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16 pages, 4400 KiB  
Article
White Matter Microstructural Alterations in Type 2 Diabetes: A Combined UK Biobank Study of Diffusion Tensor Imaging and Neurite Orientation Dispersion and Density Imaging
by Abdulmajeed Alotaibi, Mostafa Alqarras, Anna Podlasek, Abdullah Almanaa, Amjad AlTokhis, Ali Aldhebaib, Bader Aldebasi, Malak Almutairi, Chris R. Tench, Mansour Almanaa, Ali-Reza Mohammadi-Nejad, Cris S. Constantinescu, Rob A. Dineen and Sieun Lee
Medicina 2025, 61(3), 455; https://doi.org/10.3390/medicina61030455 (registering DOI) - 6 Mar 2025
Abstract
Background and objectives: Type 2 diabetes mellitus (T2DM) affects brain white matter microstructure. While diffusion tensor imaging (DTI) has been used to study white matter abnormalities in T2DM, it lacks specificity for complex white matter tracts. Neurite orientation dispersion and density imaging (NODDI) [...] Read more.
Background and objectives: Type 2 diabetes mellitus (T2DM) affects brain white matter microstructure. While diffusion tensor imaging (DTI) has been used to study white matter abnormalities in T2DM, it lacks specificity for complex white matter tracts. Neurite orientation dispersion and density imaging (NODDI) offers a more specific approach to characterising white matter microstructures. This study aims to explore white matter alterations in T2DM using both DTI and NODDI and assess their association with disease duration and glycaemic control, as indicated by HbA1c levels. Methods and Materials: We analysed white matter microstructure in 48 tracts using data from the UK Biobank, involving 1023 T2DM participants (39% women, mean age 66) and 30,744 non-T2DM controls (53% women, mean age 64). Participants underwent 3.0T multiparametric brain imaging, including T1-weighted and diffusion imaging for DTI and NODDI. We performed region-of-interest analyses on fractional anisotropy (FA), mean diffusivity (MD), axial diffusivity (AD), radial diffusivity (RD), orientation dispersion index (ODI), intracellular volume fraction (ICVF), and isotropic water fraction (IsoVF) to assess white matter abnormalities. Results: We observed reduced FA and ICVF, and increased MD, AD, RD, ODI, and IsoVF in T2DM participants compared to controls (p < 0.05). These changes were associated with longer disease duration and higher HbA1c levels (0 < r ≤ 0.2, p < 0.05). NODDI identified microstructural changes in white matter that were proxies for reduced neurite density and disrupted fibre orientation, correlating with disease progression and poor glucose control. In conclusion, NODDI contributed to DTI in capturing white matter differences in participants with type 2 diabetes, suggesting the feasibility of NODDI in detecting white matter alterations in type 2 diabetes. Type 2 diabetes can cause white matter microstructural abnormalities that have associations with glucose control. Conclusions: The NODDI diffusion model allows the characterisation of white matter neuroaxonal pathology in type 2 diabetes, giving biophysical information for understanding the impact of type 2 diabetes on brain microstructure. Future research should focus on the longitudinal tracking of these microstructural changes to better understand their potential as early biomarkers for cognitive decline in T2DM. Full article
(This article belongs to the Section Neurology)
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Figure 1
<p>Flowchart of the included study sample based on the study inclusion/exclusion criteria.</p>
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<p>(<b>A</b>) Violin plots for the fornix as a selected white matter tract (from the de-confounded dataset) with a larger effect size to visualise the intergroup DTI and NODDI-based white matter alterations in patients with T2DM (<span class="html-italic">p</span> &lt; 0.05, false discovery rate adjustment). (<b>B</b>) Global alterations with the effect sizes of each measure in each tract over the whole brain. Genu of corpus callosum (GCC), fornix, cingulate of gyrus, superior longitudinal fasciculus (SLF), anterior corona radiata (ACR), anterior limb of the internal capsule (ALIC), posterior limb of the internal capsule (PLIC), posterior thalamic radiation (PTR), tapetum, splenium of corpus callosum (SCC), external capsule (EC), and retro-lenticular part of the internal capsule (RPIC).</p>
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<p>The right tapetum is a selected white matter tract from the de-confounded dataset to visualise the association between the white matter change detected by DTI/NODDI and the metabolic profile. (<b>A</b>) Association between white matter alterations in the right tapetum and disease duration; (<b>B</b>) Association between white matter alterations in the right tapetum and HbA1c.</p>
Full article ">Figure 3 Cont.
<p>The right tapetum is a selected white matter tract from the de-confounded dataset to visualise the association between the white matter change detected by DTI/NODDI and the metabolic profile. (<b>A</b>) Association between white matter alterations in the right tapetum and disease duration; (<b>B</b>) Association between white matter alterations in the right tapetum and HbA1c.</p>
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<p>Correlations between disease duration and HbA1c with major white matter tracts in participants with T2DM. White matter structures were selected only for visualisation purposes. (<b>A</b>) White matter tracts included. (<b>B</b>) Altered ICVF and disease duration/HbA1c. (<b>C</b>) Altered ODI and disease duration/HbA1c. (<b>D</b>) Altered IsoVF and disease duration/HbA1c. Red: positive correlation; blue: negative correlation. These illustrated correlations are based on a brain model derived from a white matter atlas.</p>
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22 pages, 795 KiB  
Article
Determination and Comparison of Fat and Fibre Contents in Gluten-Free and Gluten-Containing Flours and Breads: Nutritional Implications
by María Purificación González, Paloma López-Laiz, María Achón, Rocío de la Iglesia, Violeta Fajardo, Ángela García-González, Natalia Úbeda and Elena Alonso-Aperte
Foods 2025, 14(5), 894; https://doi.org/10.3390/foods14050894 (registering DOI) - 5 Mar 2025
Abstract
The absence of gluten is a technological challenge that requires the addition of components to replace the unique viscoelastic properties of gluten, thus altering the nutritional composition of gluten-free (GF) breads. Moreover, GF flours may have different compositions as compared to gluten-containing (GC) [...] Read more.
The absence of gluten is a technological challenge that requires the addition of components to replace the unique viscoelastic properties of gluten, thus altering the nutritional composition of gluten-free (GF) breads. Moreover, GF flours may have different compositions as compared to gluten-containing (GC) counterparts because of a different origin. This may impact the nutritional quality of GF diets. The aim of the study is to provide updated analytical data on moisture, fat, and fibre contents in GF flour and bread samples, and compare them with their GC counterparts, as well as to analyse ingredients and how they impact nutritional quality. A total of 30 different flours and 24 types of bread were analysed using AOAC methods. GF cereal flours contain more fat than GC flours (3.5 ± 2.1% vs. 2.5 ± 2.1%, p < 0.001), as well as GF flours from pseudocereals, except for wholemeal buckwheat (2.6 ± 0.1%). Fibre content is lower in GF flours (3.6 ± 3.1% vs. 7.1 ± 3.9%, p = 0.03), except for GF pseudocereal and legume flours. GF breads contain almost twice as much fat 6.6 ± 2.3% vs. 1.4 ± 0.2%, p < 0.001, and 4.2 ± 1.2%, p < 0.001) and fibre (7.3 ± 2.4% vs. 2.8 ± 0.5%, p < 0.001, and 4.9 ± 2.1%, p = 0.002) as GC breads. This is due to the raw materials themselves and to the addition of ingredients, such as regular and high oleic sunflower oil, and psyllium. Fibre ingredients and additives are more frequently used in ready-to-eat GF flours and breads, and more GF breads also contain fat-based ingredients, as compared to GC. Amaranth and chickpea flours are good alternatives to produce breads with better nutritional quality. Analysis of GF products for critical nutrients is peremptory because of continuing technological and nutritional innovation. Full article
(This article belongs to the Special Issue Gluten-Free Food and Celiac Disease: 2nd Edition)
15 pages, 5870 KiB  
Article
Modelling the Constitutive Behaviour of Recycled PET for the Manufacture of Woven Fabrics
by Huidong Wei, Shan Lou, Martin Leeming and Ying Zhang
Sustainability 2025, 17(5), 2254; https://doi.org/10.3390/su17052254 - 5 Mar 2025
Abstract
Recycling polyethylene terephthalate (rPET) from packaging materials consumes a vast amount of energy and incurs significant economic and environmental costs. This study proposes directly recycling rPET into woven fabrics to eliminate reprocessing while still preserving the mechanical performance of the material. The mechanical [...] Read more.
