV), differential pulse voltammetry (DPV), and chronoamperometry at 0.1 M phosphate buffer solution (PBS) pH = 7.0. The anodic peak currents for MTX on the NiO NSs/IL/CPE were approximately 3.5 times greater than those on unmodified CPE. Based on DPV measurements, the electrochemical sensor demonstrated a linear response in the concentration range (LDR: 0.01 µM to 160.0 µM), with a limit of detection (LOD: 0.003 µM). Moreover, the NiO NSs/IL/CPE sensor demonstrated good stability, repeatability, reproducibility, and selectivity, which were of importance in the electroanalysis of compounds. Lastly, the practicality of the NiO NSs/IL/CPE sensor was assessed by analyzing MTX levels in urine samples and pharmaceutical formulation, yielding satisfactory recovery rates of 97.1% to 103.3%. Full article
(This article belongs to the Special Issue Progress of Photoelectrochemical Analysis and Sensors)
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Figure 1
<p>XRD pattern of NiO NSs.</p>
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<p>FE-SEM images of NiO NSs at three different magnifications (scale bars: 1 µm (<b>a</b>), 500 nm (<b>b</b>), and 200 nm (<b>c</b>)).</p>
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<p>CVs of bare CPE (curve a), NiO NSs/CPE (curve b), and NiO NSs/IL/CPE (curve c) in 0.1 M phosphate buffer solution (pH 7.0) containing 50.0 µM MTX (scan rate: 50 mV/s).</p>
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<p>LSVs of the modified CPE with NiO NSs/IL in 0.1 M phosphate buffer solution (pH 7.0) at different scan rates: 10 mV s<sup>−1</sup> (1), 20 mV s<sup>−1</sup> (2), 40 mV s<sup>−1</sup> (3), 60 mV s<sup>−1</sup> (4), 80 mV s<sup>−1</sup> (5), 100 mV s<sup>−1</sup> (6), 200 mV s<sup>−1</sup> (7), 300 mV s<sup>−1</sup> (8), and 400 mV s<sup>−1</sup> (9). The plot of the peak current vs. Ʋ<sup>1</sup>/<sup>2</sup> (Inset) from 10 mV s<sup>−1</sup> to 400 mV s<sup>−1</sup> containing 50.0 µM MTX.</p>
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<p>Linear sweep voltammogram of the modified CPE with NiO NSs/IL in 0.1 M phosphate buffer solution (pH 7.0) at scan rate 10 mV s<sup>−1</sup>. Inset: Tafel plot (50.0 μM MTX) derived from the rising portion of the voltammogram recorded.</p>
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<p>Chronoamperograms of 0.1 mM (1), 0.7 mM (2), 1.2 mM (3), 2.2 mM (4), and 3.0 mM (5) of MTX at the NiO NSs/IL/CPE sensor. (Inset <b>A</b>): variations of I<sub>p</sub> vs. t<sup>−1/2</sup> taken from chronoamperograms and (Inset <b>B</b>): plot of corresponding slopes against MTX concentration (0.1–3.0 mM).</p>
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<p>DPVs of NiO NSs/IL/CPE in phosphate buffer solution (0.1 M pH 7.0) in the presence of different concentrations of MTX: 0.01 µM (1), 0.1 µM (2), 0.5 µM (3), 1.0 µM (4), 5.0 µM (5), 10.0 µM (6), 20.0 µM (7), 40.0 µM (8), 60.0 µM (9), 80.0 µM (10), 100.0 µM (11), 120.0 µM (12), 140.0 µM (13), and 160.0 µM (14). DPVs were recorded at the following conditions: step potential of 0.01 V, scan rate of 50 mV/s, and pulse amplitude of 0.025 V. The plot of the I<sub>p</sub> vs. various concentrations of MTX (Inset) from 0.01 µM to 160.0 µM.</p>
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19 pages, 10067 KiB  
Article
Research on Composite 3D Well Pattern for Blocky Heavy Oil in Offshore Areas: Transition from Huff-and-Puff to Displacement-Drainage
by Zhigang Geng, Gongchang Wang, Wenqian Zheng, Chunxiao Du, Taotao Ge, Cong Tian and Dawei Wang
Processes 2024, 12(12), 2884; https://doi.org/10.3390/pr12122884 (registering DOI) - 17 Dec 2024
Abstract
In view of the deep burial depth, high formation pressure, and presence of top and bottom water in offshore extra-heavy-oil reservoirs, this paper conducts a study on the production performance and flow field variation law of steam huff-and-puff to steam flooding conversion in [...] Read more.
In view of the deep burial depth, high formation pressure, and presence of top and bottom water in offshore extra-heavy-oil reservoirs, this paper conducts a study on the production performance and flow field variation law of steam huff-and-puff to steam flooding conversion in thick heavy-oil reservoirs based on physical simulation, and analyzes the development effect of the conversion from steam huff-and-puff to steam flooding. On this basis, by comprehensively considering the advantages of gravity-assisted steam flooding and a three-dimensional HHSD well pattern obtained from physical simulation experiments, this paper proposes a well pattern development mode of steam huff-and-puff to composite displacement and drainage, and analyzes the development effect of this well pattern mode using the reservoir numerical simulation method. The research results show that, compared with the planar well pattern of steam huff-and-puff to steam flooding conversion, the adoption of the three-dimensional well pattern can significantly improve the degree of reservoir production and the expansion dynamics of the steam chamber, and mitigate adverse effects such as the increase in water cut caused by top and bottom water on thermal recovery. The composite development of steam huff-and-puff to composite displacement and drainage can be divided into three stages: thermal communication, gravity drainage-assisted steam flooding, and thermal breakthrough erosion and oil washing. The steam chamber presents a development mode of “single-point development–rapid longitudinal expansion–rapid transverse expansion upon reaching the top–polymerization into a sheet”, and simultaneously possesses the oil displacement mechanisms of both steam displacement and gravity drainage. The proposed composite mode of steam huff-and-puff to composite displacement and drainage has guided the implementation of adjustment wells in the Bohai L Oilfield, and the recovery factor has been increased by about 20% compared with the steam huff-and-puff development of the basic well pattern. This study has reference and guiding significance for the efficient thermal recovery development of this oilfield. Full article
(This article belongs to the Special Issue Flow Mechanisms and Enhanced Oil Recovery)
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<p>Cross-sectional diagram of Bohai L oilfield.</p>
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<p>Schematic diagram of the experimental apparatus and process.</p>
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<p>Schematic diagram of well locations in the physical simulation experiment of steam huff-and-puff converted to flooding (side view).</p>
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<p>Characteristics of steam chamber development during the process of conversion from steam huff-and-puff to steam flooding.</p>
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<p>Curves of recovery factor and water cut.</p>
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<p>Well layout diagram of the actual model.</p>
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<p>Schematic diagram of well layout (side view).</p>
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<p>Distribution maps of temperature field and residual oil in different layers under gravity-assisted steam flooding.</p>
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<p>Variation in the expansion speed of the heating chamber at the field scale.</p>
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<p>The curves of the recovery factor and water cut for gravity-assisted steam flooding and HHSD.</p>
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<p>Design of the combined displacement of drainage and flooding three-dimensional well pattern for the target block.</p>
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<p>Numerical simulation model diagram of the target block.</p>
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<p>Production characteristics in different stages of the conversion from steam huff-and-puff to composite displacement and drainage and the corresponding characteristics of the steam chambers.</p>
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<p>Comparison diagram of the recovery factors and steam chambers in the process of conversion from steam huff-and-puff to composite displacement and drainage for different well patterns.</p>
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<p>Comparison field diagram of the sweep of the heating chambers for different well patterns.</p>
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<p>Development effects of the three-dimensional well pattern at different planar well spacings.</p>
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<p>Development effects of the three-dimensional well pattern at different vertical well spacings.</p>
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<p>Development effects of the three-dimensional well pattern at different distances from the bottom water of the reservoir.</p>
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<p>Development effects of the three-dimensional well pattern at different steam injection rates.</p>
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<p>Development effects of the three-dimensional well pattern at different steam qualities.</p>
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<p>Development effects of the three-dimensional well pattern at different production–injection ratios.</p>
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<p>Schematic diagram of the well locations of adjustment wells in the three-dimensional well pattern of Bohai L oilfield.</p>
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<p>Production curves of adjustment wells in the three-dimensional well pattern of Bohai L oilfield.</p>
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15 pages, 3436 KiB  
Article
Assessment of Two Crosslinked Polymer Systems Including Hydrolyzed Polyacrylamide and Acrylic Acid–Hydrolyzed Polyacrylamide Co-Polymer for Carbon Dioxide and Formation Water Diversion Through Relative Permeability Reduction in Unconsolidated Sandstone Formation
by Sherif Fakher, Abdelaziz Khlaifat, Karim Mokhtar and Mariam Abdelsamei
Polymers 2024, 16(24), 3503; https://doi.org/10.3390/polym16243503 (registering DOI) - 17 Dec 2024
Abstract
One of the most challenging aspects of manipulating the flow of fluids in subsurfaces is to control their flow direction and flow behavior. This can be especially challenging for compressible fluids, such as CO2, and for multiphase flow, including both water [...] Read more.
