[go: up one dir, main page]

 
 
Sign in to use this feature.

Years

Between: -

Subjects

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Journals

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Article Types

Countries / Regions

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Search Results (15,919)

Search Parameters:
Keywords = elasticity

Order results
Result details
Results per page
Select all
Export citation of selected articles as:
13 pages, 882 KiB  
Article
Predicting Biochemical and Physiological Parameters: Deep Learning from IgG Glycome Composition
by Ana Vujić, Marija Klasić, Gordan Lauc, Ozren Polašek, Vlatka Zoldoš and Aleksandar Vojta
Int. J. Mol. Sci. 2024, 25(18), 9988; https://doi.org/10.3390/ijms25189988 (registering DOI) - 16 Sep 2024
Abstract
In immunoglobulin G (IgG), N-glycosylation plays a pivotal role in structure and function. It is often altered in different diseases, suggesting that it could be a promising health biomarker. Studies indicate that IgG glycosylation not only associates with various diseases but also [...] Read more.
In immunoglobulin G (IgG), N-glycosylation plays a pivotal role in structure and function. It is often altered in different diseases, suggesting that it could be a promising health biomarker. Studies indicate that IgG glycosylation not only associates with various diseases but also has predictive capabilities. Additionally, changes in IgG glycosylation correlate with physiological and biochemical traits known to reflect overall health state. This study aimed to investigate the power of IgG glycans to predict physiological and biochemical parameters. We developed two models using IgG N-glycan data as an input: a regression model using elastic net and a machine learning model using deep learning. Data were obtained from the Korčula and Vis cohorts. The Korčula cohort data were used to train both models, while the Vis cohort was used exclusively for validation. Our results demonstrated that IgG glycome composition effectively predicts several biochemical and physiological parameters, especially those related to lipid and glucose metabolism and cardiovascular events. Both models performed similarly on the Korčula cohort; however, the deep learning model showed a higher potential for generalization when validated on the Vis cohort. This study reinforces the idea that IgG glycosylation reflects individuals’ health state and brings us one step closer to implementing glycan-based diagnostics in personalized medicine. Additionally, it shows that the predictive power of IgG glycans can be used for imputing missing covariate data in deep learning frameworks. Full article
Show Figures

Figure 1

Figure 1
<p>Correlation between the glycan peaks in the glycomics data. The dataset shows high correlation between glycans, which necessitates appropriate predictive models that are immune or at least resistant to such correlated data. Both the elastic net and deep learning have that required property. Glycan composition of each peak within the human IgG glycome has been previously established [<a href="#B32-ijms-25-09988" class="html-bibr">32</a>]. A representative chromatogram of the human IgG glycome and a detailed characterization of the glycan composition for each peak can be found in Pučić et al. [<a href="#B32-ijms-25-09988" class="html-bibr">32</a>] and Krištić et al. [<a href="#B15-ijms-25-09988" class="html-bibr">15</a>].</p>
Full article ">Figure 2
<p>Relative RMSE (root mean square error) normalized to the mean of the dataset for prediction of selected biochemical and physiological parameters based on IgG glycosylation in the Korčula cohort. In addition to the relative area under each of the 24 glycan peaks, only sex was used as an input variable. It is predicted with 100% accuracy, which was used as a “positive control”. Other biochemical and physiological parameters can be predicted from an IgG glycosylation pattern with varying degrees of accuracy. A regression model (glmnet) and a machine learning approach (tensorflow) show a similar degree of predictive power.</p>
Full article ">Figure 3
<p>Validation of the model trained on the Korčula cohort in the Vis cohort shows that the model performs reasonably well with the data from an unrelated sampling event that encompasses a different population, time, and batch. Only the parameters measured in both cohorts are reported. Again, relative RMSE normalized to the mean of the dataset is shown as a metric of the success of prediction for selected biochemical and physiological parameters (lower RMSE means better prediction), based on IgG glycosylation as input. The machine learning approach (tensorflow) performs significantly better for most parameters than the regression model (glmnet). The machine learning approach has the additional advantage of being easily extensible.</p>
Full article ">
17 pages, 6501 KiB  
Article
Enhancing Mechanical Properties of Graphene/Aluminum Nanocomposites via Microstructure Design Using Molecular Dynamics Simulations
by Zhonglei Ma, Hongding Wang, Yanlong Zhao, Zhengning Li, Hong Liu, Yizhao Yang and Zigeng Zhao
Materials 2024, 17(18), 4552; https://doi.org/10.3390/ma17184552 - 16 Sep 2024
Abstract
This study explores the mechanical properties of graphene/aluminum (Gr/Al) nanocomposites through nanoindentation testing performed via molecular dynamics simulations in a large-scale atomic/molecular massively parallel simulator (LAMMPS). The simulation model was initially subjected to energy minimization at 300 K, followed by relaxation for 50 [...] Read more.
This study explores the mechanical properties of graphene/aluminum (Gr/Al) nanocomposites through nanoindentation testing performed via molecular dynamics simulations in a large-scale atomic/molecular massively parallel simulator (LAMMPS). The simulation model was initially subjected to energy minimization at 300 K, followed by relaxation for 50 ps under the NPT ensemble, wherein the number of atoms (N), simulation temperature (T), and pressure (P) were conserved. After the model was fully relaxed, loading and unloading simulations were performed. This study focused on the effects of the Gr arrangement with a brick-and-mortar structure and incorporation of high-entropy alloy (HEA) coatings on mechanical properties. The findings revealed that Gr sheets (GSs) significantly impeded dislocation propagation, preventing the dislocation network from penetrating the Gr layer within the plastic zone. However, interactions between dislocations and GSs in the Gr/Al nanocomposites resulted in reduced hardness compared with that of pure aluminum. After modifying the arrangement of GSs and introducing HEA (FeNiCrCoAl) coatings, the elastic modulus and hardness of the Gr/Al nanocomposites were 83 and 9.5 GPa, respectively, representing increases of 21.5% and 17.3% compared with those of pure aluminum. This study demonstrates that vertically oriented GSs in combination with HEA coatings at a mass fraction of 3.4% significantly enhance the mechanical properties of the Gr/Al nanocomposites. Full article
(This article belongs to the Section Materials Simulation and Design)
Show Figures

Figure 1

Figure 1
<p>Schematic of the nanoindentation models: pure aluminum (<b>a</b>), Gr/Al-level3 (<b>b</b>), Gr/Al-vertical3 (<b>c</b>), HEA/Gr/Al-level3 (<b>d</b>), and HEA/Gr/Al-vertical3 (<b>e</b>).</p>
Full article ">Figure 2
<p>Dislocation distributions observed along the x-axis for the five models, namely pure aluminum, Gr/Al-level3, Gr/Al-vertical3, HEA/Gr/Al-level3, and HEA/Gr/Al-vertical3, at indenter displacements of d = 15, 20, 25, 30, and 35 Å. Dislocations are colored according to their Burgers vector. Green: 1/6&lt;112&gt;; Dark blue: 1/2&lt;110&gt;; Pink: 1/6&lt;110&gt;; Yellow: 1/3&lt;100&gt;; Bright blue: 1/3&lt;111&gt;; Red: others.</p>
Full article ">Figure 3
<p>Side views of the y–z-planes of Gr/Al-level3 (<b>a</b>) and HEA/Gr/Al-level3 (<b>b</b>) at indentation depths of 0, 20, 25, and 30 Å. The viewing direction is along the x-axis.</p>
Full article ">Figure 4
<p>Side views of the y–z-planes of Gr/Al-vertical3 (<b>a</b>) at indentation depths of 0, 26, 27, 28, and 29 Å and HEA/Gr/Al-vertical3 (<b>b</b>) at indentation depths of 0, 9, 11, 13, and 16 Å. The viewing direction is along the x-axis.</p>
Full article ">Figure 5
<p>In-plane height profiles of Gr at an indentation depth of 30 Å for models Gr/Al-level3 (<b>a</b>), HEA/Gr/Al-level3 (<b>b</b>), Gr/Al-vertical3 (<b>c</b>), and HEA/Gr/Al-vertical3 (<b>d</b>).</p>
Full article ">Figure 6
<p>Evolution of total dislocation length (<b>a</b>) and indentation force (<b>b</b>) with indenter displacement.</p>
Full article ">Figure 7
<p>Hardness values vs. indentation depths.</p>
Full article ">Figure 8
<p>Force–displacement curves at the unloading stage.</p>
Full article ">Figure 9
<p>Distribution of dislocation lines and defect atoms at different indenter displacements during the unloading stage. Dislocations are colored according to their Burgers vector. Green: 1/6&lt;112&gt;; Dark blue: 1/2&lt;110&gt;; Pink: 1/6&lt;110&gt;; Yellow: 1/3&lt;100&gt;; Bright blue: 1/3&lt;111&gt;; Red: others. (<b>a</b>) pure aluminum; (<b>b</b>) Gr/Al-level3; (<b>c</b>) Gr/Al-vertical3; (<b>d</b>) HEA/Gr/Al-level3; (<b>e</b>) HEA/Gr/Al-vertical3.</p>
Full article ">Figure 10
<p>Reduced Young’s modulus of the five models.</p>
Full article ">Figure 11
<p>Dislocation length–indenter displacement curves. (<b>a</b>) pure aluminum; (<b>b</b>) Gr/Al-vertical3; (<b>c</b>) HEA/Gr/Al-level3; (<b>d</b>) HEA/Gr/Al-vertical3.</p>
Full article ">
22 pages, 7233 KiB  
Article
Incremental Growth Analysis of a Cantilever Beam under Cyclic Thermal and Axial Loads
by Ali Shahrjerdi, Hamidreza Heydari, Mahdi Bayat and Mohammadmehdi Shahzamanian
Materials 2024, 17(18), 4550; https://doi.org/10.3390/ma17184550 - 16 Sep 2024
Abstract
Ratcheting analysis for cantilever beams subjected to the thermomechanical loads is presented using the finite element method. The cantilever beam is constrained along the vertical direction, and plane stress conditions are assumed according to the bilinear isotropic hardening model. Two points are considered [...] Read more.
Ratcheting analysis for cantilever beams subjected to the thermomechanical loads is presented using the finite element method. The cantilever beam is constrained along the vertical direction, and plane stress conditions are assumed according to the bilinear isotropic hardening model. Two points are considered to obtain areas of ratcheting by using linear extrapolation. The results and output diagrams for ratcheting with elastic-perfect plastic behavior are illustrated. It was revealed that the beam behaves elastically after the first considerable plastic strain, which is seen in two shakedown regimes. The numerical results are verified with known and analytical results in the literature. The results indicate a strong correlation between the outcomes from the cyclic ANSYS Parametric Design Language (APDL) model and Bree’s analytical predictions. This consistency between the finite element analysis and the analytical solutions underscores the potential of finite element analysis as a powerful tool for addressing complex engineering challenges, offering a reliable and robust alternative to traditional analytical methods. Full article
Show Figures