Recycling polyethylene terephthalate (rPET) from packaging materials consumes a vast amount of energy and incurs significant economic and environmental costs. This study proposes directly recycling rPET into woven fabrics to eliminate reprocessing while still preserving the mechanical performance of the material. The mechanical properties of rPET were tested along two orthogonal directions, and the resulting test data were used to calibrate an elasto-plastic model in order to capture the constitutive behaviour of the material. Additionally, the virtual weaving of rPET fibres into fabrics was modelled using finite element analysis (FEA) to replicate the actual manufacturing process. The results show that rPET that is directly recycled into woven fabrics exhibits superior performance to the same material derived from reprocessing. A strong anisotropy of rPET materials was observed, with distinct elastic and ductile behaviours. The FEA simulation also revealed the critical role of the ductility of rPET fibres when used as warp yarns. The process parameters to achieve a successful weaving operation for different yarn configurations, taking into account the motion and tension of the fibres during manufacture, were also identified. A further sensitivity study highlights the influence of friction between the fibres on the tension force of warp yarns. The virtual manufacture-by-weaving model suggests that utilising rPET with a simplified recycling approach can lead to the sustainable manufacture of fabrics with broad industrial applications. Full article
(This article belongs to the Special Issue Plastic Recycling and Biopolymer Synthesis for Industrial Application)
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Figure 1
<p>Mechanical testing of rPET: (<b>a</b>) specimen design and preparation; (<b>b</b>) thickness measurement; (<b>c</b>) testing machine and specimens after testing.</p>
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<p>Consultive behaviour of rPET: (<b>a</b>) JC material model; (<b>b</b>) finite element model of the uniaxial test.</p>
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<p>Manufacture of woven fabrics: (<b>a</b>) representative region; (<b>b</b>) initial configuration of warp and weft yarns; (<b>c</b>) weaving process.</p>
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<p>Finite element model: (<b>a</b>) meshed model; (<b>b</b>) time history of boundary conditions.</p>
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<p>Testing results and material modelling (SC and SL): (<b>a</b>) experimental stress–strain relationship; (<b>b</b>) simulated SC deformation; (<b>c</b>) simulated SL deformation; (<b>d</b>) force–displacement curve.</p>
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<p>Stress distribution of rPET fibres in sequential weaving process (warp: SC, weft: SC): (<b>a</b>) steps of inserting first weft yarn; (<b>b</b>) steps of inserting other weft yarns.</p>
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<p>Stress distribution of rPET fibres in sequential weaving process (warp: SC, weft: SC): (<b>a</b>) steps of inserting first weft yarn; (<b>b</b>) steps of inserting other weft yarns.</p>
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<p>Stress distribution of rPET fibres in different weaving process: (<b>a</b>) warp: SC, weft: SL; (<b>b</b>) warp: SL, weft: SC.</p>
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<p>Reaction force of warp yarns during weaving process: (<b>a</b>) <span class="html-italic">µ</span> = 0.7 (warp: SC, weft: SC); (<b>b</b>) <span class="html-italic">µ</span> = 0.2 (warp: SC, weft: SC); (<b>c</b>) <span class="html-italic">µ</span> = 0.7 (warp: SC, weft: SL); (<b>d</b>) <span class="html-italic">µ</span> = 0.2 (warp: SC, weft: SL).</p>
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19 pages, 3937 KiB  
Review
Geometric Characterisation of Stochastic Fibrous Networks: A Comprehensive Review
by Yagiz Kayali, Andrew Gleadall and Vadim V. Silberschmidt
Fibers 2025, 13(3), 27; https://doi.org/10.3390/fib13030027 - 5 Mar 2025
Abstract
Fibrous networks are porous materials that can have stochastic and uniform microstructures. Various fibrous networks can be found in nature (e.g., collagens, hydrogels, etc.) or manufactured (e.g., composites and nonwovens). This study focuses on the geometrical characterisation of stochastic fibrous networks with continuous [...] Read more.
Fibrous networks are porous materials that can have stochastic and uniform microstructures. Various fibrous networks can be found in nature (e.g., collagens, hydrogels, etc.) or manufactured (e.g., composites and nonwovens). This study focuses on the geometrical characterisation of stochastic fibrous networks with continuous fibres in a 2D domain, discussing their main relevant parameters: basis weight, orientation distribution function, crimp, porosity, spatial distribution of fibres (uniformity), and fibre intersections. The comprehensive review of the literature is combined with original results to understand the effect of the analysed parameters on various features of fibrous networks such as mechanical performance, filtration, insulation, etc. Full article
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Figure 1
<p>Various fibrous networks with selected microstructures (microstructure of cellulosic paper based on [<a href="#B23-fibers-13-00027" class="html-bibr">23</a>], microstructure of collagen-fibrous network based on [<a href="#B1-fibers-13-00027" class="html-bibr">1</a>], and microstructure of hydrogels based on [<a href="#B24-fibers-13-00027" class="html-bibr">24</a>]).</p>
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<p>Examples of regular and random microstructures: tetragonal (<b>A</b>), triangular (<b>B</b>), and square (<b>C</b>) lattice microstructures with their unit cells; straight (<b>D</b>) and curly (<b>E</b>) random fibrous networks.</p>
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<p>Parameters contributing to the stochastic microstructure of fibrous networks with curly fibres.</p>
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<p>Historical development of techniques for ODF quantification.</p>
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<p>Different options for the graphical presentation of ODF: (<b>A</b>) probability density function (PDF) [<a href="#B54-fibers-13-00027" class="html-bibr">54</a>]; (<b>B</b>) relative frequency [<a href="#B66-fibers-13-00027" class="html-bibr">66</a>]; (<b>C</b>) radar representation based on PDF [<a href="#B51-fibers-13-00027" class="html-bibr">51</a>]; (<b>D</b>) frequency [<a href="#B55-fibers-13-00027" class="html-bibr">55</a>] (CD: cross-direction; MD: machine direction; TD: thickness direction).</p>
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<p>Geometry of fibre crimp with characterisation parameters (modified after [<a href="#B76-fibers-13-00027" class="html-bibr">76</a>]).</p>
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<p>Stretching a curly fibre.</p>
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<p>Different uniformity levels: (<b>A</b>) relatively high uniformity; (<b>B</b>) relatively medium uniformity; (<b>C</b>) relatively low uniformity (modified after [<a href="#B55-fibers-13-00027" class="html-bibr">55</a>]).</p>
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<p>Historical development of offline and online methods (see references in the text).</p>
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<p>Variation in fibre diameters: (<b>A</b>) scanning electron microscopy images of 90 <math display="inline"><semantics> <mrow> <mi mathvariant="normal">g</mi> <mo>/</mo> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msup> </mrow> </semantics></math> (gsm) polymer-based nonwoven fibrous network; (<b>B</b>) measured fibre diameters (locations of measurements are denoted in (<b>A</b>) by red circles with respective fibre ID number).</p>
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<p>Affine and non-affine deformation comparison: (<b>A</b>) fibrous network before deformation; (<b>B</b>) affine deformation; (<b>C</b>) non-affine deformation.</p>
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25 pages, 2364 KiB  
Article
Hemp Seed-Based Foods and Processing By-Products Are Sustainable Rich Sources of Nutrients and Plant Metabolites Supporting Dietary Biodiversity, Health, and Nutritional Needs
by Ricardo Ramos-Sanchez, Nicholas J. Hayward, Donna Henderson, Gary J. Duncan, Wendy R. Russell, Sylvia H. Duncan and Madalina Neacsu
Foods 2025, 14(5), 875; https://doi.org/10.3390/foods14050875 - 4 Mar 2025
Viewed by 38
Abstract
Processing hemp seeds into foods generates several by-products that are rich in nutrients and bioactive phytochemicals. This paper presents a thorough plant metabolite analysis and a comprehensive assessment of the nutrient content of 14 hemp seed-based foods and by-products and evaluates their feasibility [...] Read more.