One of the most challenging aspects of manipulating the flow of fluids in subsurfaces is to control their flow direction and flow behavior. This can be especially challenging for compressible fluids, such as CO2, and for multiphase flow, including both water and carbon dioxide (CO2). This research studies the ability of two crosslinked polymers, including hydrolyzed polyacrylamide and acrylic acid/hydrolyzed polyacrylamide crosslinked polymers, to reduce the permeability of both CO2 and formation water using different salinities and permeability values and in the presence of crude oil under different injection rates. The result showed that both polymers managed to reduce the permeability of water effectively; however, their CO2 permeability-reduction potential was much lower, with the CO2 permeability reduction being less than 50% of the water reduction potential in the majority of the experiments. This was mainly due to the high flow rate of the CO2 compared to the water, which resulted in significant shearing of the crosslinked polymer. The crosslinked polymers’ swelling ratios were impacted differently based on the salinity, with the maximum swelling ratio being 9.8. The HPAM polymer was negatively affected by the presence of crude oil, whereas increasing salinity improved its performance greatly. All in all, both polymers had a higher permeability reduction for the formation water compared to CO2 under all conditions. This research can help improve the applicability of CO2-enhanced oil recovery and CO2 storage in depleted oil reservoirs. The ability of the crosslinked polymers to improve CO2 storage will be a main focus of future research. Full article
(This article belongs to the Special Issue Progress in Polymer Networks)
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Figure 1
<p>Synthesized AA/HPAM-crosslinked polymer (yellow) and HPAM-crosslinked polymer (transparent).</p>
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<p>(<b>a</b>) Sandpack experimental setup. (<b>b</b>) Sandpack experimental setup.</p>
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<p>CO<sub>2</sub> permeability reduction for HPAM- and AA/HPAM-crosslinked polymer after one and two injection cycles at different injection rates using 3 Darcy permeability sandpack, 1 wt% polymer, and 1 wt% NaCl.</p>
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<p>CO<sub>2</sub> permeability reduction for HPAM- and AA/HPAM-crosslinked polymers after one and two injection cycles at different injection rates using 3 Darcy permeability sandpack, 1 wt% Polymer, and 10 wt% NaCl.</p>
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<p>CO<sub>2</sub> permeability deduction for HPAM- and AA/HPAM-crosslinked polymers after one and two injection cycles at different injection rates using 18 Darcy permeability sandpack, 1 wt% Polymer, and 1 wt% NaCl.</p>
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<p>CO<sub>2</sub> permeability reduction for HPAM- and AA/HPAM-crosslinked polymers after one and two injection cycles at different injection rates using 3 Darcy permeability sandpack, 1 wt% polymer, 1 wt% NaCl, and 33 cp Crude Oil.</p>
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<p>Water permeability reduction for HPAM- and AA/HPAM-crosslinked polymers after one and two injection cycles at different injection rates using 3 Darcy permeability sandpack, 1 wt% Polymer, and 1 wt% NaCl.</p>
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<p>Water permeability reduction for HPAM- and AA/HPAM-crosslinked polymers after one and two injection cycles at different injection rates using 3 Darcy permeability sandpack, 1 wt% Polymer, and 10 wt% NaCl.</p>
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<p>Water permeability reduction for HPAM- and AA/HPAM-crosslinked polymers after one and two injection cycles at different injection rates using 18 Darcy permeability sandpack, 1 wt% polymer, and 1 wt% NaCl.</p>
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<p>Water permeability reduction for HPAM- and AA/HPAM-crosslinked polymers after one and two injection cycles at different injection rates using 3 Darcy permeability sandpack, 1 wt% polymer, 1 wt% NaCl, and 33 cp crude oil.</p>
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32 pages, 9192 KiB  
Article
Reactivation of Abandoned Oilfields for Cleaner Energy Generation: Three-Dimensional Modelling of Reservoir Heterogeneity and Geometry
by Benjamin Michael Storey, Richard H. Worden, David D. McNamara, John Wheeler, Julian Parker and Andre Kristen
Processes 2024, 12(12), 2883; https://doi.org/10.3390/pr12122883 (registering DOI) - 17 Dec 2024
Abstract
With the changing picture of global energy supplies and the shift toward the energy transition, it has never been more important to look for alternative sources of energy. Globally there are tens of thousands of abandoned oil fields with considerable reserves left behind. [...] Read more.