Figure 1

Figure 1
<p>Load diagram for the uniaxial stress model.</p>
Full article ">Figure 2
<p>(<b>a</b>) Cantilever beam and applied loads. (<b>b</b>) Constant mechanical load. (<b>c</b>) Cyclic thermal gradient.</p>
Full article ">Figure 3
<p>The schematic of stress–strain regimes.</p>
Full article ">Figure 4
<p>The steps in APDL.</p>
Full article ">Figure 5
<p>The stress–strain path corresponding to the stress regime R1 at <math display="inline"><semantics> <mrow> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>p</mi> </mrow> </msub> </mrow> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </mfrac> </mstyle> <mo>=</mo> <mn>0.7</mn> <mo>,</mo> <mo> </mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>t</mi> </mrow> </msub> </mrow> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </mfrac> </mstyle> <mo>=</mo> <mn>1.5</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>x</mi> <mo>=</mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mi>d</mi> </mrow> <mrow> <mn>2</mn> </mrow> </mfrac> </mstyle> <mo>,</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>=</mo> <mn>3</mn> <mi>K</mi> </mrow> </semantics></math>.</p>
Full article ">Figure 6
<p>The stress–strain path corresponding to the stress regime R2 at <math display="inline"><semantics> <mrow> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>p</mi> </mrow> </msub> </mrow> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </mfrac> </mstyle> <mo>=</mo> <mn>0.366</mn> <mo>,</mo> <mo> </mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>t</mi> </mrow> </msub> </mrow> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </mfrac> </mstyle> <mo>=</mo> <mn>3</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>x</mi> <mo>=</mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mi>d</mi> </mrow> <mrow> <mn>2</mn> </mrow> </mfrac> </mstyle> <mo>,</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>=</mo> <mn>6</mn> <mi>K</mi> </mrow> </semantics></math>.</p>
Full article ">Figure 7
<p>The stress–strain path corresponding to the stress regime P at <math display="inline"><semantics> <mrow> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>p</mi> </mrow> </msub> </mrow> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </mfrac> </mstyle> <mo>=</mo> <mn>0.167</mn> <mo>,</mo> <mo> </mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>t</mi> </mrow> </msub> </mrow> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </mfrac> </mstyle> <mo>=</mo> <mn>3</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>x</mi> <mo>=</mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mi>d</mi> </mrow> <mrow> <mn>2</mn> </mrow> </mfrac> </mstyle> <mo>,</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>=</mo> <mn>6</mn> <mi>K</mi> </mrow> </semantics></math>.</p>
Full article ">Figure 8
<p>The stress–strain path corresponding to the stress regime S1 at <math display="inline"><semantics> <mrow> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>p</mi> </mrow> </msub> </mrow> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </mfrac> </mstyle> <mo>=</mo> <mn>0.5</mn> <mo>,</mo> <mo> </mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>t</mi> </mrow> </msub> </mrow> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </mfrac> </mstyle> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>x</mi> <mo>=</mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mi>d</mi> </mrow> <mrow> <mn>2</mn> </mrow> </mfrac> </mstyle> <mo>,</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>=</mo> <mn>2</mn> <mi>K</mi> </mrow> </semantics></math>.</p>
Full article ">Figure 9
<p>The stress–strain path corresponding to the stress regime S2 at <math display="inline"><semantics> <mrow> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>p</mi> </mrow> </msub> </mrow> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </mfrac> </mstyle> <mo>=</mo> <mn>0.25</mn> <mo>,</mo> <mo> </mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>t</mi> </mrow> </msub> </mrow> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </mfrac> </mstyle> <mo>=</mo> <mn>1.5</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>x</mi> <mo>=</mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mi>d</mi> </mrow> <mrow> <mn>2</mn> </mrow> </mfrac> </mstyle> <mo>,</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>=</mo> <mn>3</mn> <mi>K</mi> </mrow> </semantics></math>.</p>
Full article ">Figure 10
<p>The stress–strain path corresponding to the stress regime R1 at <math display="inline"><semantics> <mrow> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>p</mi> </mrow> </msub> </mrow> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </mfrac> </mstyle> <mo>=</mo> <mn>0.7</mn> <mo>,</mo> <mo> </mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>t</mi> </mrow> </msub> </mrow> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </mfrac> </mstyle> <mo>=</mo> <mn>1.5</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>x</mi> <mo>=</mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mi>d</mi> </mrow> <mrow> <mn>2</mn> </mrow> </mfrac> </mstyle> <mo>,</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>=</mo> <mn>3</mn> <mi>K</mi> </mrow> </semantics></math> with more cycles.</p>
Full article ">Figure 11
<p>The stress–strain path corresponding to the stress regime R1 at <math display="inline"><semantics> <mrow> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>p</mi> </mrow> </msub> </mrow> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </mfrac> </mstyle> <mo>=</mo> <mn>0.9</mn> <mo>,</mo> <mo> </mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>t</mi> </mrow> </msub> </mrow> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </mfrac> </mstyle> <mo>=</mo> <mn>7</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>x</mi> <mo>=</mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mi>d</mi> </mrow> <mrow> <mn>2</mn> </mrow> </mfrac> </mstyle> <mo>,</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>=</mo> <mn>14</mn> <mi>K</mi> </mrow> </semantics></math>.</p>
Full article ">Figure 12
<p>Variations in the ratchet strains with constant <math display="inline"><semantics> <mrow> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>t</mi> </mrow> </msub> </mrow> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </mfrac> </mstyle> </mrow> </semantics></math> for the plane stress model.</p>
Full article ">Figure 13
<p>Bree interaction diagram, along with results from the theory.</p>
Full article ">
15 pages, 2071 KiB  
Article
Research on Landing Dynamics of Foot-High Projectile Body for High-Precision Microgravity Simulation System
by Zhenhe Jia, Yuehua Li, Weijie Hou, Libin Zang, Qiang Han, Baoshan Zhao, Bin Gao, Haiteng Liu, Yuhan Chen, Yumin An and Huibo Zhang
Actuators 2024, 13(9), 361; https://doi.org/10.3390/act13090361 - 16 Sep 2024
Abstract
A high-precision ground microgravity simulation environment serves as the prerequisite and key to studying landing dynamics in microgravity environments. However, the microgravity level accuracy in traditional ground simulation tests is difficult to guarantee and fails to precisely depict the collision behavior of massive [...] Read more.
A high-precision ground microgravity simulation environment serves as the prerequisite and key to studying landing dynamics in microgravity environments. However, the microgravity level accuracy in traditional ground simulation tests is difficult to guarantee and fails to precisely depict the collision behavior of massive spacecraft. To solve such problems, this paper takes the microgravity simulation system based on quasi-zero stiffness (QZS) mechanism as the research object, and simulates a high-precision and high-level microgravity environment. Then, the collision contact force model of the planar foot and high elastic body rubber is established, the landing dynamics research under different microgravity environments is carried out, the influence of different microgravity environments on the landing behavior of large mass spacecraft is analyzed in depth, and ground microgravity simulation experiments are carried out. The results show that the microgravity simulation level reaches 10−4 g, the error of gravity compensation for each working condition is not more than 4.22%, and the error of sinking amount is not more than 4.61%, which verifies the superior compensation performance of the QZS mechanism and the accuracy of the dynamic model. Full article
(This article belongs to the Section Aircraft Actuators)
18 pages, 10499 KiB  
Article
Numerical Assessment of Effective Elastic Properties of Needled Carbon/Carbon Composites Based on a Multiscale Method
by Jian Ge, Xujiang Chao, Haoteng Hu, Wenlong Tian, Weiqi Li and Lehua Qi
C 2024, 10(3), 85; https://doi.org/10.3390/c10030085 (registering DOI) - 16 Sep 2024
Abstract
Needled carbon/carbon composites contain complex microstructures such as irregular pores, anisotropic pyrolytic carbon, and interphases between fibers and pyrolytic carbon matrices. Additionally, these composites have hierarchical structures including weftless plies, short-cut fiber plies, and needled regions. To predict the effective elastic properties of [...] Read more.
Needled carbon/carbon composites contain complex microstructures such as irregular pores, anisotropic pyrolytic carbon, and interphases between fibers and pyrolytic carbon matrices. Additionally, these composites have hierarchical structures including weftless plies, short-cut fiber plies, and needled regions. To predict the effective elastic properties of needled carbon/carbon composites, this paper proposes a novel sequential multiscale method. At the microscale, representative volume element (RVE) models are established based on the microstructures of the weftless ply, short-cut fiber ply, and needled region, respectively. In the microscale RVE model, a modified Voronoi tessellation method is developed to characterize anisotropic pyrolytic carbon matrices. At the macroscale, an RVE model containing hierarchical structures is developed to predict the effective elastic properties of needled carbon/carbon composites. For the data interaction between scales, the homogenization results of microscale models are used as inputs for the macroscale model. By comparing these against the experimental results, the proposed multiscale model is validated. Furthermore, the effect of porosity on the effective elastic properties of needled carbon/carbon composites is investigated based on the multiscale model. The results show that the effective elastic properties of needled carbon/carbon composites decrease with the increase in porosity, but the extent of decrease is different in different directions. Full article
(This article belongs to the Special Issue Micro/Nanofabrication of Carbon-Based Devices and Their Applications)
Show Figures