Processing hemp seeds into foods generates several by-products that are rich in nutrients and bioactive phytochemicals. This paper presents a thorough plant metabolite analysis and a comprehensive assessment of the nutrient content of 14 hemp seed-based foods and by-products and evaluates their feasibility to deliver dietary needs and daily recommendations. The protein-85-product was the hemp food and hemp fudge the hemp by-product with the highest content of protein, 93.01 ± 0.18% and 37.66 ± 0.37%, respectively. Hemp seed-hull flour had the richest insoluble non-starch polysaccharide content (39.80 ± 0.07%). Linoleic acid was the most abundant fatty acid across all the hemp seed-based samples (ranging from 53.80 ± 2.02% in the protein-85-product to 69.53 ± 0.45% in the hemp cream). The omega-6 to omega-3 fatty acid ratio varied from 3:1 to 4:1 across all hemp seed-based samples. The majority of hemp seed-based samples were rich sources of potassium, magnesium, and phosphorus. Gentisic acid, p-coumaric acid, and syringaresinol were the most abundant plant metabolites measured and found mainly in bound form. Hemp seed by-products are valuable sources of nutrients capable of meeting dietary needs and, therefore, should be re-valorized into developing healthy food formulations to deliver a truly zero-waste hemp food production. Full article
(This article belongs to the Special Issue Comprehensive Utilization of By-Products in Food Industry)
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<p>Flow diagram schematically describing all the hemp seed-based foods and by-products used for the analyses; where the hemp food products are depicted in green and the by-products in red color.</p>
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<p>Principal component analysis (UV-scaled) of the plant metabolites analyzed by targeted LC-MS/MS analysis in all the hemp seed-based samples (<b>a</b>) and biplot showing the correlation between plant metabolites and hemp seed-based samples (<b>b</b>). Mandelic acid, (<b>1</b>); 3,4-dimethoxybenzaldehyde, (<b>2</b>); ferulic dimer (5–5 linked), (<b>3</b>); hydroxytyrosol, (<b>4</b>); matairesinol, (<b>5</b>); coumarin, (<b>6</b>); 4-hydroxy-3-methoxyphenylacetic acid, (<b>7</b>); hesperidin, (<b>8</b>); poncirin, (<b>9</b>); phloridzin, (<b>10</b>); neohesperidin, (<b>11</b>); hesperitin, (<b>12</b>); didymin, (<b>13</b>); daidzein, (<b>14</b>); phenyllactic acid, (<b>15</b>); indoe-3-lactic acid, (<b>16</b>); caffeine, (<b>17</b>); glycitein, (<b>18</b>); coumesterol, (<b>19</b>); bergapten, (<b>20</b>); luteolin, (<b>21</b>); morin, (<b>22</b>); epicatechin, (<b>23</b>); benzoic acid, (<b>24</b>); 4; hydroxyphenyllactic acid, (<b>25</b>); 3,4-dihydroxyphenylpropionic acid, (<b>26</b>); quercetin, (<b>27</b>); 4-hydroxy-3-methoxyphenylpropionic acid, (<b>28</b>); indole-3-pyruvic acid, (<b>29</b>); indole-3-acetic acid, (<b>30</b>); ferulic acid, (<b>31</b>); sinapic acid, (<b>32</b>); kaempferol, (<b>33</b>); kynurenic acid, (<b>34</b>); gentisic acid, (<b>35</b>); 4-ethylphenol, (<b>36</b>); o-anisic acid, (<b>37</b>); m-coumaric acid, (<b>38</b>); scopoletin, (<b>39</b>); phenylpyruvic acid, (<b>40</b>); catechin, (<b>41</b>); naringenin, (<b>42</b>); isorhamnetin, (<b>43</b>); isoliquiritigenin, (<b>44</b>); ethylferulate, (<b>45</b>); niacin, (<b>46</b>); chlorogenic acid, (<b>47</b>); 2,3-dihydroxybenzoic acid, (<b>48</b>); 4-hydroxyphenylacetic acid, (<b>49</b>); apigenin, (<b>50</b>); 3,4-dihydroxymandelic acid, (<b>51</b>); vitexin, (<b>52</b>); tyrosol, (<b>53</b>); anthranilic acid, (<b>54</b>); cinnamic acid, (<b>55</b>); naringin, (<b>56</b>); genistein, (<b>57</b>); 3-hydroxymandelic acid, (<b>58</b>); vanillin, (<b>59</b>); quinadilic acid, (<b>60</b>); p-hydroxybenzoic acid, (<b>61</b>)<b>;</b> protocatachaldehyde, (<b>62</b>); 8-methylpsoralen, (<b>63</b>); coniferyl alcohol, (<b>64</b>); myricetin, (<b>65</b>); imperatorin, (<b>66</b>); quercitrin, (<b>67</b>); tangeretin, (<b>68</b>); luteolinidin, (<b>69</b>); formononetin, (<b>70</b>); rutin, (<b>71</b>); 4-hydroxyphenylpyruvic acid, (<b>72</b>); taxifolin, (<b>73</b>); 4-hydroxyacetophenone, (<b>74</b>); 4-hydroxy-3-methoxyacetophenone, (<b>75</b>); caffeic acid, (<b>76</b>); 2,6; dihydroxybenzoic acid, (<b>77</b>); phenylacetic acid, (<b>78</b>); indole, (<b>79</b>); quercetin-3-glucoside, (<b>80</b>); p-coumaric acid, (<b>81</b>); syringin, (<b>82</b>); syringic acid, (<b>83</b>); hyperoside, (<b>84</b>); 3-hydroxyphenylpropionic acid, (<b>85</b>); i3-carboxaldehyde, (<b>86</b>); indole-3-carboxylic acid, (<b>87</b>); ferulic dimer (8-5 linked), (<b>88</b>); 4-hydroxy-3,5-dimethoxyacetophenone, (<b>89</b>); protocatechuic acid, (<b>90</b>); vanillic acid, (<b>91</b>); salicylic acid, (<b>92</b>); syringaresinol, (<b>93</b>); phenol, (<b>94</b>); p-hydroxybenzaldehyde, (<b>95</b>); secoisolariciresinol, (<b>96</b>); 4-hydroxymandelic acid, (<b>97</b>); 4-methoxycinnamic acid, (<b>98</b>); 4-hydroxy-3-methoxymandelic acid, (<b>99</b>); pinoresinol, (<b>100</b>).</p>
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<p>Partial least squares-discriminant analysis of the content of protein, total NSPs, and the plant metabolites analyzed by targeted LC-MS/MS analysis in all the hemp seed-based samples. Mandelic acid, (<b>1</b>); 3,4-dimethoxybenzaldehyde, (<b>2</b>); benzoic acid, (<b>3</b>); indole-3-pyruvic acid, (<b>4</b>); luteolin, (<b>5</b>); morin, (<b>6</b>); gentisic acid, (<b>7</b>); epicatechin, (<b>8</b>); kynurenic acid, (<b>9</b>); ferulic acid, (<b>10</b>); 3,4-dihydroxyphenylpropionic acid, (<b>11</b>); indole-3-acetic acid, (<b>12</b>); kaempferol, (<b>13</b>); sinapic acid, (<b>14</b>); 2,3-dihydroxybenzoic acid, (<b>15</b>); 4-hydroxyphenylacetic acid, (<b>16</b>); 3,4-dihydroxymandelic acid, (<b>17</b>); cinnamic acid, (<b>18</b>); anthranilic acid, (<b>19</b>); p-hydroxybenzoic acid, (<b>20</b>); tyrosol, (<b>21</b>); 4-hydroxy-3-methoxyacetophenone, (<b>22</b>); phenyllactic acid, (<b>23</b>); glycitein, (<b>24</b>); indoe-3-lactic acid, (<b>25</b>); 4-hydroxyphenyllactic acid, (<b>26</b>); coumesterol, (<b>27</b>); caffeine, (<b>28</b>); 4-hydroxy-3; methoxyphenylpropionic acid, (<b>29</b>); bergapten, (<b>30</b>); coniferyl alcohol, (<b>31</b>); quercetin, (<b>32</b>); 8-methylpsoralen, (<b>33</b>); imperatorin, (<b>34</b>); tangeretin, (<b>35</b>); phenylpyruvic acid, (<b>36</b>); myricetin, (<b>37</b>); 4-ethylphenol, (<b>38</b>); o-anisic acid, (<b>39</b>); chlorogenic acid, (<b>40</b>); m-coumaric acid, (<b>41</b>); catechin, (<b>42</b>); quercitrin, (<b>43</b>); niacin, (<b>44</b>); formononetin, (<b>45</b>); scopoletin, (<b>46</b>); naringenin, (<b>47</b>); isorhamnetin, (<b>48</b>); isoliquiritigenin, (<b>49</b>); ethylferulate, (<b>50</b>); apigenin, (<b>51</b>); taxifolin, (<b>52</b>); rutin, (<b>53</b>); vitexin, (<b>54</b>); quinadilic acid, (<b>55</b>); genistein, (<b>56</b>); 4-hydroxyphenylpyruvic acid, (<b>57</b>); phenylacetic acid, (<b>58</b>); protocatachaldehyde, (<b>59</b>); 3-hydroxyphenylpropionic acid, (<b>60</b>); 2,6-dihydroxybenzoic acid, (<b>61</b>); 4-hydroxymandelic acid, (<b>62</b>); phenol, (<b>63</b>); ferulic dimer (5-5 linked), (<b>64</b>); 4-methoxycinnamic acid, (<b>65</b>); p-hydroxybenzaldehyde, (<b>66</b>); 4-hydroxy-3-methoxymandelic acid, (<b>67</b>); naringin, (<b>68</b>); 3-hydroxymandelic acid, (<b>69</b>); quercetin-3-glucoside, (<b>70</b>); vanillin, (<b>71</b>); vanillic acid, (<b>72</b>); syringic acid, (<b>73</b>); syringin, (<b>74</b>); 4-hydroxy-3,5-dimethoxyacetophenone, (<b>75</b>); indole-3-carboxylic acid, (<b>76</b>); p-coumaric acid, (<b>77</b>); I3-carboxaldehyde, (<b>78</b>); syringaresinol, (<b>79</b>); 4-hydroxyacetophenone, (<b>80</b>); caffeic acid, (<b>81</b>); salicylic acid, (<b>82</b>); indole, (<b>83</b>); pinoresinol, (<b>84</b>); hyperoside, (<b>85</b>); protocatechuic acid, (<b>86</b>); secoisolariciresinol, (<b>87</b>); luteolinidin, (<b>88</b>).</p>
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<p>The total plant metabolite content in hemp powders (mg/kg dry product), obtained by summing the individual plant metabolites measured by LC-MS/MS, (<b>a</b>); the eight most abundant individual plant metabolites (mg/kg dry product) measured in hemp seed-based foods and by-products, (<b>b</b>); the total plant metabolite content of hemp oil and hemp cream (mg/kg) obtained by summing the individual plant metabolites measured by LC-MS/MS, (<b>c</b>); the eight most abundant individual plant metabolites (mg/kg) measured in hemp oil (<b>d</b>) and hemp cream. Data within each sample with different letters are significantly different (<span class="html-italic">p</span> &lt; 0.05).</p>
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11 pages, 7620 KiB  
Article
Production of Graphitic Carbon from Renewable Lignocellulosic Biomass Source
by Bindu Antil, Sandeep Olhan and Randy L. Vander Wal
Minerals 2025, 15(3), 262; https://doi.org/10.3390/min15030262 - 3 Mar 2025
Viewed by 100
Abstract
Carbon materials derived from lignocellulosic biomass (LCB) precursors have emerged as sustainable and versatile candidates, exhibiting outstanding properties for energy storage applications. This study presents an innovative and cost-efficient approach to produce graphitic carbon from an LCB precursor (pinecone) using an optimized hydrothermal [...] Read more.