With the changing picture of global energy supplies and the shift toward the energy transition, it has never been more important to look for alternative sources of energy. Globally there are tens of thousands of abandoned oil fields with considerable reserves left behind. These have the potential to be reactivated to become an energy supply that is cleaner than conventional oil and gas. This can be achieved by the use of in situ combustion and the subsequent exploitation of the inherent increase in temperature and pressure to produce geothermal energy, allied to sequestration of the mixture of produced fluids. In situ combustion (ISC) has conventionally been used as an enhanced oil recovery technique, with a high failure rate that has been recently attributed to poor reservoir selection and project design. We suggest that the failure of many earlier ISC projects is due to insufficient appreciation of how the subsurface geology affects the process. With the use of computer numerical modelling, we aim to ascertain how the geometry and heterogeneity of the reservoir control the success of the process. Here we employ simple three-dimensional sector models to assess a variety of different petrophysical heterogeneities, within a set of different reservoir geometries, on the temperature, velocity, propagation stability and enthalpy rate. These models illustrate that the biggest impact on success of the ISC process for geothermal energy generation, as a function of temperature and enthalpy, is the location of the wells relative to the heterogeneities and the scale of heterogeneities. Metre-scale heterogeneities do not have a significant effect on this. Instead, the biggest contributor to the propagation stability and direction of the fire front is the presence of a large-scale (10 s to 100 s of metres) heterogeneities, such as channels, or the geometry of a tilted fault block; both have a strong control over the direction of the propagation, and therefore are important factors with regards to well placement. Full article
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Figure 1
<p>Relative permeability curves used in all simulations: (<b>a</b>) oil–water relative permeability and (<b>b</b>) liquid–gas relative permeability curves with temperature dependence included [<a href="#B62-processes-12-02883" class="html-bibr">62</a>].</p>
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<p>Viscosity vs. temperature graphs to illustrate how the initial oil viscosity decreases with increasing temperature [<a href="#B64-processes-12-02883" class="html-bibr">64</a>,<a href="#B65-processes-12-02883" class="html-bibr">65</a>].</p>
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<p>Diagrams of each of the different geometries that is used for the model, with injection and production wells marked and depth scale. (<b>a</b>) Base–case cube model without any tectonic structure, (<b>b</b>) periclinal fold with four-way dip closure, (<b>c</b>) tilted fault block dipping at 45°.</p>
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<p>Porosity distribution of the three heterogeneous sub-models (note that the homogeneous model is not represented here). (<b>a</b>) Gaussian distribution of porosity with a mean porosity of 20% and standard deviation of 4; (<b>b</b>) facies-controlled heterogeneity of a single channel of defined orientation that, in this case, is not intersected by the injector or producer wells; (<b>c</b>) layered model with alternating 5% and 20 percent layers. All models’ permeabilities are derived from the Kozeny–Carman relationship (Equation (1)), each sub model is used with each geo-model.</p>
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<p>Oil saturation distribution plots with the fire front marked, for each of the different type A models, no heterogeneity. (<b>a</b>) Model 1-A, homogeneous cube geometry, revealing the development of a wedge-shaped fire front moving more at the top than the base of the structure. (<b>b</b>) Model 2-A, homogeneous periclinal fold, illustrating the development of a wedge-shaped fire front with the majority of the oil bank to the top of the reservoir. (<b>c</b>) Model 3-A, homogenous tilted fault block, revealing a strong preference for the migration of oil up-dip and to the left of the reservoir.</p>
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<p>Graphs of average properties by layer for each homogenous model. (<b>a</b>) Average temperature of six hottest points. (<b>b</b>) Average velocity of the six hottest points. (<b>c</b>) Average propagation angle with respect to the production and injection wells for the six hottest points.</p>
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<p>Oil saturation distribution plots with the fire front marked on for each of the different type B models, with heterogeneous distribution of petrophysical properties. (<b>a</b>) Model 1-B, randomly distributed heterogeneity cube geometry, revealing a distorted fire front moving predominantly to the left of the grid and beginning to split (<b>b</b>) Model 2-B, randomly distributed heterogeneity periclinal fold, revealing a distorted shape to the fire front but moving towards the apex of the structure. (<b>c</b>) Model 3-B, randomly distributed heterogeneity tilted fault block, showing that the fire front preferentially migrates up-dip as well as the formation of a small movement towards the production well.</p>
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<p>Graphs of average properties by layer for each randomly distributed heterogeneity model. (<b>a</b>) Average temperature of six hottest points. (<b>b</b>) Average velocity of the six hottest points. (<b>c</b>) Average propagation angle with respect to the production and injection wells for the six hottest points.</p>
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<p>Oil saturation distribution plots with the fire front marked on for each of the different type C models, facies-controlled (channel) petrophysical heterogeneity. (<b>a</b>) Model 1-C, facies-controlled heterogeneity cube geometry, revealing minor movement of oil to the right-hand side of the upper layers of the reservoir. (<b>b</b>) Model 2-C, facies-controlled periclinal fold, revealing a small displacement of oil around the injection well within the upper layers of the reservoir. (<b>c</b>) Model 3-C, facies-controlled tilted fault block, revealing extinction of the fire front before it could develop and no movement of oil.</p>
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<p>Graphs of average properties by layer for each facies-controlled heterogeneity model. (<b>a</b>) Average temperature of six hottest points. (<b>b</b>) Average velocity of the six hottest points. (<b>c</b>) Average propagation angle with respect to the production and injection wells for the six hottest points.</p>
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<p>Oil saturation distribution plots with the fire front marked on for each of the different type D models, with layered stratigraphic petrophysical heterogeneity. (<b>a</b>) Model 1-D, layered cube geometry, revealing the preferential movement of oil within the higher porosity and permeability layers. (<b>b</b>) Model 2-D, layered periclinal fold, showing the preferential movement of oil within the high-porosity and permeability layers and slight distortions of the fire front within the top layer. (<b>c</b>) Model 3-D, layered tilted fault block, illustrating the preferential movement of oil within the high-porosity and permeability layers and the preferential movement of the fire front up-dip.</p>
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<p>Graphs of average properties by layer for each layered model. (<b>a</b>) Average temperature of the six hottest points. (<b>b</b>) Average velocity of the six hottest points. (<b>c</b>) Average propagation angle with respect to the production and injection wells for the six hottest points.</p>
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<p>Graph to illustrate the cumulative enthalpy of each model when run for a duration of 5 years, not including models 2-A, 3-A, or 3-B, as these models did not run to completion. Given the selected orientation of the channel relative to the injector and producer wells, the facies-controlled heterogeneity models do not develop a significant fire front and do not generate any significant enthalpy after 5 years. The other models generate enthalpy after 5 years, with the cube models generating earlier than others.</p>
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<p>Graph of the temperature difference compared to the base–case cube model to determine the different effects on the peak average temperature when changing the geometry of the reservoir for each heterogeneity. (<b>a</b>) Homogeneous reservoir. (<b>b</b>) Randomly distributed heterogeneity. (<b>c</b>) Facies-controlled (channel) heterogeneity. (<b>d</b>) Layered reservoir.</p>
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<p>Graph of the velocity difference compared to the base–case cube model to ascertain the different effects on the velocity when changing the geometry of the reservoir for each heterogeneity. (<b>a</b>) Homogeneous reservoir. (<b>b</b>) Randomly distributed heterogeneity. (<b>c</b>) Facies-controlled (channel) heterogeneity. (<b>d</b>) Layered reservoir.</p>
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<p>Graph of the propagation angle difference compared to the base–case cube model to ascertain the different effects on the propagation angle when changing the geometry of the reservoir for each heterogeneity. (<b>a</b>) Homogeneous reservoir. (<b>b</b>) Randomly distributed heterogeneity. (<b>c</b>) Facies-controlled (channel) heterogeneity. (<b>d</b>) Layered reservoir.</p>
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<p>Graphs of the temperature difference compared to the base–case homogeneous model to illustrate the different effects of the changing petrophysical heterogeneity for each reservoir geometry. (<b>a</b>) Cube model. (<b>b</b>) Periclinal fold model. (<b>c</b>) Tilted fault block model.</p>
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<p>Graphs of the velocity difference compared to the base–case homogeneous model to illustrate the different effects of the changing petrophysical heterogeneity for each reservoir geometry. (<b>a</b>) Cube model. (<b>b</b>) Periclinal fold model. (<b>c</b>) Tilted fault block model.</p>
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<p>Graphs of the propagation angle difference compared to the base–case homogeneous model to illustrate the different effects of the changing petrophysical heterogeneity for each reservoir geometry. (<b>a</b>) Cube model. (<b>b</b>) Periclinal fold model. (<b>c</b>) Tilted fault block model.</p>
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<p>Box and whisker pots of the difference between the cube and the other geometries, and between the homogeneous reservoir with the heterogeneous reservoirs, showing the interquartile ranges, median average and outliers. (<b>a</b>) Overall effects of temperature. (<b>b</b>) Overall effects on velocity. (<b>c</b>) Overall effects on propagation angle.</p>
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18 pages, 1043 KiB  
Article
The Ongoing Multi-Dimensional Impacts of COVID-19 on Wellbeing: Evidence from a Quasi-Longitudinal Survey in Israel
by Fabian Israel, Danielle Zaychik, Yonat Rein-Sapir, Eran Feitelson, Deborah Shmueli, Alex Altshuler, Pnina Plaut and Eli Salzberger
Sustainability 2024, 16(24), 11042; https://doi.org/10.3390/su162411042 (registering DOI) - 17 Dec 2024
Abstract
During the COVID-19 pandemic, many countries implemented widespread restrictions in an effort to mitigate the spread of the virus. These measures had various impacts on the wellbeing of residents. This study explores the effects of the pandemic on wellbeing across different segments of [...] Read more.