Figure 1

Figure 1
<p>The microstructural illustration of needled carbon/carbon composites.</p>
Full article ">Figure 2
<p>(<b>a</b>) The SEM image of the weftless ply and (<b>b</b>) the distribution of the fiber diameter.</p>
Full article ">Figure 3
<p>Illustration of the ICVI process, where the precursor gas enters the reaction chamber and reacts on the surface of carbon fibers to obtain pyrolytic carbon, and the temperature uniformity is assured by the graphite heater.</p>
Full article ">Figure 4
<p>(<b>a</b>) Microstructures of needled carbon/carbon composites, where <span class="html-italic">t<sub>s</sub></span> is the thickness of the short-cut fiber ply, <span class="html-italic">t<sub>u</sub></span> is the thickness of the weftless ply, and <span class="html-italic">D<sub>F</sub></span> is the diameter of the needled region. (<b>b</b>) Short-cut fiber ply lies between the 0° and 90° weftless plies. (<b>c</b>) The pyrolytic carbon morphology under the polarized light microscope. (<b>d</b>–<b>f</b>) The grayscale histograms of (<b>a</b>–<b>c</b>) are presented, respectively.</p>
Full article ">Figure 5
<p>The schematic diagram of the tensile test of needled C/C composites.</p>
Full article ">Figure 6
<p>The multiscale scheme for predicting the effective elastic properties of needled C/C composites.</p>
Full article ">Figure 7
<p>(<b>a</b>) The RVE model of the weftless ply before partitioning the equivalent matrix, and (<b>b</b>) the RVE model after partitioning the equivalent matrix.</p>
Full article ">Figure 8
<p>(<b>a</b>) The RVE model of the short-cut fiber ply before partitioning the equivalent matrix, and (<b>b</b>) the RVE model after partitioning the equivalent matrix.</p>
Full article ">Figure 9
<p>Illustration of the RVE model of the needled fiber region.</p>
Full article ">Figure 10
<p>The macroscale model of needled C/C composites.</p>
Full article ">Figure 11
<p>Effects of the mesh size on (<b>a</b>) <span class="html-italic">E</span><sub>11</sub>/<span class="html-italic">E</span><sub>22</sub> and <span class="html-italic">E</span><sub>33</sub>, (<b>b</b>) <span class="html-italic">G</span><sub>12</sub> and <span class="html-italic">G</span><sub>13</sub>/<span class="html-italic">G</span><sub>23</sub>, (<b>c</b>) <span class="html-italic">ν</span><sub>12</sub> and <span class="html-italic">ν</span><sub>13</sub>/<span class="html-italic">ν</span><sub>23</sub>, and (<b>d</b>) the relative error.</p>
Full article ">Figure 12
<p>Effects of the model length on (<b>a</b>) <span class="html-italic">E</span><sub>11</sub>/<span class="html-italic">E</span><sub>22</sub> and <span class="html-italic">E</span><sub>33</sub>, (<b>b</b>) <span class="html-italic">G</span><sub>12</sub> and <span class="html-italic">G</span><sub>13</sub>/<span class="html-italic">G</span><sub>23</sub>, (<b>c</b>) <span class="html-italic">ν</span><sub>12</sub> and <span class="html-italic">ν</span><sub>13</sub>/<span class="html-italic">ν</span><sub>23</sub>, and (d) the relative error.</p>
Full article ">Figure 13
<p>Effects of the model thickness on (<b>a</b>) <span class="html-italic">E</span><sub>11</sub>/<span class="html-italic">E</span><sub>22</sub> and <span class="html-italic">E</span><sub>33</sub>, (<b>b</b>) <span class="html-italic">G</span><sub>12</sub> and <span class="html-italic">G</span><sub>13</sub>/<span class="html-italic">G</span><sub>23</sub>, (<b>c</b>) <span class="html-italic">ν</span><sub>12</sub> and <span class="html-italic">ν</span><sub>13</sub>/<span class="html-italic">ν</span><sub>23</sub>, and (<b>d</b>) the relative error.</p>
Full article ">Figure 14
<p>Effects of porosity <span class="html-italic">V<sub>p</sub></span> on the effective elastic properties of (<b>a1</b>,<b>a2</b>) the needled region, (<b>b1</b>,<b>b2</b>) weftless ply, (<b>c1</b>,<b>c2</b>) short-cut fiber ply, and (<b>d1</b>,<b>d2</b>) needled C/C composite.</p>
Full article ">Figure 14 Cont.
<p>Effects of porosity <span class="html-italic">V<sub>p</sub></span> on the effective elastic properties of (<b>a1</b>,<b>a2</b>) the needled region, (<b>b1</b>,<b>b2</b>) weftless ply, (<b>c1</b>,<b>c2</b>) short-cut fiber ply, and (<b>d1</b>,<b>d2</b>) needled C/C composite.</p>
Full article ">
20 pages, 5152 KiB  
Article
Polyphenol-Rich Cranberry Beverage Positively Affected Skin Health, Skin Lipids, Skin Microbiome, Inflammation, and Oxidative Stress in Women in a Randomized Controlled Trial
by Lindsey Christman, Anna De Benedetto, Elizabeth Johnson, Christina Khoo and Liwei Gu
Nutrients 2024, 16(18), 3126; https://doi.org/10.3390/nu16183126 - 16 Sep 2024
Abstract
This study aimed to determine whether a polyphenol-rich cranberry beverage affects skin properties, lipids, and the microbiome in women using a randomized, double-blinded, placebo-controlled, cross-over design. Twenty-two women with Fitzpatrick skin types 2–3 were randomized to drink a cranberry beverage or placebo for [...] Read more.
This study aimed to determine whether a polyphenol-rich cranberry beverage affects skin properties, lipids, and the microbiome in women using a randomized, double-blinded, placebo-controlled, cross-over design. Twenty-two women with Fitzpatrick skin types 2–3 were randomized to drink a cranberry beverage or placebo for six weeks. After a 21-day washout, they consumed the opposite beverage for six weeks. Six weeks of cranberry beverage significantly reduced UVB-induced erythema, improved net elasticity on the face and forearm, smoothness on the face, and gross elasticity on the forearm compared to the placebo. When stratified by age, these effects of the cranberry beverage were primarily observed in women >40 years old. SOD activities were improved after six weeks of cranberry beverage consumption compared to the placebo, while glutathione peroxide and TNF-α were improved compared to baseline. These effects were found to differ by age group. Skin lipid composition was modulated by both the cranberry beverage and the placebo. Cranberry beverages did not change α- or β-diversity but altered the abundance of several skin microbes at the species and strain level. Consumption of a cranberry beverage for six weeks improved specific skin properties and oxidative stress and modulated skin lipids and microbiome compared to placebo. Full article
(This article belongs to the Special Issue Nutritional Value and Health Benefits of Dietary Bioactive Compounds)
Show Figures