Carbon materials derived from lignocellulosic biomass (LCB) precursors have emerged as sustainable and versatile candidates, exhibiting outstanding properties for energy storage applications. This study presents an innovative and cost-efficient approach to produce graphitic carbon from an LCB precursor (pinecone) using an optimized hydrothermal treatment process followed by carbonization and graphitization. The developed pinecone-derived graphitic carbon (PDGC) was analyzed using X-ray diffraction (XRD), transmission electron microscopy (TEM) and scanning electron microscopy (SEM). XRD analysis confirmed the formation of a graphitic phase, indicated by a sharp and intense (002) peak, decreased interplanar spacing (d002), increased crystallite size (Lc~20.4 nm), and a high degree of graphitization (g~0.7), closely aligning with the characteristics of pure graphite. Additionally, TEM and SEM micrographs revealed a flake-like morphology with well-defined, continuous, and extended graphitic layers within the PDGC structure. The distinctive structural attributes of the developed material position it as a promising candidate for batteries and capacitors, while also serving as a model for converting LCB into advanced carbon materials. Full article
(This article belongs to the Special Issue Graphite Minerals and Graphene, 2nd Edition)
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Graphical abstract

Graphical abstract
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<p>Illustration outlining the development process of graphitic carbon from pinecone feedstock.</p>
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<p>(<b>a</b>) XRD pattern of PDGC and natural graphite, (<b>b</b>,<b>c</b>) extended view of XRD diffractograms of PDGC and natural graphite in different 2<span class="html-italic">θ</span> degree range, and (<b>d</b>) deconvoluted diffractogram of PDGC (inset: extended view of deconvoluted diffractogram).</p>
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<p>TEM images of PDGC highlighting its graphitic morphology at different magnifications: (<b>a</b>,<b>b</b>) display a flaky, layered structure resembling natural graphite, (<b>c</b>) structured graphitic layers, with the inset revealing a 0.337 nm lattice spacing, characteristic of the (002) planes in graphite, and (<b>d</b>) its associated FFT pattern.</p>
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<p>(<b>a</b>,<b>b</b>) SEM images of PDGC showing a flake-like morphology similar to natural graphite (as reported in Ref. [<a href="#B52-minerals-15-00262" class="html-bibr">52</a>]).</p>
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<p>Graphitization mechanism for the conversion of LCB into graphitic carbon.</p>
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27 pages, 8299 KiB  
Article
Monte Carlo Micro-Stress Field Simulations in Flax/E-Glass Composite Laminae with Non-Circular Flax Fibres
by Nenglong Yang, Zhenmin Zou, Constantinos Soutis, Prasad Potluri and Kali Babu Katnam
Polymers 2025, 17(5), 674; https://doi.org/10.3390/polym17050674 - 2 Mar 2025
Viewed by 151
Abstract
This study explores the mechanical behaviour of intra-laminar hybrid flax/E-glass composites, focusing on the role of micro-scale irregularities in flax fibres. By employing computational micromechanics and Monte Carlo simulations, it analyses the influence of flax fibre geometry and elastic properties on the performance [...] Read more.
This study explores the mechanical behaviour of intra-laminar hybrid flax/E-glass composites, focusing on the role of micro-scale irregularities in flax fibres. By employing computational micromechanics and Monte Carlo simulations, it analyses the influence of flax fibre geometry and elastic properties on the performance of hybrid and non-hybrid composites. A Non-Circular Fibre Distribution (NCFD) algorithm is introduced to generate microstructures with randomly distributed non-circular flax and circular E-glass fibres, which are then modelled using a 3D representative volume element (RVE) model developed in Python 2.7 and implemented with Abaqus/Standard. The RVE dimensions were specified as ten times the mean characteristic length of flax fibres (580 μm) for the width and length, while the thickness was defined as one-tenth the radius of the E-glass fibre. Results show that Monte Carlo simulations accurately estimate the effect of fibre variabilities on homogenised elastic constants when compared to measured values and Halpin-Tsai predictions, and they effectively evaluate the fibre/matrix interfacial stresses and von Mises matrix stresses. While these variabilities minimally affect the homogenised properties, they increase the presence of highly stressed regions, especially at the interface and matrix of flax/epoxy composites. Additionally, intra-laminar hybridisation further increases local stress in these critical areas. These findings improve our understanding of the relationship between the natural fibre shape and mechanical performance in flax/E-glass composites, providing valuable insights for designing and optimising advanced composite materials to avoid or delay damage, such as matrix cracking and splitting, under higher applied loads. Full article
(This article belongs to the Special Issue Structure, Characterization and Application of Bio-Based Polymers)
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Figure 1

Figure 1
<p>Representative microstructures of hybrid and non-hybrid composites created using the NCFD algorithm, showing the effects of varying flax fibre shapes and the specified fibre volume fractions for flax, E-glass, and matrix (<math display="inline"><semantics> <mrow> <msub> <mrow> <mi>V</mi> </mrow> <mrow> <mi>f</mi> <mi>F</mi> </mrow> </msub> <mo>,</mo> <msub> <mrow> <msub> <mrow> <mi>V</mi> </mrow> <mrow> <mi>f</mi> <mi>E</mi> </mrow> </msub> <mo>,</mo> <mi>V</mi> </mrow> <mrow> <mi>m</mi> </mrow> </msub> </mrow> </semantics></math>) as follows: (<b>a</b>) (0.48, 0.12, 0.40), (<b>b</b>) (0.48, 0.12, 0.40), (<b>c</b>) (0.60, 0, 0.40), (<b>d</b>) (0.60, 0, 0.40).</p>
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<p>The mean homogenised elastic constants computed from eight Monte Carlo simulation cases, with colour-coded bars transitioning from light to dark red for MCS cases 1–4 (flax/E-glass composites) and light to dark blue for MCS cases 5–8 (flax composites): (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>E</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>11</mn> </mrow> </msub> </mrow> </semantics></math> (GPa), (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>E</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>22</mn> </mrow> </msub> </mrow> </semantics></math> (GPa), (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>G</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>12</mn> </mrow> </msub> </mrow> </semantics></math> (GPa), (<b>d</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>G</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>23</mn> </mrow> </msub> </mrow> </semantics></math> (GPa), (<b>e</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>ν</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>12</mn> </mrow> </msub> </mrow> </semantics></math> and (<b>f</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>ν</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>23</mn> </mrow> </msub> </mrow> </semantics></math>.</p>
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<p>Interface reversed cumulative surface percentages as functions of interfacial stresses: (<b>a1</b>,<b>b1</b>,<b>c1</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>n</mi> </mrow> </msub> </mrow> </semantics></math>, (<b>a2</b>,<b>b2</b>,<b>c2</b>) <math display="inline"><semantics> <mrow> <mfenced open="|" close="|" separators="|"> <mrow> <msub> <mrow> <mi>τ</mi> </mrow> <mrow> <mi>n</mi> <mi>t</mi> </mrow> </msub> </mrow> </mfenced> </mrow> </semantics></math>, for flax/E-glass composites (MCS cases 1–4) subjected to transverse tension (<math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>22</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> MPa), where the leftmost point represents the percentage of interface regions experiencing normalised interfacial stresses greater than 0.1, progressively decreasing rightward to illustrate the proportion subjected to increasing stress, with MCS 1 (baseline) shown by the red line, which may be partially obscured when comparing data from MCS 2, MCS 3, and MCS 4 in each subplot.</p>