During the COVID-19 pandemic, many countries implemented widespread restrictions in an effort to mitigate the spread of the virus. These measures had various impacts on the wellbeing of residents. This study explores the effects of the pandemic on wellbeing across different segments of the population in Israel, a country that rapidly administered vaccines and eased restrictions. Two online surveys were conducted on a representative sample of the population, one during the peak of the crisis and another 15 months later during the tail end. The analysis, conducted using multivariate statistical methods, revealed that the negative effects on wellbeing observed during the height of the crisis had largely diminished over time. The significant lifestyle changes prompted by the pandemic and governmental responses had mostly short-lived consequences on wellbeing. Yet, social connections continued to exhibit the strongest association with mitigating subjective wellbeing impacts. Additionally, this study found that the gap in wellbeing between disadvantaged and privileged groups widened as the crisis subsided, suggesting that some disasters may have an initial equalizing effect that wears off with time. The results emphasize the importance of considering the wellbeing impacts when implementing public health policies and providing ongoing support, particularly for disadvantaged populations, throughout the recovery period. Full article
(This article belongs to the Section Health, Well-Being and Sustainability)
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<p>Implications of responses to COVID-19 on short-term wellbeing; source: Feitelson et al., 2022 [<a href="#B7-sustainability-16-11042" class="html-bibr">7</a>].</p>
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<p>Life satisfaction by survey.</p>
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<p>Two-step cluster scores. More affected and less affected according to respondents’ profiles.</p>
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<p>Life satisfaction by cluster.</p>
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17 pages, 5358 KiB  
Article
A PDA@ZIF-8-Incorporated PMIA TFN-FO Membrane for Seawater Desalination: Improving Water Flux and Anti-Fouling Performance
by Yu Ma, Rui Jia, Zhen-Liang Xu, Aida Aibulatova, Xiao-Gang Jin, Yin-Xin Fang, Ming-Xiao Zhang and Sun-Jie Xu
Membranes 2024, 14(12), 272; https://doi.org/10.3390/membranes14120272 - 16 Dec 2024
Abstract
Forward osmosis (FO) technology, known for its minimal energy requirements, excellent resistance to fouling, and significant commercial potential, shows enormous promise in the development of sustainable technologies, especially with regard to seawater desalination and wastewater. In this study, we improved the performance of [...] Read more.
Forward osmosis (FO) technology, known for its minimal energy requirements, excellent resistance to fouling, and significant commercial potential, shows enormous promise in the development of sustainable technologies, especially with regard to seawater desalination and wastewater. In this study, we improved the performance of the FO membrane in terms of its mechanical strength and hydrophilic properties. Generally, the water flux (Jw) of polyisophenylbenzamide (PMIA) thin-film composite (TFC)-FO membranes is still inadequate for industrial applications. Here, hydrophilic polydopamine (PDA)@ zeolitic imidazolate frameworks-8 (ZIF-8) nanomaterials and their integration into PMIA membranes using the interfacial polymerization (IP) method were investigated. The impact of PDA@ZIF-8 on membrane performance in both pressure-retarded osmosis (PRO) and forward osmosis (FO) modes was analyzed. The durability and fouling resistance of these membranes were evaluated over the long term. When the amount of ZIF-8@PDA incorporated in the membrane reached 0.05 wt% in the aqueous phase in the IP reaction, the Jw values for the PRO mode and FO mode were 12.09 LMH and 11.10 LMH, respectively. The reverse salt flux (Js)/Jw values for both modes decreased from 0.75 and 0.80 to 0.33 and 0.35, respectively. At the same time, the PRO and FO modes’ properties were stable in a 15 h test. The incorporation of PDA@ZIF-8 facilitated the formation of water channels within the nanoparticle pores. Furthermore, the Js/Jw ratio decreased significantly, and the FO membranes containing PDA@ZIF-8 exhibited high flux recovery rates and superior resistance to membrane fouling. Therefore, PDA@ZIF-8-modified FO membranes have the potential for use in industrial applications in seawater desalination. Full article
(This article belongs to the Section Membrane Applications for Water Treatment)
16 pages, 1724 KiB  
Article
New Materialist Mapping the Lived Experiencing of Trauma in Perinatal and Infant Mental Health
by Emma van Daal and Ariel Moy
Soc. Sci. 2024, 13(12), 682; https://doi.org/10.3390/socsci13120682 - 16 Dec 2024
Abstract
Contemporary therapeutic trauma practice privileges symptom-based models that overlook the potential of materiality and space in trauma healing. The responsibility for recovery is situated in the individual (i.e., the parent). We suggest that trauma and lived experiencing produce and are produced by the [...] Read more.
Contemporary therapeutic trauma practice privileges symptom-based models that overlook the potential of materiality and space in trauma healing. The responsibility for recovery is situated in the individual (i.e., the parent). We suggest that trauma and lived experiencing produce and are produced by the complex relational entanglings of parent, infant, and the dyad with the world. Employing a new materialist orientation to perinatal and infant mental health and trauma, we propose multimodal mapping as an approach that can move with the multisensorial, multidimensional rhythms of trauma and trauma healing as they unfold in a series of now moments; moments that emerge within the context of the parent–infant relationship. This article re-presents the conceptual material and multimodal maps that emerged from our presentation and experiential invitation at the Big Trauma, Big Change Forum, 2024. Organised into two interconnected parts, we begin by emphasising the capacity of multimodal mapping to enable a nuanced translation of lived experiencing for parents and infants, in research and practice, that can transform trauma and potentiate healing. The second part brings focus to a new mapping experiment whereby the audience engaged in a multimodal process of re-configuring the lived experiencing of parent–infant night-time spaces using collage, images, and group process. We include three illustrations of night-time spaces common to parents and infants, exploring the power of materiality, the arts, and objects in transforming the affective, sensory, and embodied affordances that shape mental health. Arts-based mapping interventions can profoundly shape how we understand and respond to trauma, moving us towards a “more-than” conceptualisation of lived experiencing that is sensed and animated in everyday and every “thing” moments. Our hope is to inspire the audience in adopting a relational orientation that innovates new processes of discovery by mapping the human and more-than-human elements involved in parent–infant well-being and the unravelling of trauma. Full article
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<p>Illustrations in situ, 23 March 2024 (digital photograph).</p>
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<p>“Nursery Collage”, author and co-inquirers, 23 March 2024 (aquarelle graphite on paper and mixed media, 42 cm × 29.7 cm).</p>
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<p>“NICU Collage”, author and co-inquirers, 23 March 2024 (aquarelle graphite on paper and mixed media, 42 cm × 29.7 cm).</p>
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<p>‘Nightriders Collage’ author and co-inquirers, 23 March 2024 (aquarelle graphite on paper and mixed media, 42 cm × 29.7 cm).</p>
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21 pages, 5705 KiB  
Article
Effects of DHEA and DHEAS in Neonatal Hypoxic–Ischemic Brain Injury
by Elena Mayer, Ira Winkler, Eva Huber, Martina Urbanek, Ursula Kiechl-Kohlendorfer, Elke Griesmaier and Anna Posod
Antioxidants 2024, 13(12), 1542; https://doi.org/10.3390/antiox13121542 - 16 Dec 2024
Abstract
Neonatal brain injury remains a significant issue with limited treatment options. This study investigates the potential of the endogenous neurosteroid dehydroepiandrosterone (DHEA) and its sulfate ester (DHEAS) as neuroprotective agents, building on evidence of their mechanisms in adult brain injury models. The primary [...] Read more.