Figure 1

Figure 1
<p>The CONSORT flow diagram of the study shows the enrollment, randomization, participation, and data analysis throughout the study.</p>
Full article ">Figure 2
<p>Plasma levels of SOD (<b>A</b>), GPx (<b>B</b>), AGE (<b>C</b>), TNF-α (<b>D</b>), IL-17 (<b>E</b>), and Hs-CRP (<b>F</b>) in all 22 participants. Plasma was collected at baseline and final time points after six weeks of cranberry beverage or placebo consumption. Results are expressed as mean ± SD. <sup>&amp;</sup> is the significant difference between cranberry and placebo; <sup>#</sup> is the significant difference between final and baseline. SOD: superoxide dismutase, GPx: glutathione peroxide; IL-interleukin; TNF: tumor necrosis factor; Hs-CRP: high-sensitivity C-reactive protein.</p>
Full article ">Figure 3
<p>Cranberry beverage intake altered skin lipids compared to baseline and placebo. Panels (<b>A1</b>,<b>B1</b>,<b>C1</b>) are score plots derived from paired partial least squares discriminant analysis (PLS-DA). Panels (<b>A2</b>,<b>B2</b>,<b>C2</b>) are corresponding cross-validated score plots. Each dot represents a participant (<span class="html-italic">n</span> = 20).</p>
Full article ">Figure 4
<p>Spearman correlation of discriminant skin lipids, skin parameters, and blood biomarkers for all participants (<span class="html-italic">n</span> = 20). Different colors represent differences in Rho value. The bold black outlines indicate significant correlations.</p>
Full article ">Figure 5
<p>Cranberry beverage intake affected the relative abundance of differential taxa at the species level. The <span class="html-italic">q</span> values were calculated by MaAsLin2. The boxes represent the interquartile range (IQR) between the first and third quartiles. Dots indicate individual participants.</p>
Full article ">Figure 6
<p>Cranberry beverage intake affected the relative abundance of differential taxa at the strain level. The q values were calculated by MaAsLin2. The boxes represent the interquartile range (IQR) between the first and third quartiles. Dots indicate individual participants.</p>
Full article ">Figure 7
<p>Significantly changed microbial taxa correlated with skin parameters, oxidative stress, and inflammatory biomarkers. Significant correlations were identified using MaAsLin2 and are plotted as (−log(<span class="html-italic">q</span>-value) * sign(coeff)). Significant positive or negative correlations were indicated by ‘+’ and ‘−‘.</p>
Full article ">Figure 8
<p>Spearman correlations between discriminant skin lipids determined by paired PLS-DA and significantly changed microbial taxa determined by MaAsLin2. Different color values represent different Rho values. The bold black outline indicates significant correlations.</p>
Full article ">
19 pages, 419 KiB  
Article
Rayleigh Waves in a Thermoelastic Half-Space Coated by a Maxwell–Cattaneo Thermoelastic Layer
by Stan Chiriţă and Ciro D’Apice
Mathematics 2024, 12(18), 2885; https://doi.org/10.3390/math12182885 - 16 Sep 2024
Viewed by 64
Abstract
This paper investigates the propagation of in-plane surface waves in a coated thermoelastic half-space. First, it investigates a special case where the surface layer is described by the Maxwell–Cattaneo thermoelastic approach, while the half-space is filled by a thermoelastic material described by the [...] Read more.
This paper investigates the propagation of in-plane surface waves in a coated thermoelastic half-space. First, it investigates a special case where the surface layer is described by the Maxwell–Cattaneo thermoelastic approach, while the half-space is filled by a thermoelastic material described by the classical Fourier law for the heat flux. The contact between the layer and the half-space is assumed to be welded, i.e., the displacements and the temperature, as well as the stresses and the heat flux are continuous through the interface of the layer and the half-space. The boundary and continuity conditions of the problem are formulated and then the exact dispersion relation of the surface waves is established. An illustrative numerical simulation is presented for the case of an aluminum thermoelastic layer coating a thermoelastic copper half-space, highlighting important aspects regarding the propagation of Rayleigh waves in such structures. The exact effective boundary conditions at the interface are also established replacing the entire effect of the layer on the half-space. The general case of the problem is also investigated when both the surface layer and the half-space are described by the Maxwell–Cattaneo thermoelasticity theory. This study helps to further understand the propagation characteristics of elastic waves in layered structures with thermal effects described by the Maxwell–Cattaneo approach. Full article
(This article belongs to the Special Issue Advanced Computational Mechanics)
Show Figures

Figure 1

Figure 1
<p>Layered structure.</p>
Full article ">Figure 2
<p>The variation in the dimensionless propagation speed <math display="inline"><semantics> <mrow> <mo form="prefix">Re</mo> <mo>(</mo> <mi>C</mi> <mo>)</mo> <mo>&gt;</mo> <mn>0</mn> </mrow> </semantics></math> with respect to the relaxation time <math display="inline"><semantics> <mrow> <mi>τ</mi> <mo>∈</mo> <mo>[</mo> <mn>0</mn> <mo>,</mo> <msup> <mn>10</mn> <mrow> <mo>−</mo> <mn>2</mn> </mrow> </msup> <mspace width="0.166667em"/> <mi mathvariant="normal">s</mi> <mo>]</mo> </mrow> </semantics></math>, (the thickness of the layer is fixed at <math display="inline"><semantics> <mrow> <mi>h</mi> <mo>=</mo> <msup> <mn>10</mn> <mrow> <mo>−</mo> <mn>3</mn> </mrow> </msup> <mspace width="0.166667em"/> <mi mathvariant="normal">m</mi> </mrow> </semantics></math>).</p>
Full article ">Figure 3
<p>The variation in the dimensionless dumping in time <math display="inline"><semantics> <mrow> <mo form="prefix">Im</mo> <mo>(</mo> <mi>C</mi> <mo>)</mo> <mo>&gt;</mo> <mn>0</mn> </mrow> </semantics></math> of the amplitude of wave, with respect to the relaxation time <math display="inline"><semantics> <mrow> <mi>τ</mi> <mo>∈</mo> <mo>[</mo> <mn>0</mn> <mo>,</mo> <msup> <mn>10</mn> <mrow> <mo>−</mo> <mn>2</mn> </mrow> </msup> <mspace width="0.166667em"/> <mi mathvariant="normal">s</mi> <mo>]</mo> </mrow> </semantics></math>, (the thickness of the layer is fixed at <math display="inline"><semantics> <mrow> <mi>h</mi> <mo>=</mo> <msup> <mn>10</mn> <mrow> <mo>−</mo> <mn>3</mn> </mrow> </msup> <mspace width="0.166667em"/> <mi mathvariant="normal">m</mi> </mrow> </semantics></math>).</p>
Full article ">
16 pages, 5561 KiB  
Article
Metagenomic and Metabolomic Analyses Reveal the Role of Gut Microbiome-Associated Metabolites in the Muscle Elasticity of the Large Yellow Croaker (Larimichthys crocea)
by Zhenheng Cheng, Hao Huang, Guangde Qiao, Yabing Wang, Xiaoshan Wang, Yanfeng Yue, Quanxin Gao and Shiming Peng
Animals 2024, 14(18), 2690; https://doi.org/10.3390/ani14182690 - 16 Sep 2024
Viewed by 105
Abstract
The large yellow croaker (LYC, Larimichthys crocea) is highly regarded for its delicious taste and unique flavor. The gut microbiota has the ability to affect the host muscle performance and elasticity by regulating nutrient metabolism. The purpose of this study is to [...] Read more.
The large yellow croaker (LYC, Larimichthys crocea) is highly regarded for its delicious taste and unique flavor. The gut microbiota has the ability to affect the host muscle performance and elasticity by regulating nutrient metabolism. The purpose of this study is to establish the relationship between muscle quality and intestinal flora in order to provide reference for the improvement of the muscle elasticity of LYC. In this study, the intestinal contents of high muscle elasticity males (IEHM), females (IEHF), and low muscle elasticity males (IELM) and females (IELF) were collected and subjected to metagenomic and metabolomic analyses. Metagenomic sequencing results showed that the intestinal flora structures of LYCs with different muscle elasticities were significantly different. The abundance of Streptophyta in the IELM (24.63%) and IELF (29.68%) groups was significantly higher than that in the IEHM and IEHF groups. The abundance of Vibrio scophthalmi (66.66%) in the IEHF group was the highest. Based on metabolomic analysis by liquid chromatograph-mass spectrometry, 107 differentially abundant metabolites were identified between the IEHM and IELM groups, and 100 differentially abundant metabolites were identified between the IEHF and IELF groups. Based on these metabolites, a large number of enriched metabolic pathways related to muscle elasticity were identified. Significant differences in the intestinal metabolism between groups with different muscle elasticities were identified. Moreover, the model of the relationship between the intestinal flora and metabolites was constructed, and the molecular mechanism of intestinal flora regulation of the nutrient metabolism was further revealed. The results help to understand the molecular mechanism of different muscle elasticities of LYC and provide an important reference for the study of the mechanism of the effects of LYC intestinal symbiotic bacteria on muscle development, and the development and application of probiotics in LYC. Full article
(This article belongs to the Section Animal Genetics and Genomics)
Show Figures