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<p>Interface reversed cumulative surface percentages as functions of interfacial stresses: (<b>a1</b>,<b>b1</b>,<b>c1</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>n</mi> </mrow> </msub> </mrow> </semantics></math>, (<b>a2</b>,<b>b2</b>,<b>c2</b>) <math display="inline"><semantics> <mrow> <mfenced open="|" close="|" separators="|"> <mrow> <msub> <mrow> <mi>τ</mi> </mrow> <mrow> <mi>n</mi> <mi>t</mi> </mrow> </msub> </mrow> </mfenced> </mrow> </semantics></math>, for flax composites (MCS cases 5–8) subjected to transverse tension (<math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>22</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> <mtext> </mtext> <mi mathvariant="normal">M</mi> <mi mathvariant="normal">P</mi> <mi mathvariant="normal">a</mi> <mo>)</mo> </mrow> </semantics></math>, where the leftmost point represents the percentage of interface regions experiencing normalised interfacial stresses greater than 0.1, progressively decreasing rightward to illustrate the proportion subjected to increasing stress, with MCS 5 (baseline) shown by the red line, which may be partially obscured when comparing data from MCS 6, MCS 7, and MCS 8 in each subplot.</p>
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<p>Interface reversed cumulative surface percentages as functions of interfacial stresses: (<b>a1</b>,<b>b1</b>,<b>c1</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>n</mi> </mrow> </msub> </mrow> </semantics></math>, (<b>a2</b>,<b>b2</b>,<b>c2</b>) <math display="inline"><semantics> <mrow> <mfenced open="|" close="|" separators="|"> <mrow> <msub> <mrow> <mi>τ</mi> </mrow> <mrow> <mi>n</mi> <mi>t</mi> </mrow> </msub> </mrow> </mfenced> </mrow> </semantics></math>, for MCS cases 1–4 (flax/E-glass composites) subjected to out-of-plane shear (<math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>23</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> <mtext> </mtext> <mi mathvariant="normal">M</mi> <mi mathvariant="normal">P</mi> <mi mathvariant="normal">a</mi> <mo>)</mo> </mrow> </semantics></math>, where the leftmost point represents the percentage of interface regions experiencing normalised interfacial stresses greater than 0.1, progressively decreasing rightward to illustrate the proportion subjected to increasing stress, with MCS 1 (baseline) shown by the red line, which may be partially obscured when comparing data from MCS 2, MCS 3, and MCS 4 in each subplot.</p>
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<p>Interface reversed cumulative surface percentages as functions of interfacial stresses: (<b>a1</b>,<b>b1</b>,<b>c1</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>n</mi> </mrow> </msub> </mrow> </semantics></math>, (<b>a2</b>,<b>b2</b>,<b>c2</b>) <math display="inline"><semantics> <mrow> <mfenced open="|" close="|" separators="|"> <mrow> <msub> <mrow> <mi>τ</mi> </mrow> <mrow> <mi>n</mi> <mi>t</mi> </mrow> </msub> </mrow> </mfenced> </mrow> </semantics></math>, for MCS cases 5–8 (flax laminae) subjected to out-of-plane shear (<math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>23</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> <mtext> </mtext> <mi mathvariant="normal">M</mi> <mi mathvariant="normal">P</mi> <mi mathvariant="normal">a</mi> <mo>)</mo> </mrow> </semantics></math>, where the leftmost point represents the percentage of interface regions experiencing normalised interfacial stresses greater than 0.1, progressively decreasing rightward to illustrate the proportion subjected to increasing stress, with MCS 5 (baseline) shown by the red line, which may be partially obscured when comparing data from MCS 6, MCS 7, and MCS 8 in each subplot.</p>
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<p>Normalised von Mises stress versus reversed cumulative matrix volume percentages for flax/E-glass composites (MCS Cases 1–4), subjected to: (<b>a1</b>,<b>b1</b>,<b>c1</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>22</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> MPa, (<b>a2</b>,<b>b2</b>,<b>c2</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>12</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> MPa, and (<b>a3</b>,<b>b3</b>,<b>c3</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>23</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> MPa, where the leftmost point represents all matrix regions (100%), progressively decreasing rightward to show the proportion subjected to increasing stress, with MCS 1 (baseline) indicated by the red line, which may be partially obscured when comparing data from MCS 2, MCS 3, and MCS 4 in each subplot.</p>
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<p>Normalised von Mises stress versus reversed cumulative matrix volume percentages for flax composites (MCS cases 5–8), subjected to: (<b>a1</b>,<b>b1</b>,<b>c1</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>22</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> MPa, (<b>a2</b>,<b>b2</b>,<b>c2</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>12</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> MPa, and (<b>a3</b>,<b>b3</b>,<b>c3</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>23</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> MPa, where the leftmost point represents all matrix regions (100%), progressively decreasing rightward to show the proportion subjected to increasing stress, with MCS 5 (baseline) indicated by the red line, which may be partially obscured when comparing data from MCS 6, MCS 7, and MCS 8 in each subplot.</p>
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<p>Average normalised <math display="inline"><semantics> <mrow> <msubsup> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>v</mi> <mi>M</mi> </mrow> <mrow> <mi>m</mi> <mi>a</mi> <mi>x</mi> </mrow> </msubsup> </mrow> </semantics></math> calculated across eight Monte Carlo simulations under varying loading conditions, with colour-coded bars transitioning from light to dark red for MCS cases 1–4 (flax/E-glass composites) and light to dark blue for MCS cases 5–8 (flax composites): (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>11</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> <mtext> </mtext> <mi mathvariant="normal">M</mi> <mi mathvariant="normal">P</mi> <mi mathvariant="normal">a</mi> </mrow> </semantics></math>, (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>22</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> <mtext> </mtext> <mi mathvariant="normal">M</mi> <mi mathvariant="normal">P</mi> <mi mathvariant="normal">a</mi> </mrow> </semantics></math>, (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>12</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> <mtext> </mtext> <mi mathvariant="normal">M</mi> <mi mathvariant="normal">P</mi> <mi mathvariant="normal">a</mi> </mrow> </semantics></math> and (<b>d</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>23</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> <mtext> </mtext> <mi mathvariant="normal">M</mi> <mi mathvariant="normal">P</mi> <mi mathvariant="normal">a</mi> </mrow> </semantics></math>.</p>
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<p>Distribution of von Mises stress within the matrix of the flax/E-glass composite (excluding fibres) with a RVE size of <math display="inline"><semantics> <mrow> <mn>580</mn> <mo>×</mo> <mn>580</mn> <mtext> </mtext> <mo>μ</mo> <mi mathvariant="normal">m</mi> </mrow> </semantics></math>, incorporating both fibre-level variabilities, shown for four distinct loading conditions: (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>11</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> MPa, (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>22</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> MPa, (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>12</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> MPa, and (<b>d</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>23</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> MPa.</p>
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<p>Distribution of von Mises stress fields in the flax composite (excluding fibres) with a RVE size of <math display="inline"><semantics> <mrow> <mn>580</mn> <mo>×</mo> <mn>580</mn> <mtext> </mtext> <mo>μ</mo> <mi mathvariant="normal">m</mi> </mrow> </semantics></math>, incorporating both fibre-level variabilities, shown for four distinct loading conditions: (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>11</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> MPa, (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>22</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> MPa, (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>12</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> MPa, and (<b>d</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mover accent="true"> <mrow> <mi>σ</mi> </mrow> <mo stretchy="false">^</mo> </mover> </mrow> <mrow> <mn>23</mn> </mrow> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> MPa.</p>
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14 pages, 9188 KiB  
Article
Filament Type Recognition for Additive Manufacturing Using a Spectroscopy Sensor and Machine Learning
by Gorkem Anil Al and Uriel Martinez-Hernandez
Sensors 2025, 25(5), 1543; https://doi.org/10.3390/s25051543 - 2 Mar 2025
Viewed by 318
Abstract
This study presents a novel approach for filament recognition in fused filament fabrication (FFF) processes using a multi-spectral spectroscopy sensor module combined with machine learning techniques. The sensor module measures 18 wavelengths spanning the visible to near-infrared spectra, with a custom-designed shroud to [...] Read more.