Neonatal brain injury remains a significant issue with limited treatment options. This study investigates the potential of the endogenous neurosteroid dehydroepiandrosterone (DHEA) and its sulfate ester (DHEAS) as neuroprotective agents, building on evidence of their mechanisms in adult brain injury models. The primary objective was to evaluate their neuroprotective and anti-oxidative properties in a mouse model of neonatal hypoxic–ischemic brain injury. Using the modified Rice–Vannucci model, brain injury was induced in 7-day-old mouse pups, followed by treatment with various concentrations of DHEA and DHEAS (0.1, 1, and 10 µg/g body weight) via intraperitoneal injection after a 2 h recovery period. Mice were sacrificed after 24 hours for analysis of somatometry, brain injury, apoptosis, microglial activation, and oxidative stress markers (NOX2, 4-HNE, 8-OHdG), along with the anti-oxidant marker SOD1. While no statistically significant effects of DHEA or DHEAS were observed at the tested doses and time points, the absence of toxic or adverse effects highlights their safety profile. These findings provide a foundation for further research into optimizing dosing strategies, timing, and delivery methods. Future studies should refine these variables to maximize neuroprotective efficacy, investigate DHEA(S)’ exact mechanisms of action, and explore their potential for clinical application in neonatal care. Full article
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<p>Representative images of regions of interest (ROI) were captured in two section planes. Whole-brain visualization was conducted at 40× magnification (scale bars = 1000 µm). (<b>a</b>) Occipital section plane: ROI 1: contralateral white matter, ROI 2: ipsilateral white matter, ROI 3: contralateral cortex, ROI 4: ipsilateral cortex, ROI 5: contralateral hippocampus, ROI 6: ipsilateral hippocampus, ROI 7: contralateral thalamus, ROI 8: ipsilateral thalamus. (<b>b</b>) Frontal section plane: ROI 1: contralateral white matter, ROI 2: ipsilateral white matter, ROI 3: contralateral cortex, ROI 4: ipsilateral cortex, ROI 5: contralateral striatum, ROI 6: ipsilateral striatum.</p>
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<p>Flow diagram illustrating the experimental workflow and animal cohort distribution.</p>
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<p>Neuropathological injury assessment. Representative images of Cresyl Violet-stained coronal brain sections displaying hypoxic–ischemic injury in different treatment groups (<b>a</b>–<b>h</b>). Whole-brain visualization was performed using a 40-fold magnification (scale bars = 1000 µm). Two coronal section planes corresponding to coronal level 72 (bregma −1.755 mm, left) and coronal level 44 (bregma 1.045 mm, right) are displayed per brain. Treatment groups are as follows: (<b>a</b>) control 1× PBS, (<b>b</b>) solvent control 1× PBS + DMSO, (<b>c</b>) DHEA 0.1 µg/g bodyweight (bw), (<b>d</b>) DHEA 1 µg/g bw, (<b>e</b>) DHEA 10 µg/g bw, (<b>f</b>) DHEAS 0.1 µg/g bw, (<b>g</b>) DHEAS 1 µg/g bw, (<b>h</b>) DHEAS 10 µg/g bw.</p>
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<p>Representative photomicrographs of activated caspase-3-positive cells in the occipital section plane cortex (CX), white matter (WM), and hippocampus (HC) (coronal level 72, bregma −1.755 mm). Arrows indicate positive cells. Visualization was performed using a 100-fold (scale bar = 50 µm) (<b>a</b>) and 200-fold magnification (scale bar = 20 μm) (<b>b</b>).</p>
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<p>Representative photomicrographs of activated Iba1-positive microglial cells in the occipital section plane cortex (coronal level 72, bregma −1.755 mm). Visualization was performed using a 200-fold (scale bar = 50 µm) magnification.</p>
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<p>Microglial activation in different brain regions in the occipital (<b>a</b>) and frontal (<b>b</b>) section plane. Occipital section plane (<b>a</b>) corresponds to coronal level 72 (bregma −1.755 mm). Frontal section plane (<b>b</b>) corresponds to coronal level 44 (bregma 1.045 mm). Numbers in the different treatment groups indicate concentrations in µg/g bodyweight. Center lines in the boxes represent medians, box edges mark 1st and 3rd quartiles, and whiskers indicate 10th and 90th percentiles. No overall significant differences in microglial cell activation in the analyzed brain regions were detected (Kruskal–Wallis test, all <span class="html-italic">p</span> &gt; 0.05). Animals per group: n = 6.</p>
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<p>Microglial activation in different brain regions in the occipital (<b>a</b>) and frontal (<b>b</b>) section plane. Occipital section plane (<b>a</b>) corresponds to coronal level 72 (bregma −1.755 mm). Frontal section plane (<b>b</b>) corresponds to coronal level 44 (bregma 1.045 mm). Numbers in the different treatment groups indicate concentrations in µg/g bodyweight. Center lines in the boxes represent medians, box edges mark 1st and 3rd quartiles, and whiskers indicate 10th and 90th percentiles. No overall significant differences in microglial cell activation in the analyzed brain regions were detected (Kruskal–Wallis test, all <span class="html-italic">p</span> &gt; 0.05). Animals per group: n = 6.</p>
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<p>Relative SOD1 expression across treatment groups. Numbers in the different treatment groups indicate concentrations in µg/g bodyweight. (<b>a</b>) Truncated violin plots depict the distribution of relative SOD1 expression levels in different treatment groups in the cytosolic protein fractions of the contralateral and the ipsilateral hemispheres, with the control group set to 1 (dotted line). The width of the violins corresponds to the frequency of observations at each expression level. The extreme tails of the distributions were truncated to highlight the central portion of the data, emphasizing the median (dashed lines), the interquartile range (black lines), and the overall shape of the distribution. The control group serves as the baseline for comparison, and its distribution is centered around 1. Number of pooled samples per group: n = 3–4. (<b>b</b>) Exemplary Western blots showing SOD1 reactivity in different treatment groups in the contralateral (left) and ipsilateral hemisphere (right). β-Actin served as a loading control.</p>
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<p>Relative NOX2 expression across treatment groups. Numbers in the different treatment groups indicate concentrations in µg/g bodyweight. (<b>a</b>) Truncated violin plots depict the distribution of relative NOX2 expression levels in different treatment groups in cytosolic protein fractions of the contralateral and the ipsilateral hemispheres, with the control group set to 1 (dotted line). The width of the violins corresponds to the frequency of observations at each expression level. The extreme tails of the distributions were truncated to highlight the central portion of the data, emphasizing the median (dashed lines), the interquartile range (black lines), and the overall shape of the distribution. The control group serves as the baseline for comparison, and its distribution is centered around 1. Number of pooled samples per group: n = 3–4. (<b>b</b>) Exemplary Western blots showing NOX2 reactivity in different treatment groups in the contralateral (left) and ipsilateral hemispheres (right). β-Actin served as a loading control.</p>
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<p>Plasma concentrations of oxidative stress markers 4-HNE (<b>a</b>) and 8-OHdG (<b>b</b>). Numbers in the different treatment groups indicate concentrations in µg/g bodyweight. Center lines in the boxes represent medians, box edges mark 1st and 3rd quartiles, and whiskers indicate 10th and 90th percentiles. (<b>a</b>) No overall significant differences in 4-HNE plasma concentrations were detected. Number of pooled samples per group: n = 5–6. (<b>b</b>) No overall significant differences in 8-OHdG plasma levels were detected. Number of pooled samples per group: n = 6–8.</p>
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22 pages, 3915 KiB  
Review
Graphene Oxide and Reduced Graphene Oxide Saturable Absorbers: Advancements in Erbium-Doped Fiber Lasers for Mode-Locking and Q-Switching
by Tahani A. Alrebdi, Noor Fatima, Ali M. Alshehri, Adnan Khalil and Haroon Asghar
Photonics 2024, 11(12), 1181; https://doi.org/10.3390/photonics11121181 - 16 Dec 2024
Abstract
Graphene oxide (GO) and reduced graphene oxide (rGO) have emerged as robust materials in the development of SAs for erbium-doped fiber lasers (EDFLs). Their exceptional optical properties, such as broadband absorption and fast recovery times, make them ideal candidates for achieving ultrashort pulse [...] Read more.