Figure 1

Figure 1
<p>Muscle elastic characteristics of LYCs.</p>
Full article ">Figure 2
<p>Agarose gel electrophoresis for sex determination in LYCs.</p>
Full article ">Figure 3
<p>Structural analysis of the LYC intestinal flora. (<b>a</b>) Male LYC intestinal flora at the phylum level; (<b>b</b>) Female LYC intestinal flora at the phylum level; (<b>c</b>) Male LYC intestinal flora at the genus level; (<b>d</b>) Female LYC intestinal flora at the genus level; (<b>e</b>) Male LYC intestinal flora at the species level; (<b>f</b>) Female LYC intestinal flora at the species level; (<b>g</b>) Male LYC intestinal flora Alpha diversity analysis; (<b>h</b>) Female LYC intestinal flora Alpha diversity analysis. * <span class="html-italic">p</span> ≤ 0.05.</p>
Full article ">Figure 4
<p>Analysis of the differences in the gut flora of LYC with different muscle elasticities: (<b>a</b>) Venn diagrams between the IEHM and IELM groups at the genus level; (<b>b</b>) Non-metric multidimensional scaling (NMDS) analysis of the intestinal flora in male LYCs; (<b>c</b>) Principal coordinate analysis (PCoA) of the intestinal flora in male LYCs; (<b>d</b>) Principal component analysis (PCA) of the intestinal flora in male LYCs; (<b>e</b>) Venn diagrams between the IEHF and IELF groups at the genus level.; (<b>f</b>) Non-metric multidimensional scaling (NMDS) analyses of the intestinal flora in female LYCs; (<b>g</b>) Principal coordinate analysis (PCoA) of the intestinal flora in female LYCs; (<b>h</b>) Principal component analysis (PCA) of the intestinal flora in female LYCs.</p>
Full article ">Figure 5
<p>Heat map of the relative abundance of the gut flora. (<b>a</b>) Heat map of the relative abundance of the gut flora in males at the phylum level; (<b>b</b>) Heat map of the relative abundance of the gut flora in females at the phylum level; (<b>c</b>) Heat map of the relative abundance of the gut flora in males at the genus level; (<b>d</b>) Heat map of the relative abundance of the gut flora in females at the genus level; (<b>e</b>) Heat map of the relative abundance of the gut flora in males at the species level; (<b>f</b>) Heat map of the relative abundance of the gut flora in females at the species level; LYC, large yellow croaker; LYC, large yellow croaker; IEHM, intestinal contents of high muscle elasticity males; IELM, intestinal contents of low muscle elasticity males; IEHF, intestinal contents of high muscle elasticity females; IELF, intestinal contents of low muscle elasticity females.</p>
Full article ">Figure 6
<p>Analysis of LYC intestinal metabolites: (<b>a</b>) Intestinal metabolite analysis in male LYCs (Pos, positive ion mode); (<b>b</b>) Intestinal metabolite analysis in male LYCs (Neg, negative ion mode); (<b>c</b>) Intestinal metabolite analysis in female LYCs (positive ion mode); (<b>d</b>) Intestinal metabolite analysis in female LYCs (negative ion mode); (<b>e</b>) Differential metabolite analysis of LYC intestinal contents (positive ion mode); (<b>f</b>) Differential metabolite analysis of LYC intestinal contents (negative ion mode).</p>
Full article ">Figure 7
<p>Analysis of LYC intestinal metabolites: (<b>a</b>) Random forest analysis of intestinal metabolites in male LYCs; (<b>b</b>) Random forest analysis of intestinal metabolites in female LYCs; (<b>c</b>) Differential metabolite enriched pathway analysis of intestinal contents in male LYCs; (<b>d</b>) Differential metabolite enriched pathway analysis of intestinal contents in female LYCs. LYC, large yellow croaker; IEHM, intestinal contents of high muscle elasticity males; IELM, intestinal contents of low muscle elasticity males; IEHF, intestinal contents of high muscle elasticity females; IELF, intestinal contents of low muscle elasticity females; PC2, principal component 2.</p>
Full article ">Figure 8
<p>Association analysis of the LYC gut flora with differentially abundant metabolites. (<b>a</b>) male LYCs; (<b>b</b>) female LYCs. LYC, large yellow croak. The symbol * is the degree to which the metabolite is associated with a particular flora, where * is a significant association and ** is a very significant association. (<a href="#animals-14-02690-f008" class="html-fig">Figure 8</a>a,b).</p>
Full article ">
23 pages, 2541 KiB  
Article
Biostimulants Enhance the Nutritional Quality of Soilless Greenhouse Tomatoes
by Hayriye Yildiz Dasgan, Kahraman S. Aksu, Kamran Zikaria and Nazim S. Gruda
Plants 2024, 13(18), 2587; https://doi.org/10.3390/plants13182587 - 15 Sep 2024
Viewed by 235
Abstract
The application of biostimulants in vegetable cultivation has emerged as a promising approach to enhance the nutritional quality of crops, particularly in controlled environment agriculture and soilless culture systems. In this study, we employed a rigorous methodology, applying various biostimulants amino acids, Plant [...] Read more.
The application of biostimulants in vegetable cultivation has emerged as a promising approach to enhance the nutritional quality of crops, particularly in controlled environment agriculture and soilless culture systems. In this study, we employed a rigorous methodology, applying various biostimulants amino acids, Plant Growth-Promoting Rhizobacteria (PGPR), fulvic acid, chitosan, and vermicompost along with mineral fertilizers, both foliar and via the roots, to soilless greenhouse tomatoes during spring cultivation. The experiment, conducted in a coir pith medium using the ‘Samyeli F1’ tomato cultivar, demonstrated that plants treated with biostimulants performed better than control plants. Notable variations in nutritional components were observed across treatments. PGPR had the best effects on the physical properties of the tomato fruit, showing the highest fruit weight, fruit length, equatorial diameter, fruit volume, fruit skin elasticity, and fruit flesh hardness while maintaining high color parameters L, a, and b. PGPR and fulvic acid demonstrated significant enhancements in total phenolics and flavonoids, suggesting potential boosts in antioxidant properties. Amioacid and vermicompost notably elevated total soluble solids, indicating potential fruit sweetness and overall taste improvements. On the other hand, vermicompost stood out for its ability to elevate total phenolics and flavonoids while enhancing vitamin C content, indicating a comprehensive enhancement of nutritional quality. In addition, vermicompost had the most significant impact on plant growth parameters and total yield, achieving a 43% increase over the control with a total yield of 10.39 kg/m2. These findings underline the specific nutritional benefits of different biostimulants, offering valuable insights for optimizing tomato cultivation practices to yield produce with enhanced health-promoting properties. Full article
17 pages, 3885 KiB  
Article
Rheological Characterization of Genipin-Based Crosslinking Pigment and O-Carboxymethyl Chitosan–Oxidized Hyaluronic Acid In Situ Formulable Hydrogels
by Ivo Marquis Beserra Junior, Débora de Sousa Lopes, Milena Costa da Silva Barbosa, João Emídio da Silva Neto, Henrique Nunes da Silva, Marcus Vinícius Lia Fook, Rômulo Feitosa Navarro and Suédina Maria de Lima Silva
Polymers 2024, 16(18), 2615; https://doi.org/10.3390/polym16182615 - 15 Sep 2024
Viewed by 277
Abstract
The aim of this study was to develop a material capable of rapidly absorbing bodily fluids and forming a resilient, adhesive, viscoelastic hydrogel in situ to prevent post-surgical adhesions. This material was formulated using O-carboxymethyl chitosan (O-CMCS), oxidized hyaluronic acid (OHA), and a [...] Read more.
The aim of this study was to develop a material capable of rapidly absorbing bodily fluids and forming a resilient, adhesive, viscoelastic hydrogel in situ to prevent post-surgical adhesions. This material was formulated using O-carboxymethyl chitosan (O-CMCS), oxidized hyaluronic acid (OHA), and a crosslinking pigment derived from genipin and glutamic acid (G/GluP). Both crosslinked (O-CMCS/OHA-G/GluP) and non-crosslinked hydrogels (O-CMCS/OHA) were evaluated using a HAAKE™ MARS™ rheometer for their potential as post-surgical barriers. A rheological analysis, including dynamic oscillatory measurements, revealed that the crosslinked hydrogels exhibited significantly higher elastic moduli (G′), indicating superior gel formation and mechanical stability compared to non-crosslinked hydrogels. The G/GluP crosslinker enhanced gel stability by increasing the separation between G′ and G″ and achieving a lower loss tangent (tan δ < 1.0), indicating robustness under dynamic physiological conditions. The rapid hydration and gelation properties of the hydrogels underscore their effectiveness as physical barriers. Furthermore, the O-CMCS/OHA-G/GluP hydrogel demonstrated rapid self-healing and efficient application via spraying or spreading, with tissue adherence and viscoelasticity to facilitate movement between tissues and organs, effectively preventing adhesions. Additionally, the hydrogel proved to be both cost effective and scalable, highlighting its potential for clinical applications aimed at preventing post-surgical adhesions. Full article
(This article belongs to the Special Issue Study in Chitosan and Crosslinked Chitosan Nanoparticles)
Show Figures