This study presents a novel approach for filament recognition in fused filament fabrication (FFF) processes using a multi-spectral spectroscopy sensor module combined with machine learning techniques. The sensor module measures 18 wavelengths spanning the visible to near-infrared spectra, with a custom-designed shroud to ensure systematic data collection. Filament samples include polylactic acid (PLA), thermoplastic polyurethane (TPU), thermoplastic copolyester (TPC), carbon fibre, acrylonitrile butadiene styrene (ABS), and ABS blended with Carbon fibre. Data are collected using the Triad Spectroscopy module AS7265x (composed of AS72651, AS72652, AS72653 sensor units) positioned at three measurement distances (12 mm, 16 mm, 20 mm) to evaluate recognition performance under varying configurations. Machine learning models, including k-Nearest Neighbors (kNN), Logistic Regression, Support Vector Machine (SVM), and Multi-Layer Perceptron (MLP), are employed with hyperparameter tuning applied to optimise classification accuracy. Results show that the data collected on the AS72651 sensor, paired with the SVM model, achieves the highest accuracy of 98.95% at a 20 mm measurement distance. This work introduces a compact, high-accuracy filament recognition module that can enhance the autonomy of multi-material 3D printing by dynamically identifying and switching between different filaments, optimising printing parameters for each material, and expanding the versatility of additive manufacturing applications. Full article
(This article belongs to the Special Issue Advanced Optical Sensors Based on Machine Learning: 2nd Edition)
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<p>Low-cost spectroscopy sensor and filament samples. (<b>a</b>) Triad Spectral Sensor module from SparkFun Electronics [<a href="#B31-sensors-25-01543" class="html-bibr">31</a>]. (<b>b</b>) Examples of filaments used for data collection and recognition processes.</p>
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<p>Shroud design for systematic data collection. (<b>a</b>) Shroud with three pairs of holes at heights of 12 mm, 16 mm, and 20 mm to place filaments for data collection. (<b>b</b>) The shroud is mounted on the board and covered with a lid. (<b>c</b>) Example of filaments placed at different heights for data collection. (<b>d</b>) Procedure for data collection from filaments using the AS72651 sensor, (<b>e</b>) the AS72652, and (<b>f</b>) the AS72651 sensor.</p>
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<p>(<b>a</b>–<b>l</b>) Spectral information for each filament obtained from the multi-spectral sensor; filaments are positioned on the AS72651 sensor at a height of 12 mm. (<b>m</b>) Spectral information of baseline measurement. (<b>n</b>) The mean spectrum of Red PLA obtained at three distances on the AS72651 sensor. (<b>o</b>) The mean spectrum of the Red PLA filament collected at a 12 mm measurement distance using three different sensors.</p>
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<p>(<b>a</b>–<b>i</b>) t-SNE visualisation of the collected data from each data collection configuration.</p>
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<p>Overview of the data collection process and machine learning implementation for filament recognition.</p>
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<p>The average recognition accuracy of the machine learning models obtained through a 5-fold cross-validation approach; data collected positioning the filaments on the sensors: (<b>a</b>) AS72651, (<b>b</b>) AS72652, and (<b>c</b>) AS72653.</p>
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<p>The highest recognition results achieved using data collected at a 20 mm measurement distance on the AS72651 sensor: (<b>a</b>) k-Nearest Neighbours (kNN), (<b>b</b>) Logistic Regression, (<b>c</b>) Support Vector Machine (SVM), and (<b>d</b>) Multi-Layer Perceptron (MLP).</p>
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12 pages, 3387 KiB  
Article
A Novel Chrono-Potentiometry (CP) Method for Determining the Moisture Content of Wood Above the Fibre Saturation Point (FSP)
by Valdek Tamme, Hannes Tamme, Peeter Muiste and Ahto Kangur
Forests 2025, 16(3), 446; https://doi.org/10.3390/f16030446 - 1 Mar 2025
Viewed by 250
Abstract
The use of a novel chrono-potentiometry method (abbreviated as “CP”) in the determination of the moisture content in wood (abbreviated as “MC”) above the FSP is a practical application of the electrical charging effect (or ECE). In the specific case of this CP [...] Read more.
The use of a novel chrono-potentiometry method (abbreviated as “CP”) in the determination of the moisture content in wood (abbreviated as “MC”) above the FSP is a practical application of the electrical charging effect (or ECE). In the specific case of this CP method, the ECE consists of an electrical charging phase for the wood and a discharge phase following the interruption of the charging current. The electrical resistance, R, and the electrical chargeability, Cha(E), of three hardwood species were determined from the final potential, E1, of the charging phase and the initial potential, E2, of the discharge phase, with the three hardwood species being birch (Betula spp.), aspen (Populus spp.), and black alder (Alnus glutinosa (L.) Gaertn). An auxiliary variable in the form of U (E1; E2) was defined as a function of E1 and E2. This was used as an independent electrical variable in the calibration model for a CP moisture meter for the three tree species when it came to the moisture content (MC) region above the FSP (fibre saturation point). It was found that upon a determination of the MC in the wood, the traditional calibration model (the R-model), which uses the electrical resistance of wood, was able to predict a single-measurement precision level of +/−10% for the MC while the U-model predicted a precision level of +/−1.75% for the MC over a single MC measurement in the wood. Full article
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Figure 1
<p>(<b>a</b>) MetrOhm Autolab with self-made junction box. (CE + RE) and (WE + SE)—signal cables, DE—differential electrometer, GND—ground. (<b>b</b>) Test specimen 1 in climate chamber [<a href="#B11-forests-16-00446" class="html-bibr">11</a>]. e1 and e2—pin electrodes; L, T, and R—anatomical directions of the wood.</p>
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<p>(<b>a</b>) The example of the approximate equality of the average moisture content of the specimen and the local moisture content measured at the depth of 1/3 of the surface of the test specimen (adapted from [<a href="#B13-forests-16-00446" class="html-bibr">13</a>]). (<b>b</b>) The CP general shape of the charge–discharge cycle in the example of the birch wood.</p>
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<p>The average electrical charging number for birch wood under galvanostatic charging at any average MC value of the wood.</p>
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<p>(<b>a</b>) A plot of the linear correlation for parameters E1 and E2. (<b>b</b>) A plot of the linear correlation for parameters E0 and E3.</p>
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<p>(<b>a</b>) An example of a cloud of experimentally determined potential curves for birch wood during the electrical charging phase. (<b>b</b>) An example of a cloud of experimentally determined potential curves for birch wood during the electrical discharge phase.</p>
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<p>(<b>a</b>) An example of a minimisation mechanism for random measurement errors in measured electrical quantities in connection with a birch test specimen during the composition of the auxiliary variable, U, using Equation (9) to define the auxiliary variable. (<b>b</b>) The dependence of electrical chargeability on the wood’s MC in the region above the FSP, as calculated using Equation (4) for three tree species.</p>
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<p>(<b>a</b>) The dependence of the MC on the actual (gravimetric) MC for birch wood, as predicted in the R-model of electrical resistance. (<b>b</b>) The dependence of the MC as predicted from the U-model for birch wood focussing on the actual MC. To be able to create a comparison, the tolerance interval for the focussed model is supplemented by the tolerance interval from the previous, <a href="#forests-16-00446-f006" class="html-fig">Figure 6</a>a (the R-model), i.e., the “wide interval”.</p>
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<p>(<b>a</b>) The dependence of the MC on the actual (gravimetric) MC for aspen wood as predicted in the R-model of electrical resistance. (<b>b</b>) The dependence of the MC as predicted in the U-model for aspen wood focussing on the actual MC. To be able to create a comparison, the tolerance interval for the focussed model is supplemented by the tolerance interval from the previous, <a href="#forests-16-00446-f006" class="html-fig">Figure 6</a>a (the R-model), i.e., the “wide interval”.</p>
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<p>(<b>a</b>) The dependence of the MC on the actual (gravimetric) MC for alder wood as predicted in the R-model of electrical resistance. (<b>b</b>) The dependence of the MC as predicted in the U-model for alder wood focussing on the actual MC. To be able to create a comparison, the tolerance interval for the focussing model is supplemented by the tolerance interval from the previous, <a href="#forests-16-00446-f006" class="html-fig">Figure 6</a>a (the R-model), i.e., the “wide interval”.</p>
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13 pages, 255 KiB  
Article
Association of Paternal BMI and Diet During Pregnancy with Offspring Birth Measures: The STEPS Study
by Michelle L. Kearns, Mirkka Lahdenperä, Laura Galante, Samuli Rautava, Hanna Lagström and Clare M. Reynolds
Nutrients 2025, 17(5), 866; https://doi.org/10.3390/nu17050866 - 28 Feb 2025
Viewed by 211
Abstract
Background/Objectives: Maternal Body Mass Index (BMI), diet quality, and their associated effects on offspring birth measures are well-established. Emerging evidence, largely from animal studies, has indicated paternal factors can influence offspring birth outcomes. However, this effect is poorly understood in humans. Our aim [...] Read more.
Background/Objectives: Maternal Body Mass Index (BMI), diet quality, and their associated effects on offspring birth measures are well-established. Emerging evidence, largely from animal studies, has indicated paternal factors can influence offspring birth outcomes. However, this effect is poorly understood in humans. Our aim was to examine the association between paternal BMI and diet quality score and offspring birth measures. Methods: Participants from the STEPS (Steps to the healthy development) Study in Southwest Finland were recruited during the first trimester of pregnancy or after delivery. A total of 1586 fathers and their children were included for BMI analysis, and 208 fathers and their children were included for dietary analyses. Paternal BMI was calculated using self-reported weight and height at recruitment, and dietary behaviour was assessed using the Index of Diet Quality (IDQ) at 30 weeks’ gestation. Offspring birth weight and length z-scores were calculated using the recently published references specific to the Finnish population. Generalized linear model analyses were carried out to determine associations between paternal factors and offspring z-scores. Results: The mean paternal BMI was 26 (SD ± 3.5). Over half of the fathers were classed as having an unhealthy diet, classified as poor in adhering to nutrition recommendations including higher intakes of saturated fatty acids, and inadequate intakes of protein, saccharose, fibre, vitamins, and minerals. Paternal BMI was not significantly associated with offspring birth weight (β = 0.00 p = 0.884) or birth length (β = 0.00, p = 0.774) z-scores when adjusted for maternal and other paternal and parental factors. Paternal diet quality score was not associated with offspring birth weight (β = −0.01, p = 0.515) or birth length (β = 0.07 p = 0.291) z-scores. Conclusions: This study shows paternal BMI or diet quality at 30 weeks’ gestation does not significantly impact offspring birth measures. Given the known impact of nutrition on epigenetics, examining the potential influence of paternal factors at conception on offspring growth is of major importance and should be included in future studies. Full article
(This article belongs to the Special Issue 2024 Collection: Dietary, Lifestyle and Children Health)
17 pages, 3699 KiB  
Article
A Systematic Investigation of Beam Losses and Position-Reconstruction Techniques Measured with a Novel oBLM at CLEAR
by Montague King, Sara Benitez, Alexander Christie, Ewald Effinger, Jose Esteban, Wilfrid Farabolini, Antonio Gilardi, Pierre Korysko, Jean Michel Meyer, Belen Salvachua, Carsten P. Welsch and Joseph Wolfenden
Instruments 2025, 9(1), 4; https://doi.org/10.3390/instruments9010004 - 28 Feb 2025
Viewed by 155
Abstract
Optical Beam-Loss Monitors (oBLMs) allow for cost-efficient and spatially continuous measurements of beam losses at accelerator facilities. A standard oBLM consists of several tens of metres of optical fibre aligned parallel to a beamline, coupled to photosensors at either or both ends. Using [...] Read more.