Graphene oxide (GO) and reduced graphene oxide (rGO) have emerged as robust materials in the development of SAs for erbium-doped fiber lasers (EDFLs). Their exceptional optical properties, such as broadband absorption and fast recovery times, make them ideal candidates for achieving ultrashort pulse operation in EDFLs. With its higher oxygen content, GO offers greater nonlinearity and a tunable absorption spectrum, while rGO, yielded through chemical reduction, exhibits enhanced electrical conductivity and higher saturable absorption. These properties facilitate the generation of ultrashort pulses in EDFLs, which are highly desired for various medical imaging, telecommunications, and material processing applications. This review paper comprehensively analyzes the advancements in GO and rGO SAs in the context of EDFLs for mode-locking and Q-switching applications. The performance of EDFLs utilizing GO and rGO SAs is critically evaluated, focusing on key parameters, such as modulation depth, pulse duration, repetition rate, average power, pulse energy, peak power, and signal-to-noise ratio. Additionally, this review delves into the various synthesis methods of GO and rGO thin film, highlighting their impact on the optical properties and performance of SAs. The discussion on techniques to integrate the SAs into laser cavities includes direct deposition of nanoparticles/thin-film-based SAs, tapered-fiber-based SAs, and D-shaped SAs. Furthermore, the paper explores the challenges encountered during the fabrication of ideal GO and rGO SAs, with issues related to uniformity, stability, and tunability, along with proposed solutions to address these challenges. The insights provided offer valuable guidance for future research aimed at enhancing the performance of EDFLs using GO/rGO SAs. Full article
(This article belongs to the Special Issue The Emerging Science in Microstructured Optical Fibers)
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<p>Evolution of EDFLs showing significant advancements in materials, techniques, and applications over time.</p>
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<p>Schematic diagram of the synthesis of GO using the Hummer’s method technique.</p>
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<p>Schematic diagram of the synthesis of rGO using the modified Hummer’s method technique.</p>
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<p>(<b>a</b>) Fiber ferrule without SA deposition. (<b>b</b>) Fiber ferrule with GO nanoparticle-based SA.</p>
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<p>(<b>a</b>) Fiber ferrule without SA deposition. (<b>b</b>) Fiber ferrule with GO thin-film-based SA.</p>
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<p>Schematics of the tapered optical fiber.</p>
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<p>Schematics of the D-shaped optical fiber.</p>
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<p>Schematic of the experimental setup of a Q-switched EDFL.</p>
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<p>Schematic of the experimental setup of a mode-locked EDFL.</p>
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28 pages, 2124 KiB  
Article
ElasticPay: Instant Peer-to-Peer Offline Extended Digital Payment System
by Annapureddy Venkata Sai Kumar Reddy and Gourinath Banda
Sensors 2024, 24(24), 8034; https://doi.org/10.3390/s24248034 (registering DOI) - 16 Dec 2024
Abstract
The widespread reliance on paper-based currency poses significant drawbacks, such as counterfeiting, lack of transparency, and environmental impacts. While Central Bank Digital Currencies (CBDCs) address many of these issues, their dependence on continuous internet connectivity limits their usability in scenarios with poor or [...] Read more.
The widespread reliance on paper-based currency poses significant drawbacks, such as counterfeiting, lack of transparency, and environmental impacts. While Central Bank Digital Currencies (CBDCs) address many of these issues, their dependence on continuous internet connectivity limits their usability in scenarios with poor or no network access. To overcome such limitations, this paper introduces ElasticPay, a novel Peer-to-Peer (P2P) Offline Digital Payment System that leverages advanced hardware security measures realised through Trusted Platform Modules (TPMs), Trusted Execution Environments (TEEs), and Secure Elements (SEs). ElasticPay ensures transaction privacy, unforgeability, and immediate settlement while preventing double spending. Our approach integrates robust recovery mechanisms and provides a scalable solution for diverse environments. Extensive experimentation validates the system’s reliability and practicality, highlighting its potential to advance secure and inclusive CBDC ecosystems. We demonstrate the proposed solution implementation on the iPhone mobilephone because it has an inbuilt Secure Enclave, which is an integrated implementation of the necessary TPM, TEE, and SE functionalities. Full article
15 pages, 1824 KiB  
Article
Assessment of Gravity Deportment of Gold-Bearing Ores: Gravity Recoverable Gold Test
by Oldřich Šigut, Tomáš Široký, Iva Janáková, Radek Střelecký and Vladimír Čablík
Minerals 2024, 14(12), 1279; https://doi.org/10.3390/min14121279 - 16 Dec 2024
Abstract
This study investigated the potential of low-grade gold deposits in modern mining, particularly in the context of declining high-grade resources. The primary method for processing these ores was gravity separation with the Knelson concentrator. A GRG test (gravity recoverable gold test) was conducted [...] Read more.
This study investigated the potential of low-grade gold deposits in modern mining, particularly in the context of declining high-grade resources. The primary method for processing these ores was gravity separation with the Knelson concentrator. A GRG test (gravity recoverable gold test) was conducted on two gold-bearing samples: a polymetallic Cu-Zn-Au ore from Zlaté Hory–Západ (Czech Republic) containing refractory gold and an ore with free gold from Kašperské Hory (Czech Republic). The study evaluated the effectiveness of the GRG test for gold recovery from these ores. The results showed that the Kašperské Hory sample predominantly contained relatively large gold grains, with recovery rates dropping significantly upon finer comminution. In the sample from the Zlaté Hory–Západ deposit, the greatest GRG release occurred in the first and last test stages, suggesting that larger sulfide grains with bound gold passed predominantly in the first stage, while fine gold with residual sulfides passed in the third. Both samples achieved high overall GRG recovery rates, with 64.2% for Kašperské Hory and more than 66% for Zlaté Hory–Západ, demonstrating the efficacy of centrifugal concentrators for both ores. Full article
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<p>A procedural flow sheet for the GRG test.</p>
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<p>Microstructure of the input sample from Kašperské Hory (SEM and microanalysis).</p>
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<p>Recovery of gold by concentration stage (Kašperské Hory).</p>
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<p>Microstructure of the input sample from Zlaté Hory–Západ (SEM and microanalysis).</p>
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<p>Recovery of gold by concentration stage (Zlaté Hory–Západ).</p>
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14 pages, 4119 KiB  
Article
Fluorescently Tagged Poly(methyl methacrylate)s
by Fabia Grisi, Rubina Troiano, Donatella Fiore, Patrizia Gazzerro, Mariateresa Lettieri, Vincenzo Venditto and Stefania Pragliola
Molecules 2024, 29(24), 5940; https://doi.org/10.3390/molecules29245940 - 16 Dec 2024
Abstract
Plastic pollution is a global problem affecting the environment and, consequently, people’s well-being. Careful and timely end-of-life plastic recycling is certainly a way, albeit a partial one, to remedy the problem. The immediate identification and selection of the different types of plastic materials [...] Read more.