Figure 1

Figure 1
<p>Reactions involved in the synthesis of O-CMCS (<b>a</b>), visual presentation of O-CMCS (<b>b</b>), and FTIR spectra of CS and O-CMCS (<b>c</b>).</p>
Full article ">Figure 2
<p>Reactions involved in the synthesis of OHA (<b>a</b>), visual presentation of OHA (<b>b</b>), and FTIR spectra of HA and OHA (<b>c</b>).</p>
Full article ">Figure 3
<p>Visual presentation of crosslinker pigment G/GluP (<b>a</b>), reactions involved in the synthesis of G/GluP (<b>b</b>), and FTIR spectra of Glu, G, and G/GluP (<b>c</b>).</p>
Full article ">Figure 4
<p>Visual presentation of powders without crosslinker (O-CMCS/OHA100, O-CMCS/OHA75, O-CMCS/OHA50, and O-CMCS/OHA25) (<b>a</b>) and with crosslinker (O-CMCS/OHA100-G/GluP, O-CMCS/OHA75-G/GluP, and O-CMCS/OHA50-G/GluP) (<b>b</b>).</p>
Full article ">Figure 5
<p>Reactions involved in the synthesis of crosslinked powder (<b>a</b>) and FTIR spectra of G/GluP and powders without crosslinker (O-CMCS/OHA100) and with crosslinker (O-CMCS/OHA100-G/GluP) (<b>b</b>).</p>
Full article ">Figure 6
<p>Curves of <span class="html-italic">G</span>′ and <span class="html-italic">G</span>″ as a function of frequency for the hydrogel prepared with the crosslinker pigment (O-CMCS/OHA100-G/GluP) (<b>a</b>) and without the crosslinker pigment (O-CMCS/OHA100) (<b>b</b>).</p>
Full article ">Figure 7
<p>Curve of tan <span class="html-italic">δ</span> as a function of frequency for the O-CMCS/OHA100 hydrogel crosslinked with the G/GluP pigment (O-CMCS/OHA100-G/GluP HG).</p>
Full article ">Figure 8
<p>Curves of the complex modulus as a function of frequency for the O-CMCS/OHA100 hydrogel crosslinked with the G/GluP pigment (O-CMCS/OHA100-G/GluP HG).</p>
Full article ">Figure 9
<p>Curve of the complex viscosity as a function of frequency for the O-CMCS/OHA100 hydrogel crosslinked with the G/GluP pigment (O-CMCS/OHA100-G/GluP HG).</p>
Full article ">
22 pages, 6630 KiB  
Article
Tribological Properties of Nitrate Graphite Foils
by Nikolai S. Morozov, David V. Demchenko, Pavel O. Bukovsky, Anastasiya A. Yakovenko, Vladimir A. Shulyak, Alexandra V. Gracheva, Sergei N. Chebotarev, Irina G. Goryacheva and Viktor V. Avdeev
Nanomaterials 2024, 14(18), 1499; https://doi.org/10.3390/nano14181499 - 15 Sep 2024
Viewed by 160
Abstract
This study investigates the tribological properties of graphite foils (GF) with densities of 1.0, 1.3, and 1.6 g/cm3, produced from purified natural graphite of different particle sizes (40–80 μm, 160–200 μm, >500 μm). Surface roughness was measured after cold rolling and [...] Read more.
This study investigates the tribological properties of graphite foils (GF) with densities of 1.0, 1.3, and 1.6 g/cm3, produced from purified natural graphite of different particle sizes (40–80 μm, 160–200 μm, >500 μm). Surface roughness was measured after cold rolling and friction testing at static (0.001 mm/s) and dynamic conditions (0.1 Hz and 1 Hz). Results showed that static friction tests yielded similar roughness values (Sa ≈ 0.5–0.7 μm, Sq ≈ 0.5–1.0 μm) across all densities and particle sizes. Dynamic friction tests revealed increased roughness (Sa from 0.7 to 3.5 μm, Sq from 1.0 to 6.0–7.0 μm). Friction coefficients (µ) decreased with higher sliding speeds, ranging from 0.22 to 0.13. GF with 40–80 μm particles had the lowest friction coefficient (µ = 0.13–0.15), while 160–200 μm particles had the highest (µ = 0.15–0.22). Density changes had minimal impact on friction for the 40–80 μm fraction but reduced friction for the 160–200 μm fraction. Young’s modulus increased with density and decreased with particle size, showing values from 127–274 MPa for 40–80 μm, 104–212 MPa for 160–200 μm, and 82–184 MPa for >500 μm. The stress–strain state in the graphite foil samples was simulated under normal and tangential loads. This makes it possible to investigate the effect of the anisotropy of the material on the stress concentration inside the sample, as well as to estimate the elasticity modulus under normal compression. Structural analyses indicated greater plastic deformation in GF with 40–80 μm particles, reducing coherent-scattering region size from 28 nm to 24 nm. GF samples from 160–200 μm and >500 μm fractions showed similar changes, expanding with density increase from 18 nm to 22 nm. Misorientation angles of GF nanocrystallites decreased from 30° to 27° along the rolling direction (RD). The coherent scattering regions of GF with 40–80 μm particles increased, but no significant changes in the coherent scattering regions were observed for the 160–200 μm and >500 μm fractions during dynamic friction tests. Microstrains and residual macrostresses in GF increased with density for all fractions, expanding under higher friction-induced loads. Higher values of both stresses indicate a higher level of accumulated deformation, which appears to be an additional factor affecting the samples during friction testing. This is reflected in the correlation of the results with the roughness and friction coefficient data of the tested samples. Full article
(This article belongs to the Section 2D and Carbon Nanomaterials)
Show Figures

Figure 1

Figure 1
<p>Schematic diagram of the experiment: 1—steel counterbody (also green), 2—GF sample (also red), 3—a holder (also blue), orange—fasteners, <span class="html-italic">F</span>—normal load, <span class="html-italic">ω</span>—the frequency ofreciprocating motion.</p>
Full article ">Figure 2
<p>Geometry and computational grid for normal load.</p>
Full article ">Figure 3
<p>Geometry and computational grid for the tangential loading.</p>
Full article ">Figure 4
<p>Topography of the original GF surfaces for the density of 1.0 g/cm<sup>3</sup> (<b>a</b>,<b>d</b>,<b>g</b>), 1.3 g/cm<sup>3</sup> (<b>b</b>,<b>e</b>,<b>h</b>), 1.6 g/cm<sup>3</sup> (<b>c</b>,<b>f</b>,<b>i</b>) by the fractions of 40–80 μm (<b>a</b>–<b>c</b>), 160–200 μsam (<b>d</b>–<b>f</b>), and &gt;500 μm (<b>g</b>–<b>i</b>).</p>
Full article ">Figure 5
<p>Topography of the GF surfaces for the density of 1.0 g/cm<sup>3</sup> (<b>a</b>–<b>c</b>), 1.3 g/cm<sup>3</sup> (<b>d</b>–<b>f</b>), and 1.6 g/cm<sup>3</sup> (<b>g</b>–<b>i</b>) obtained from the fractions of 40–80 μm following the experimental studies at the sliding velocity of 1 μm/s (<b>a</b>,<b>d</b>,<b>g</b>), frequency 0.1 Hz (<b>b</b>,<b>d</b>,<b>h</b>), and 1 Hz (<b>c</b>,<b>f</b>,<b>i</b>).</p>
Full article ">Figure 6
<p>Relationship between the value of average roughness and the density in the graphite foils by the fractions of 40–80 μm (<b>a</b>), 160–200 μm (<b>b</b>), &gt;500 μm (<b>c</b>) before (the black lines) and after (the colored lines) the frictions testings.</p>
Full article ">Figure 7
<p>A typical view of recording static (<b>a</b>) and dynamic (<b>b</b>) friction coefficients on a UMT-3MT laboratory tribometer.</p>
Full article ">Figure 8
<p>Relationship between the static (the blue curves) and dynamic (the green and red curves) friction coefficient and the density in the graphite foils by the fractions of 40–80 μm (<b>a</b>), 160–200 μm (<b>b</b>), &gt;500 μm (<b>c</b>).</p>
Full article ">Figure 9
<p>(<b>a</b>) Typical case of the relationship between load (1) and unload (2) and the penetration depth for GF material; (<b>b</b>) the elastic modulus of GF in relation to their density and fractional composition; (<b>c</b>) relationship between the compression depth and the applied load for GF, with the density being 1.0 g/cm<sup>3</sup> by the fraction 40–80 μm (the black curve), 160–200 μm (the red curve), &gt;500 μm (the green curve).</p>
Full article ">Figure 10
<p>Images of the graphite foil from the 40–80 μm fraction in the original state (<b>a</b>), after the testings of static (<b>b</b>) and dynamic frictions at 0.1 Hz (<b>c</b>) and 1.0 Hz (<b>d</b>).</p>
Full article ">Figure 11
<p>Dependences of the vertical displacement of the sample (μm) on the load <span class="html-italic">P</span> (N), obtained numerically (the continuous lines) and experimentally (the dashed lines); (<b>a</b>): linear elasticity, <span class="html-italic">E</span> = 10 MPa (the red line—<math display="inline"><semantics> <mrow> <mi>ν</mi> <mo>=</mo> <mn>0.1</mn> </mrow> </semantics></math>, and the blue line—<math display="inline"><semantics> <mrow> <mi>ν</mi> <mo>=</mo> <mn>0.3</mn> </mrow> </semantics></math>), (<b>b</b>): hyper-elasticity, <math display="inline"><semantics> <mrow> <mi>ν</mi> <mo>=</mo> <mn>0.1</mn> </mrow> </semantics></math> (the red line—<span class="html-italic">E</span> = 9.5 MPa, and the blue line—<span class="html-italic">E</span> = 9.0 MPa, the green line—<span class="html-italic">E</span> = 8.5 MPa), (<b>c</b>): hyper-elasticity, <math display="inline"><semantics> <mrow> <mi>ν</mi> <mo>=</mo> <mn>0.3</mn> </mrow> </semantics></math> (the red line—<span class="html-italic">E</span> = 7.5 MPa, the blue line—<span class="html-italic">E</span> = 7 MPa, the green line—<span class="html-italic">E</span> = 6.5 MPa).</p>
Full article ">Figure 12
<p>The outcome of the numerical modeling for vertical displacement at 350 μm (von Mises stress distribution over the sample volume, Pa); (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>ν</mi> <mo>=</mo> <mn>0.1</mn> </mrow> </semantics></math>, (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>ν</mi> <mo>=</mo> <mn>0.3</mn> </mrow> </semantics></math>, and distribution of the stress tensor component <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>τ</mi> </mrow> <mrow> <mi>y</mi> <mi>z</mi> </mrow> </msub> </mrow> </semantics></math>, Pa, in the bar following application of the tangential forces in the middle plane <span class="html-italic">Oyz</span>; (<b>c</b>) isotropic material, (<b>d</b>) anisotropic material.</p>
Full article ">Figure 13
<p>The size of the coherent–scattering region in relation to density in the graphite foils, by the fractions of 40–80 μm (<b>a</b>), 160–200 μm (<b>b</b>), &gt;500 μm (<b>c</b>), before (the black lines) and after (the colored lines) the friction testings.</p>
Full article ">Figure 14
<p>The misorientation angle size for the nanocrystallites in relation to the density in the graphite foils by the fractions of 40–80 μm (<b>a</b>), 160–200 μm (<b>b</b>), &gt;500 μm (<b>c</b>) in RD, and from similar fractions in TD (<b>d</b>–<b>f</b>) before (the black lines) and after (the colored lines) the friction testings.</p>
Full article ">Figure 15
<p>The microstrain values in the nanocrystallites in relation to the density in the graphite foils by the fractions of 40–80 μm (<b>a</b>), 160–200 μm (<b>b</b>), &gt;500 μm (<b>c</b>) before (the black lines) and after (the colored lines) the friction testings.</p>
Full article ">Figure 16
<p>The macrostrains values in relation to the density in the graphite foils by the fractions of 40–80 μm (<b>a</b>), 160–200 μm (<b>b</b>), &gt;500 μm (<b>c</b>) in RD, and from similar fractions in TD (<b>d</b>–<b>f</b>) before (the black lines) and after (the colored lines) the friction tests.</p>
Full article ">
17 pages, 5959 KiB  
Article
Effects of Different Cooling Treatments on Heated Granite: Insights from the Physical and Mechanical Characteristics
by Qinming Liang, Gun Huang, Jinyong Huang, Jie Zheng, Yueshun Wang and Qiang Cheng
Materials 2024, 17(18), 4539; https://doi.org/10.3390/ma17184539 - 15 Sep 2024
Viewed by 220
Abstract
The exploration of Hot Dry Rock (HDR) geothermal energy is essential to fulfill the energy demands of the increasing population. Investigating the physical and mechanical properties of heated rock under different cooling methods has significant implications for the exploitation of HDR. In this [...] Read more.
The exploration of Hot Dry Rock (HDR) geothermal energy is essential to fulfill the energy demands of the increasing population. Investigating the physical and mechanical properties of heated rock under different cooling methods has significant implications for the exploitation of HDR. In this study, ultrasonic testing, uniaxial strength compression experiments, Brazilian splitting tests, nuclear magnetic resonance (NMR), and scanning electron microscope (SEM) were conducted on heated granite after different cooling methods, including cooling in air, cooling in water, cooling in liquid nitrogen, and cycle cooling in liquid nitrogen. The results demonstrated that the density, P-wave velocity (Vp), uniaxial compressive strength (UCS), tensile strength (σt), and elastic modulus (E) of heated granite tend to decrease as the cooling rate increases. Notably, heated granite subjected to cyclic liquid nitrogen cooling exhibits a more pronounced decline in physical and mechanical properties and a higher degree of damage. Furthermore, the cooling treatments also lead to an increase in rock pore size and porosity. At a faster cooling rate, the fracture surfaces of the granite transition from smooth to rough, suggesting enhanced fracture propagation and complexity. These findings provide critical theoretical insights into optimizing stimulation performance strategies for HDR exploitation. Full article
(This article belongs to the Special Issue Manufacturing, Characterization and Modeling of Advanced Materials)
Show Figures