Optical Beam-Loss Monitors (oBLMs) allow for cost-efficient and spatially continuous measurements of beam losses at accelerator facilities. A standard oBLM consists of several tens of metres of optical fibre aligned parallel to a beamline, coupled to photosensors at either or both ends. Using the timing information from loss signals, the loss positions can be reconstructed. This paper presents a novel oBLM system recently deployed at the CERN Linear Electron Accelerator for Research (CLEAR). Multiple methods of extracting timing and position information from measured waveforms with silicon photomultipliers (SiPM) and photomultiplier tubes (PMT) are investigated. For this installation, the optimal approach is determined to be applying a constant fraction discrimination (CFD) on the upstream readout. The position resolution is found to be similar for the tested SiPM and PMT. This work has resulted in the development of a user interface to aid operations by visualising the beam losses and their positions in real time. Full article
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<p>A schematic of the beam structure at CLEAR. In both subplots, the y-axis represents the charge while the x-axis represents the time. For the bottom subplot, the time range is much smaller, allowing us to better visualise the beam-train substructure [<a href="#B13-instruments-09-00004" class="html-bibr">13</a>].</p>
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<p>A schematic of the fibre installation at CLEAR. Due to the positioning of the readout electronics in the gallery above the accelerator, a 130 m fibre is necessary to cover the 40 m beam line.</p>
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<p>A loss shower created by a 220 MeV electron beam impacting a 1 cm thick copper target at an x-position of 0 cm. Only particles hitting the fibre are shown. The x-axis represents the distance along the beam, the y-axis gives the vertical distance between the beam axis and the optical fibre. Each fibre-hit location is visualised by a black dashed line connecting the copper and fibre impact locations, the red dashed line visualises a fibre hit at an x-position of 0 cm.</p>
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<p>Fibre-hit positions of charged particles with a velocity greater than the speed of light within silica for a 220 MeV electron beam impacting a 1 cm thick copper target at a position of 0 cm. The number of photons being induced and captured upstream (light blue) or downstream (red) are also shown, with the x-axis representing the horizontal distance to the copper target and the y-axis showing the number of fibre hits and captured photons. A bin size of 20 cm was chosen. The transparent bands visualise the standard errors of the distributions, which were calculated by splitting the primary particles into five evenly sized groups.</p>
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<p>Schematics of two loss positions and the corresponding up- (<b>a</b>) and downstream (<b>b</b>) signal path. Dark blue indicates the direction of the beam, and orange indicates the direction of the photons in the fibre towards the corresponding readout. The overall beam and signal path of the loss at <math display="inline"><semantics> <msub> <mi>L</mi> <mn>1</mn> </msub> </semantics></math> is shown in black, with the same for <math display="inline"><semantics> <msub> <mi>L</mi> <mn>2</mn> </msub> </semantics></math> in light blue.</p>
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<p>A plot showing the mean measured upstream waveforms, read out with a PMT at 700 V for loss signals created by a 30 bunch beam. The time in nanoseconds is shown on the x-axis, with the signal in volts on the y-axis. To visualise statistical fluctuations, the standard deviation on the waveforms are given by the transparent bands.</p>
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<p>A plot showing the mean measured downstream waveforms, read out with a PMT at 700 V for loss signals created by a 30 bunch beam. The time in nanoseconds is shown on the x-axis, with the signal in volts on the y-axis. To visualise statistical fluctuations, the standard deviation on the waveforms are given by the transparent bands.</p>
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<p>A plot showing the measured upstream waveforms, read out with a SiPM at 43 V for loss signals created by a 10 bunch beam. The time in nanoseconds is shown on the x-axis, with the signal in volts on the y-axis. To visualise statistical fluctuations, the standard deviation on the waveforms are given by the transparent bands.</p>
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<p>A plot showing the measured downstream waveforms, read out with a SiPM at 43 V for loss signals created by a 10 bunch beam. The time in nanoseconds is shown on the x-axis, with the signal in volts on the y-axis. To visualise statistical fluctuations, the standard deviation on the waveforms are given by the transparent bands.</p>
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<p>An example plot showing the reconstructed loss position as a function of the screen position for multiple bunch numbers using a constant fraction discrimination and combining SiPM readouts. The dashed black line is a fit to this data and the uncertainty on the data points is the standard deviation from the 20 measured waveforms for each point. The uncertainty on the fitted offset is 4 cm.</p>
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<p>oBLM GUI showing a beam loss occurring at the start (right) of the accelerator, visualised by the pink bar and the blue upstream waveform overlaid on a schematic of the accelerator. Also, various buttons can be seen, which can be used to calibrate the loss positions to the known beam screen locations.</p>
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15 pages, 937 KiB  
Article
Incorporating Non-Linear Epoxy Resin Development in Infusion Simulations: A Dual-Exponent Viscosity Model Approach
by Mohammad W. Tahir, Umar Khan and Jan-Peter Schümann
Polymers 2025, 17(5), 657; https://doi.org/10.3390/polym17050657 - 28 Feb 2025
Viewed by 145
Abstract
In the field of liquid composite moulding (LCM) simulations, a long-standing assumption has dominated–the belief in constant resin viscosity. While effective in many cases, this assumption may not hold for the infusion process, which lasts for an extended period. This impacts the mechanical [...] Read more.
In the field of liquid composite moulding (LCM) simulations, a long-standing assumption has dominated–the belief in constant resin viscosity. While effective in many cases, this assumption may not hold for the infusion process, which lasts for an extended period. This impacts the mechanical properties of the cured epoxy, which are crucial for load transfer in polymer structures. The majority of epoxy resins operate on a bipartite foundation, wherein their viscosity undergoes dynamic alterations during the process of cross-linking. Temperature and cross-linking intricately interact, with elevated temperatures initially reducing viscosity due to kinetic energy but later increasing it as cross-linking accelerates. This interplay significantly influences the efficiency of the infusion process, especially in large and intricate moulds. This article explores the significant temperature dependence of epoxy resin viscosity, proposing an accurate model rooted in its non-linear evolution. This model aligns with empirical evidence, offering insights into determining the optimal starting temperature for efficient mould filling. This study presents an advanced infusion model that extends existing non-linear dual-split viscosity approaches by incorporating the experimental validation of viscosity variations. Unlike previous models that primarily focus on theoretical or numerical frameworks, this work integrates experimental insights to optimize infusion temperature for efficient resin infusion in large and complex parts. Building on these findings, a novel mould-filling technique is proposed to enhance efficiency and reduce material waste. Full article
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Graphical abstract

Graphical abstract
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<p>Schematic of the LCM.</p>
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<p>Plot of temperature development of RIMR 035c epoxy resin with four different hardeners redrawn from manufacturer datasheet.</p>
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<p>Plot of viscosity development with curing for the epoxy resin with fitted data for single exponent model presented in Equation (<a href="#FD1-polymers-17-00657" class="html-disp-formula">1</a>).</p>
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<p>Plot of viscosity development with curing for the epoxy resin with fitted data for dual exponent model shown in Equation (<a href="#FD3-polymers-17-00657" class="html-disp-formula">3</a>).</p>
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<p>Schematic diagram of a typical infusion process in Equation (<a href="#FD3-polymers-17-00657" class="html-disp-formula">3</a>).</p>
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<p>Plot of temperature development of RIMR 035c epoxy resin with four different hardeners under insulated setup [<a href="#B29-polymers-17-00657" class="html-bibr">29</a>].</p>
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<p>Comparison of the flow front position for real infusion of epoxy and the model presented in Equation (<a href="#FD6-polymers-17-00657" class="html-disp-formula">6</a>).</p>
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<p>Plot of the flow front with time for UD flow case. The dotted red line exemplifies a three-hour mould filling time-frame. Infusion at 40 or 45 °C results in an early gelation point causing an incomplete mould filling, while 25 °C causes inefficient filling and extended duration. An optimal starting temperature of 35 °C ensures efficient mould filling.</p>
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19 pages, 1444 KiB  
Article
Valorization of Arbutus unedo L. Pomace: Exploring the Recovery of Bioactive Phenolic Compounds from Distillation By-Products
by Ritamaria Di Lorenzo, Maria Grazia Ferraro, Ceferino Carrera, Federica Iazzetti, Nuria Chinchilla, Maria Maisto, María José Aliaño-González, Vincenzo Piccolo, Anabela Romano, Lucia Ricci, Bruno Medronho, Adua Marzocchi, Marialuisa Piccolo, Gian Carlo Tenore, Carlo Irace and Sonia Laneri
Antioxidants 2025, 14(3), 278; https://doi.org/10.3390/antiox14030278 - 27 Feb 2025
Viewed by 158
Abstract
This study explores the potential of Arbutus unedo L. pomace, a by-product of the food industry, as a natural ingredient for skincare applications. In Portugal, A. unedo L. fruits are traditionally used to produce “Aguardente de Medronho”, a spirit with a protected geographical [...] Read more.