Plastic pollution is a global problem affecting the environment and, consequently, people’s well-being. Careful and timely end-of-life plastic recycling is certainly a way, albeit a partial one, to remedy the problem. The immediate identification and selection of the different types of plastic materials in the recycling process certainly facilitate its recovery and reuse, allowing the damage caused by plastic emission into the environment to be limited. Recently, new technologies for automatic sorting of plastics based upon fluorescent tagging have been considered. This article reports the synthesis and characterization of fluorescent copolymers of poly(methyl methacrylate) (PMMA) that could be potentially used as fluorescent markers of commercial PMMA. Poly(methylmetacrylate-co-2-(9-carbazolyl)ethyl methacrylate) (P(MMA-co-CEMA)) and poly(methylmetacrylate-co-7-methacryloyloxycoumarin) (P(MMA-co-MAOC)) samples containing a small number of fluorescent units (<4%) were synthesized by free-radical polymerization. All copolymer samples show chemico-physical properties like those of pure PMMA and produce fluorescence emission under 290 nm wavelength excitation. P(MMA-co-CEMA)s and P(MMA-co-MAOC)s were also tested as fluorescent dyes for PMMA identification. The experimental results demonstrate that PMMA/P(MMA-co-CEMA) and PMMA/P(MMA-co-MAOC) blends prepared using 1% by weight of fluorescent copolymer show a homogeneous morphology completely similar to pure PMMA and are still optically active. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Macromolecular Chemistry)
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<p><sup>13</sup>C NMR spectrum of run <b>3</b> (CDCl<sub>3</sub> solvent, TMS scale, 25 °C).</p>
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<p><sup>13</sup>C NMR spectrum of run <b>6</b> (CDCl<sub>3</sub> solvent, TMS scale, 25 °C).</p>
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<p>The 600 MHz 2D DOSY NMR spectrum of run <b>3</b> (CDCl<sub>3</sub> solvent, TMS scale, 25 °C).</p>
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<p>The 600 MHz 2D DOSY NMR spectrum of run <b>6</b> (CDCl<sub>3</sub> solvent, TMS scale, 25 °C).</p>
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<p>X-ray diffraction patterns of runs <b>1</b>–<b>6</b> from <a href="#molecules-29-05940-t001" class="html-table">Table 1</a> and amorphous PMMA sample.</p>
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<p>DSC curves (second heating run) of runs <b>1</b>–<b>6</b> from <a href="#molecules-29-05940-t001" class="html-table">Table 1</a>.</p>
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<p>UV-vis absorption and emission spectra (Λ<sub>ecc</sub> = 290 nm) of run <b>3</b> in solution and solid state.</p>
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<p>UV-vis absorption and emission spectra (Λ<sub>ecc</sub> = 290 nm) of run <b>6</b> in solution and solid state.</p>
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<p>SEM micrographs of (<b>A</b>) pure PMMA, (<b>B</b>) PMMA/P(MMA-co-CEMA) blend, and (<b>C</b>) PMMA/P(MMA-co-MAOC) blend films.</p>
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<p>Emission spectra of the PMMA/P(MMA-<span class="html-italic">co</span>-CEMA) and PMMA/P(MMA-<span class="html-italic">co</span>-MAOC) blends containing 1% by weight of P(MMA-<span class="html-italic">co</span>-CEMA) and P(MMA-<span class="html-italic">co</span>-MAOC), respectively (Λ<sub>ecc</sub> = 290 nm).</p>
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<p>Representative images of P(MMA-<span class="html-italic">co</span>-CEMA), PMMA/P(MMA-<span class="html-italic">co</span>-CEMA) blend, P(MMA-<span class="html-italic">co</span>-MAOC), and PMMA/P(MMA-<span class="html-italic">co</span>-MAOC) blend fluorescence properties. In (<b>a</b>) and (<b>c</b>), brightfield images are shown. Panels (<b>b</b>) and (<b>d</b>) show blue fluorescence (analyzed with DAPI filters: 340–360 nm excitation range and 440–460 nm emission range). Scale bars in (<b>a</b>) and (<b>b</b>) = 1000 µm; scale bars in (<b>c</b>) and (<b>d</b>) = 200 µm.</p>
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<p>PE (<b>a</b>), PP (<b>b</b>), and PS (<b>c</b>) fluorescent copolymer structures as reported in Refs. [<a href="#B16-molecules-29-05940" class="html-bibr">16</a>,<a href="#B17-molecules-29-05940" class="html-bibr">17</a>].</p>
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<p>Copolymer synthesis.</p>
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25 pages, 11059 KiB  
Article
The Design and Application of a Regional Management Model to Set Up Wind Farms and the Adaptation to Climate Change Effects—Case of La Coruña (Galicia, Northwest of Spain)
by Blanca Valle, Javier Velázquez, Derya Gülçin, Fernando Herráez, Ali Uğur Özcan, Ana Hernando, Víctor Rincón, Rui Alexandre Castanho and Kerim Çiçek
Land 2024, 13(12), 2201; https://doi.org/10.3390/land13122201 - 16 Dec 2024
Abstract
The implantation of wind farms in the European territory is being deployed at an accelerated pace. In the proposed framework, the province of La Coruña in the autonomous community of Galicia is tested, with a wide deployment of this type of infrastructure in [...] Read more.
The implantation of wind farms in the European territory is being deployed at an accelerated pace. In the proposed framework, the province of La Coruña in the autonomous community of Galicia is tested, with a wide deployment of this type of infrastructure in the territory initiated in the 80s, representing the third autonomous community with the largest exploitation of wind resources, which provides sufficient information, extrapolated to the entire community, to demonstrate the practical usefulness and potential of the method of obtaining the territorial model proposed in this article The regional has been used as the basic administrative subunit of the study variables, considering that the territory thus delimited could have common physical and cultural characteristics. The methodology presented in this article involves the collection and processing of public cartographic data on various factors most repeatedly or agreed upon in the consulted bibliography based on studies by experts in the technical, environmental, and environmental areas, including explanatory variables of risk in a broader context of climate change as the first contribution of this study. Another contribution is the inclusion in the model of the synergistic impact measured as the distance to wind farms in operation (21% of the total area of the sample) to which an area of influence of 4 times the rotor diameter of each of the wind turbines im-planted has been added as a legal and physical restriction. On a solid basis of selection of explanatory variables and with the help of Geographic Information Systems (GIS) and multi-criteria analysis (MCDM), techniques widely documented in the existing literature for the determination of optimal areas for the implementation of this type of infrastructure, a methodological proposal is presented for the development of a strategic, long-term territorial model, for the prioritization of acceptable areas for the implementation of wind farms, including forecasts of increased energy demand due to the effect of climate change and the population dynamics of the study region that may influence energy consumption. This article focuses on the use of multivariate clustering techniques and spatial analysis to identify priority areas for long-term sustainable wind energy projects. With the proposed strategic territorial model, it has been possible to demonstrate that it is not only capable of discriminating between three categories of acceptable areas for the implementation of wind farms, taking into account population and climate change forecasts, but also that it also locates areas that could require conservationist measures to protect new spaces or to recover the soil because they present high levels of risk due to natural or anthropic disasters considered. The results show acceptable areas for wind energy implementation, 23% of the total area of the sample, 3% conservation as ecological spaces to be preserved, and 7% recovery due to high-risk rates. The findings show that coastal regions generally show a more positive carrying capacity, likely due to less dense development or regulatory measures protecting these areas. In contrast, certain inland regions show more negative values, suggesting these areas might be experiencing higher ecological disturbance from construction activities. This information highlights the importance of strategic site analysis to balance energy production with conservation needs. The study provides insights into wind farm deployment that considers the visual and ecological characteristics of the landscape, promoting sustainability and community acceptance. For this reason, these insights can be effectively used for advancing renewable energy infrastructures within the European Union’s energy transition goals, particularly under the climate and energy objectives set for 2030. Full article
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<p>Geographical location of the study area.</p>
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<p>Methodological flowchart.</p>
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<p>Presents four bar charts compare judgments across different groups for the formation of models in four distinct blocks: skills, risks, impact, and climate change. Each chart contrasts the average scores given by two areas: the Impact, Risk, and Climate Change Area (green bars) and the Constructive Area (yellow bars). The first chart examines the skills block, where group A1 stands out with the highest score from the Impact, Risk, and Climate Change Area, significantly surpassing the Constructive Area’s score. Other groups, such as A2, A3, A4, and A5, show a more balanced assessment between the two areas, with slight variances, but no other group exhibits a stark difference like A1. In the risks block, there is a noticeable divergence in the judgments between the groups. RIE1 receives the highest score from the Impact, Risk, and Climate Change Area, while the Constructive Area gives RIE4 the highest score. The other groups (RIE2, RIE3, and RIE5) display varied judgments, with RIE3 and RIE4 showing relatively higher scores from the Constructive Area compared to the Impact, Risk, and Climate Change Area, indicating a more favorable assessment of risks by the Constructive Area. The impact block chart reveals that group I2 receives the highest score from the Impact, Risk, and Climate Change Area, which is significantly higher than the score given by the Constructive Area. Other groups, such as I1, I3, and I4, show closer scores between the two areas, but I3 and I4 receive marginally higher scores from the Constructive Area, suggesting a slight preference in their impact assessment. In the climate change block, CC5 is rated significantly higher by the Impact, Risk, and Climate Change Area compared to the Constructive Area. Groups CC1, CC2, CC3, and CC4 show more varied results, with CC4 receiving a higher score from the Constructive Area and CC3 showing a balanced assessment from both areas.</p>
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<p>Carrying capacity of the ecosystems of the province of La Coruña for construction.</p>
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<p>Model of climate change for construction in the province of La Coruña.</p>
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<p>Territorial model by management categories.</p>
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18 pages, 3357 KiB  
Article
Deep Eutectic Solvent (TOPO/D2EHPA/Menthol) for Extracting Metals from Synthetic Hydrochloric Acid Leachates of NMC-LTO Batteries
by Arina V. Kozhevnikova, Nikita A. Milevskii, Dmitriy V. Lobovich, Yulia A. Zakhodyaeva and Andrey A. Voshkin
Metals 2024, 14(12), 1441; https://doi.org/10.3390/met14121441 - 16 Dec 2024
Abstract
The recycling of lithium-ion batteries is increasingly important for both resource recovery and environmental protection. However, the complex composition of cathode and anode materials in these batteries makes the efficient separation of metal mixtures challenging. Hydrometallurgical methods, particularly liquid extraction, provide an effective [...] Read more.