Figure 1

Figure 1
<p>Samples and equipment. (<b>a</b>) Specimens for uniaxial compression strength experiment and Brazilian split tests. (<b>b</b>) MTS815 experimental apparatus. (<b>c</b>) AG-250kN IS Electronic Precision Material Testing Machine.</p>
Full article ">Figure 2
<p>Changes in mass loss rate and volume expansion rate of granite under different heating temperatures and cooling treatments. (<b>a</b>) Results of the temperature at 200 °C. (<b>b</b>) Results of the temperature at 300 °C.</p>
Full article ">Figure 3
<p>Density changes of granite after different cooling methods. (<b>a</b>) Results of the temperature at 200 °C. (<b>b</b>) Results of the temperature at 300 °C.</p>
Full article ">Figure 4
<p>Changes of <span class="html-italic">V</span><sub>p</sub> of granite treated with different cooling methods. (<b>a</b>) Results of the temperature at 200 °C. (<b>b</b>) Results of the temperature at 300 °C.</p>
Full article ">Figure 5
<p>Uniaxial compressive strength of granite after different cooling treatments.</p>
Full article ">Figure 6
<p>Changes in the tensile strength of granite under different cooling methods.</p>
Full article ">Figure 7
<p>Changes of elastic modulus of granite under different cooling methods.</p>
Full article ">Figure 8
<p>Pore size distribution of heated granite samples under different cooling methods. (<b>a</b>) Results of the temperature at 200 °C. (<b>b</b>) Results of the temperature at 300 °C.</p>
Full article ">Figure 9
<p>Changes in granite porosity under different cooling methods.</p>
Full article ">Figure 10
<p>Morphology of fracture surfaces of heated granite under different cooling treatments at 200 °C.</p>
Full article ">Figure 11
<p>Morphology of fracture surfaces of heated granite under different cooling treatments at 300 °C.</p>
Full article ">Figure 12
<p>Changes in <span class="html-italic">D</span> of heated granite under different cooling methods.</p>
Full article ">
17 pages, 11151 KiB  
Article
Electrical Impedance Tomography-Based Electronic Skin for Multi-Touch Tactile Sensing Using Hydrogel Material and FISTA Algorithm
by Zhentao Jiang, Zhiyuan Xu, Mingfu Li, Hui Zeng, Fan Gong and Yuke Tang
Sensors 2024, 24(18), 5985; https://doi.org/10.3390/s24185985 - 15 Sep 2024
Viewed by 208
Abstract
Flexible electronic skin (e-skin) can enable robots to have sensory forms similar to human skin, enhancing their ability to obtain more information from touch. The non-invasive nature of electrical impedance tomography (EIT) technology allows electrodes to be arranged only at the edges of [...] Read more.
Flexible electronic skin (e-skin) can enable robots to have sensory forms similar to human skin, enhancing their ability to obtain more information from touch. The non-invasive nature of electrical impedance tomography (EIT) technology allows electrodes to be arranged only at the edges of the skin, ensuring the stretchability and elasticity of the skin’s interior. However, the image quality reconstructed by EIT technology has deteriorated in multi-touch identification, where it is challenging to clearly reflect the number of touchpoints and accurately size the touch areas. This paper proposed an EIT-based flexible tactile sensor that employs self-made hydrogel material as the primary sensing medium. The sensor’s structure, fabrication process, and tactile imaging principle were elaborated. To improve the quality of image reconstruction, the fast iterative shrinkage-thresholding algorithm (FISTA) was embedded into the EIDORS toolkit. The performances of the e-skin in aspects of assessing the touching area, quantitative force sensing and multi-touch identification were examined. Results showed that the mean intersection over union (MIoU) of the reconstructed images was improved up to 0.84, and the tactile position can be accurately imaged in the case of the number of the touchpoints up to seven (larger than two to four touchpoints in existing studies), proving that the combination of the proposed sensor and imaging algorithm has high sensitivity and accuracy in multi-touch tactile sensing. The presented e-skin shows potential promise for the application in complex human–robot interaction (HRI) environments, such as prosthetics and wearable devices. Full article
(This article belongs to the Section Physical Sensors)
Show Figures