This study explores the potential of Arbutus unedo L. pomace, a by-product of the food industry, as a natural ingredient for skincare applications. In Portugal, A. unedo L. fruits are traditionally used to produce “Aguardente de Medronho”, a spirit with a protected geographical indication. The distillation process generates pomace, comprising skins, pulp remnants, seeds, and residual alcohol rich in phenolic compounds, whose levels are significantly increased during distillation. In addition to their documented high antioxidant content, these residues also display notable antimicrobial properties. However, their potential benefits for skin health have not yet been explored. The methodology entailed the preparation of the pomace extract and a comprehensive analysis of its polyphenolic content and antioxidant capacity under laboratory conditions and in preclinical cellular models. The by-products demonstrated a high polyphenol content and potent antioxidant activity, comparable to vitamin C. Bioscreening on human skin models (i.e., dermal fibroblasts and keratinocytes) revealed their ability to reduce reactive oxygen species (ROS) formation under oxidative stress in skin cells, highlighting their potential to mitigate skin aging and damage caused by environmental pollutants. Moreover, bioscreens in vitro revealed a high safety profile, without any interference with cell viability at concentrations up to 100 µg/mL. These findings support the use of A. unedo L. pomace extract as a sustainable ingredient for the development of antioxidant-rich and eco-friendly cosmetic or dermatologic products. Full article
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<p>Chromatographic profile of <span class="html-italic">A. unedo</span> L. pomace extract in negative acquisition mode by HPLC–HESI–MS/MS analysis.</p>
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<p>Antiradical activity of <span class="html-italic">A. unedo</span> L. pomace extract, expressed as (<b>a</b>) IC<sub>50</sub> of the ABTS assay and (<b>b</b>) IC<sub>50</sub> of the DPPH assay. Values represent the mean ± standard deviation of triplicate reading.</p>
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<p>Preclinical bioscreens for the evaluation of <span class="html-italic">A. unedo</span> L. pomace extract safety and biocompatibility in human skin models. Concentration–response curves by the “cell survival index” for HDFa and HaCaT cells following 48 h (<b>a</b>) and 72 h (<b>b</b>) of treatment with a range of concentrations (5–100 μg/mL) of <span class="html-italic">A. unedo</span> L. pomace extract. Results are expressed in line graphs as a percentage of untreated control cells and are reported as the mean of three independent experiments ± SEM (<span class="html-italic">n</span> = 15).</p>
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<p>Antioxidant activity of <span class="html-italic">A. unedo</span> L. pomace extract in human skin models. ROS detection in HaCaT (<b>a</b>) and HDFa (<b>b</b>) after 24 h and 48 h of treatment with H<sub>2</sub>O<sub>2</sub> alone or in combination with 50 μg/mL of <span class="html-italic">A. unedo</span> L. pomace extract, or with vitamin C. Results are expressed as a percentage of untreated control cells and are reported as the mean of three independent experiments ± SEM (<span class="html-italic">n</span> = 15). * <span class="html-italic">p</span> &lt; 0.05; ** <span class="html-italic">p</span> &lt; 0.01; *** <span class="html-italic">p</span> &lt; 0.001 vs. control; <sup>#</sup> <span class="html-italic">p</span> &lt; 0.05, <sup>##</sup> <span class="html-italic">p</span> &lt; 0.01; <sup>###</sup> <span class="html-italic">p</span> &lt; 0.001 vs. H<sub>2</sub>O<sub>2</sub>-treated cells.</p>
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21 pages, 3022 KiB  
Article
Carbonated Aggregates and Basalt Fiber-Reinforced Polymers: Advancing Sustainable Concrete for Structural Use
by Rabee Shamass, Vireen Limbachiya, Oluwatoyin Ajibade, Musab Rabi, Hector Ulises Levatti Lopez and Xiangming Zhou
Buildings 2025, 15(5), 775; https://doi.org/10.3390/buildings15050775 - 26 Feb 2025
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Abstract
In the transition towards a circular economy, redesigning construction materials for enhanced sustainability becomes crucial. To contribute to this goal, this paper investigates the integration of carbonated aggregates (CAs) and basalt fibre-reinforced polymers (BFRPs) in concrete infrastructures as an alternative to natural sand [...] Read more.
In the transition towards a circular economy, redesigning construction materials for enhanced sustainability becomes crucial. To contribute to this goal, this paper investigates the integration of carbonated aggregates (CAs) and basalt fibre-reinforced polymers (BFRPs) in concrete infrastructures as an alternative to natural sand (NS) and steel reinforcement. CA is manufactured using accelerated carbonation that utilizes CO2 to turn industrial byproducts into mineralised products. The structural performance of CA and BFRP-reinforced concrete simply supported slab was investigated through conducting a series of experimental tests to assess the key structural parameters, including bond strength, bearing capacity, failure behavior, and cracking bbehaviour. Carbon footprint analysis (CFA) was conducted to understand the environmental impact of incorporating BFRP and CA. The results indicate that CA exhibits a higher water absorption rate compared to NS. As the CA ratio increased, the ultrasonic pulse velocity (UPV), compressive, tensile, and flexural strength decreased, and the absorption capacity of concrete increased. Furthermore, incorporating 25% CA in concrete has no significant effect on the bond strength of BFRP. However, the load capacity decreased with an increasing CA replacement ratio. Finally, integrating BFRP and 50% of CA into concrete slabs reduced the slab’s CFA by 9.7% when compared with steel-reinforced concrete (RC) slabs. Full article
(This article belongs to the Topic Green Construction Materials and Construction Innovation)
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<p>Particle size distribution.</p>
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<p>(<b>a</b>) The CA used in this study; (<b>b</b>) the BFRP and steel bars.</p>
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<p>Pull-out test. (<b>a</b>) The sample preparation; (<b>b</b>) a schematic of the pull-out specimen.</p>
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<p>(<b>a</b>) The slab mould showing the reinforcement arrangements; (<b>b</b>) a diagram illustrating the elevation and end-view of the slab specimens.</p>
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<p>(<b>a</b>) Ultrasonic pulse velocity testing; (<b>b</b>) the testing arrangement for the pull-out; (<b>c</b>) the testing arrangement of the slabs.</p>
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<p>UPV and absorption capacity for different mixes.</p>
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<p>Mechanical properties of concrete mixes at twenty-eight days.</p>
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<p>Bond–slip curves for steel and BFRP samples with different carbonated aggregate content.</p>
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<p>The load–deflection relationship of the slabs.</p>
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<p>Failure modes of the tested slabs.</p>
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15 pages, 1232 KiB  
Review
Fibre Lasers: Promising Solutions
by Sergey Kobtsev
Photonics 2025, 12(3), 200; https://doi.org/10.3390/photonics12030200 - 26 Feb 2025
Viewed by 183
Abstract
This work analyses promising solutions for controlling the output radiation properties of fibre lasers. The design of fibre lasers is radically different from that of other laser types. This is why many conventionally used solutions and approaches are incompatible with fibre lasers. Furthermore, [...] Read more.
This work analyses promising solutions for controlling the output radiation properties of fibre lasers. The design of fibre lasers is radically different from that of other laser types. This is why many conventionally used solutions and approaches are incompatible with fibre lasers. Furthermore, fibre lasers following “all-fibre” designs also allow certain solutions that are impossible in other types of lasers. This work discusses those solutions, highlighting the promising applications for all-fibre lasers. Both the advantages and disadvantages of the very low sensitivity of the fibre laser cavities to the external factors are covered. Solutions that are already available commercially or may be expected to be in the near future are highlighted. Various aspects of sensor and communications applications of fibre lasers are discussed. Full article
(This article belongs to the Section Lasers, Light Sources and Sensors)
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<p>The scientist or developer often faces a dilemma; isolation from external factors complicates methods of control over the output radiation (the fibre laser configuration shown in the figure is illustrative; any resemblance to actual components is purely coincidental).</p>
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<p>Use of optical fibre to form the laser cavity allows the significant elongation of the cavity length of such a laser (the fibre laser configuration shown in the figure is illustrative; any resemblance to actual components is purely coincidental).</p>
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<p>Electrical control of the fibre laser output parameters is, undoubtedly, very desirable, but such methods are still insufficiently developed (the fibre laser configuration shown in the figure is illustrative; any resemblance to actual components is purely coincidental).</p>
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