The recycling of lithium-ion batteries is increasingly important for both resource recovery and environmental protection. However, the complex composition of cathode and anode materials in these batteries makes the efficient separation of metal mixtures challenging. Hydrometallurgical methods, particularly liquid extraction, provide an effective means of separating metal ions, though they require periodic updates to their extraction systems. This study introduces a hydrophobic deep eutectic solvent composed of trioctylphosphine oxide, di(2-ethylhexyl)phosphoric acid, and menthol, which is effective for separating Ti(IV), Co(II), Mn(II), Ni(II), and Li+ ions from hydrochloric acid leachates of NMC (LiNixMnyCo1−x−yO2) batteries with LTO (Li4Ti5O12) anodes. By optimising the molar composition of the trioctylphosphine oxide/di(2-ethylhexyl)phosphoric acid/menthol mixture to a 4:1:5 ratio, high extraction efficiency was achieved. The solvent demonstrated stability over 10 cycles, and conditions for its regeneration were successfully established. At room temperature, the DES exhibited a density of 0.89 g/mL and a viscosity of 56 mPa·s, which are suitable for laboratory-scale extraction processes. Experimental results from a laboratory setup with mixer-settlers confirmed the efficiency of separating Ti(IV) and Co(II) ions in the context of their extraction kinetics. Full article
(This article belongs to the Section Extractive Metallurgy)
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<p>A photo and scheme of a laboratory installation in operation: <span class="html-italic">a</span>—raffinate solution, <span class="html-italic">b</span>—extract solution, <span class="html-italic">c</span>—initial solution with appropriate metal concentration and HCl, <span class="html-italic">d</span>—HDES, P—pump, E—extractor.</p>
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<p>Dependence of density (<b>a</b>) and dynamic viscosity (<b>b</b>) of the HDES composed of TOPO/D2EHPA/menthol in a 4:1:5 ratio on temperature.</p>
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<p>Dependence of the degree of extraction of metal ions on the menthol content in the HDES. HDES phase: χ<sub>TOPO</sub>/χ<sub>D2EHPA</sub> = 1:1. Aqueous phase: [HCl] = 8 mol/L; V<sub>aq</sub>/V<sub>HDES</sub> = 1/1; mixing time was 30 min.</p>
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<p>The dependence of the degree of extraction of metal ions on the content of TOPO and D2EHPA in the HDES. HDES phase: χ<sub>menthol</sub> = 4. Aqueous phase: [HCl] = 8 mol/L, 0.069 g/L Li, 0.589 g/L Co, 0.587 g/L Ni, 0.549 g/L Mn, and 0.479 g/L Ti; V<sub>aq</sub>/V<sub>HDES</sub> = 1/1; mixing time was 30 min.</p>
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<p>Dependence of the degree of metal ion extraction on the molar fraction of D2EHPA. Aqueous phase: [HCl] = 8 mol/L, 0.069 g/L Li, 0.589 g/L Co, 0.587 g/L Ni, 0.549 g/L Mn, and 0.479 g/L Ti. HDES phase: χ<sub>TOPO</sub> = 4; V<sub>aq</sub>/V<sub>HDES</sub> = 1/1; mixing time was 30 min.</p>
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<p>Dependence of the degree of extraction of metal ions on the phase contact time. HDES phase: TOPO/D2EHPA/menthol = 4:1:5. Aqueous phase: [HCl] = 6 mol/L, 0.069 g/L Li, 0.589 g/L Co, 0.587 g/L Ni, 0.549 g/L Mn, and 0.479 g/L Ti; V<sub>aq</sub>/V<sub>HDES</sub> = 1/1.</p>
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<p>The dependence of the degree of extraction of metal ions on the concentration of HCl. HDES phase: TOPO/D2EHPA/menthol = 4:1:5. Aqueous phase: 0.069 g/L Li, 0.589 g/L Co, 0.587 g/L Ni, 0.549 g/L Mn, and 0.479 g/L Ti; V<sub>aq</sub>/V<sub>HDES</sub> = 1/1; mixing time was 30 min.</p>
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<p>Dependence of the degree of extraction of metal ions on the volume ratio of the aqueous and organic phases. HDES phase: TOPO/D2EHPA/menthol = 4:1:5. Aqueous phase: 0.069 g/L Li, 0.589 g/L Co, 0.587 g/L Ni, 0.549 g/L Mn, and 0.479 g/L Ti; mixing time was 30 min.</p>
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<p>Isotherms of the Me extraction with TOPO/D2EHPA/menthol = 4:1:5. Aqueous phase: [HCl] = 1, 6, 9 mol/L for Ti(IV), Co(II), and Mn(II) ions, respectively; V<sub>aq</sub>/V<sub>HDES</sub> = 1/1; mixing time was 30 min.</p>
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<p>Dependence of the degree of stripping of Ti(IV), Co(II), and Mn(II) ions on the phase contact time. Extraction conditions for Ti(IV), Co(II), and Mn(II): [HCl] = 1, 6, and 9 mol/L, respectively. Stripping conditions for Ti(IV): [H<sub>3</sub>PO<sub>4</sub>] = 3 mol/L, 3 vol.% H<sub>2</sub>O<sub>2</sub>; for Co(II) and Mn(II): [HCl] = 1 mol/L.</p>
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<p>The possibility of the reuse of TOPO/D2EHPA/menthol 4:1:5. Conditions for the stripping of Ti(IV): [H<sub>3</sub>PO<sub>4</sub>] = 3 mol/L, 3 vol.% H<sub>2</sub>O<sub>2</sub>; Co(II) and Mn(II) ions: [HCl] = 1 mol/L.</p>
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<p>Dependence of the degree of extraction of metals from HCl 1 mol/L solution (<b>a</b>) and Co(II) and Mn(II) from HCl 6 mol/L solution (<b>b</b>) on the volume flow rate of the phases.</p>
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