Figure 1

Figure 1
<p>The working mechanism of EIT. (<b>a</b>) The basic working principle of the 16-electrode EIT system. (<b>b</b>) Discretizing the domain of the sensing material into a collection of a finite number of elements and nodes using the finite element method. (<b>c</b>) Sensitivity matrix composed of discrete grid cells.</p>
Full article ">Figure 2
<p>Imaging process of EIT-based tactile sensor. <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>U</mi> </mrow> <mrow> <mi>m</mi> <mo>×</mo> <mn>1</mn> </mrow> </msub> </mrow> </semantics></math> represents boundary voltage data, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>S</mi> </mrow> <mrow> <mi>m</mi> <mo>×</mo> <mi>n</mi> </mrow> </msub> </mrow> </semantics></math> represents the sensitivity matrix, and <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>g</mi> </mrow> <mrow> <mi>n</mi> <mo>×</mo> <mn>1</mn> </mrow> </msub> </mrow> </semantics></math> represents the conductivity distribution of all grid cells in Ω.</p>
Full article ">Figure 3
<p>CAD drawing of the sensor container. (<b>a</b>) Resin housing and (<b>b</b>) copper electrodes assembled at the boundary of the housing. Dimensions are given in mm.</p>
Full article ">Figure 4
<p>(<b>a</b>) The proposed EIT-based flexible sensor. (<b>b</b>) The waveform of boundary voltage in the case of a homogeneous field.</p>
Full article ">Figure 5
<p>The touch mechanism of an EIT-based tactile sensor. (<b>a</b>) The conventional touch-detection mechanism. Physical compression causes material deformation, which leads to a change in the electrical resistance. (<b>b</b>) The hydrogel-based sensor touch-detection mechanism. Both the touch of highly conductive materials and the compression caused by pressure result in electrical resistance changes, which makes the hydrogel-based skin more sensitive to conductive changes.</p>
Full article ">Figure 6
<p>Block diagrams of the (<b>a</b>) EIT system and (<b>b</b>) main components of the hardware.</p>
Full article ">Figure 7
<p>Imaging results of single- and multi-touch detection with different algorithms on EIT-based tactile sensor.</p>
Full article ">Figure 8
<p>MIoU values for image reconstruction using the proposed method (FISTA) and other traditional methods.</p>
Full article ">Figure 9
<p>(<b>a</b>) Diagram of the position-moving weights at different touchpoints. A metal sheet is placed under the weights to maintain the same area of force. (<b>b</b>) Photo of the weights of different masses.</p>
Full article ">Figure 10
<p>Reconstructed images of different masses of the weights applied on the hydrogel-based skin.</p>
Full article ">Figure 11
<p>Relationship between the magnitude of weights and relative change in conductivity at different touchpoints. The slope of the fitted lines through data points indicates the relative magnitude of the sensitivity in different area (k<sub>1</sub> &lt; k<sub>2</sub> &lt; k<sub>3</sub> &lt; k<sub>4</sub>).</p>
Full article ">Figure 12
<p>Weights applied onto the equally spaced 2 to 7 touchpoints of the sensor and the corresponding reconstructed images.</p>
Full article ">
16 pages, 8326 KiB  
Article
Cytoarchitecture of Breast Cancer Cells under Diabetic Conditions: Role of Regulatory Kinases—Rho Kinase and Focal Adhesion Kinase
by Diganta Dutta, Matthew Ziemke, Payton Sindelar, Hernan Vargas, Jung Yul Lim and Surabhi Chandra
Cancers 2024, 16(18), 3166; https://doi.org/10.3390/cancers16183166 - 15 Sep 2024
Viewed by 224
Abstract
Diabetes greatly reduces the survival rates in breast cancer patients due to chemoresistance and metastasis. Reorganization of the cytoskeleton is crucial to cell migration and metastasis. Regulatory cytoskeletal protein kinases such as the Rho kinase (ROCK) and focal adhesion kinase (FAK) play a [...] Read more.
Diabetes greatly reduces the survival rates in breast cancer patients due to chemoresistance and metastasis. Reorganization of the cytoskeleton is crucial to cell migration and metastasis. Regulatory cytoskeletal protein kinases such as the Rho kinase (ROCK) and focal adhesion kinase (FAK) play a key role in cell mobility and have been shown to be affected in cancer. It is hypothesized that diabetes/high-glucose conditions alter the cytoskeletal structure and, thus, the elasticity of breast cancer cells through the ROCK and FAK pathway, which can cause rapid metastasis of cancer. The aim of the study was to investigate the role of potential mediators that affect the morphology of cancer cells in diabetes, thus leading to aggressive cancer. Breast cancer cells (MDA-MB-231 and MCF-7) were treated with 5 mM glucose (low glucose) or 25 mM glucose (high glucose) in the presence of Rho kinase inhibitor (Y-27632, 10 mM) or FAK inhibitor (10 mM). Cell morphology and elasticity were monitored using atomic force microscopy (AFM), and actin staining was performed by fluorescence microscopy. For comparative study, normal mammary breast epithelial cells (MCF-10A) were used. It was observed that high-glucose treatments modified the cytoskeleton of the cells, as observed through AFM and fluorescence microscopy, and significantly reduced the elasticity of the cells. Blocking the ROCK or FAK pathway diminished the high-glucose effects. These changes were more evident in the breast cancer cells as compared to the normal cells. This study improves the knowledge on the cytoarchitecture properties of diabetic breast cancer cells and provides potential pathways that can be targeted to prevent such effects. Full article
(This article belongs to the Special Issue Application of Imaging in Breast Cancer)
Show Figures

Figure 1

Figure 1
<p>Atomic force microscopy of triple negative breast cancer cells (MDA-MB-231) treated with varying concentrations of glucose. Cells treated with (<b>a</b>) low glucose 5 mM and (<b>b</b>) high glucose 25 mM.</p>
Full article ">Figure 2
<p>Atomic force microscopy of triple negative breast cancer cells (MDA-MB-231) treated with varying concentrations of glucose in presence of Rho kinase inhibitor Y-27,632 (Y, 10 mM) for 24 h. Cells treated with (<b>a</b>) low glucose (5 mM) in combination with Y (10 mM) and (<b>b</b>) high glucose (25 mM) in combination with Y (10 mM).</p>
Full article ">Figure 3
<p>Atomic force microscopy of triple negative breast cancer cells (MDA-MB-231) treated with varying glucose in presence of FAK inhibitor (F, 10 mM) for 24 h. Cells treated with low glucose (5 mM) in combination with F (10 mM). The red dotted square highlights a region further magnified to the right.</p>
Full article ">Figure 4
<p>Atomic force microscopy of breast cancer cells (MCF-7) treated with varying concentrations of glucose for 24 h. Cells treated with (<b>a</b>) low glucose 5 mM and (<b>b</b>) high glucose 25 mM.</p>
Full article ">Figure 5
<p>Atomic force microscopy of breast cancer cells (MCF-7) treated with varying concentrations of glucose in presence of Rho kinase inhibitor Y-27632 (Y, 10 mM) for 24 h. Cells treated with (<b>a</b>) low glucose (5 mM) in combination with Y (10 mM) and (<b>b</b>) high glucose (25 mM) in combination with Y (10 mM).</p>
Full article ">Figure 6
<p>Atomic force microscopy of normal mammary epithelial cells (MCF-10A) treated with varying concentrations of glucose for 24 h. Cells treated with (<b>a</b>) low glucose 5 mM and (<b>b</b>) high glucose 25 mM.</p>
Full article ">Figure 7
<p>Modulus of elasticity of MDA-MB-231 cells treated with varying concentrations of glucose in the presence of the Y compound. Cells were treated for 24 h with low glucose (5 mM, 5G), high glucose (25 mM, 25G), low glucose with inhibitor (5G + Y), and high glucose with inhibitor (25G + Y). N = 28~75.</p>
Full article ">Figure 8
<p>Modulus of elasticity of MDA-MB-231 cells treated with varying concentrations of glucose in the presence of the F compound. Cells were treated for 24 h with low glucose (5 mM, 5G), high glucose (25 mM, 25G), low glucose with inhibitor (5G + F), and high glucose with inhibitor (25G + F). N = 50~83.</p>
Full article ">Figure 9
<p>Modulus of elasticity of MCF-7 cells treated with varying concentrations of glucose in the presence of the F compound. Cells were treated for 24 h with low glucose (5 mM, 5G), high glucose (25 mM, 25G), low glucose with inhibitor (5G + F), and high glucose with inhibitor (25G + F). N = 40~50.</p>
Full article ">Figure 10
<p>Modulus of elasticity of MCF-10A cells treated with varying concentrations of glucose in the presence of the Y compound. Cells were treated for 24 h with low glucose (5 mM, 5G), high glucose (25 mM, 25G), low glucose with inhibitor (5G + Y), and high glucose with inhibitor (25G + Y). N = 78~38.</p>
Full article ">Figure 11
<p>Actin staining of MDA-MB-231 cells treated with varying concentrations of glucose in the presence of the F compound. Cells were treated for 24 h with (<b>a</b>) low glucose (5 mM, 5G), (<b>b</b>) high glucose (25 mM, 25G), (<b>c</b>) low glucose with inhibitor (5G + F), and (<b>d</b>) high glucose with inhibitor (25G + F).</p>
Full article ">
11 pages, 3831 KiB  
Article
A Custom-Developed Device for Testing Tensile Strength and Elasticity of Vascular and Intestinal Tissue Samples for Anastomosis Regeneration Research
by Zoltan Attila Godo, Laszlo Adam Fazekas, Gergo Fritsch, Balazs Szabo and Norbert Nemeth
Sensors 2024, 24(18), 5984; https://doi.org/10.3390/s24185984 - 15 Sep 2024
Viewed by 293
Abstract
Optimizing the regeneration process of surgically created anastomoses (blood vessels, intestines, nerves) is an important topic in surgical research. One of the most interesting parameter groups is related to the biomechanical properties of the anastomoses. Depending on the regeneration process and its influencing [...] Read more.
Optimizing the regeneration process of surgically created anastomoses (blood vessels, intestines, nerves) is an important topic in surgical research. One of the most interesting parameter groups is related to the biomechanical properties of the anastomoses. Depending on the regeneration process and its influencing factors, tensile strength and other biomechanical features may change during the healing process. Related to the optimal specimen size, the range and accuracy of measurements, and applicability, we have developed a custom-tailored microcontroller-based device. In this paper, we describe the hardware and software configuration of the latest version of the device, including experiences and comparative measurements of tensile strength and elasticity of artificial materials and biopreparate tissue samples. The machine we developed was made up of easily obtainable parts and can be easily reproduced on a low budget. The basic device can apply a force of up to 40 newtons, and can grasp a 0.05–1 cm wide, 0.05–1 cm thick tissue. The length of the test piece on the rail should be between 0.3 and 5 cm. Low production cost, ease of use, and detailed data recording make it a useful tool for experimental surgical research. Full article
(This article belongs to the Special Issue Feature Papers in Biosensors Section 2024)
Show Figures

Figure 1

Figure 1
<p>Representative picture of the structure of the device from different views. A robust frame is required for stable and accurate operation of the instrument.</p>
Full article ">Figure 2
<p>Representative picture of the HJJ-001 type grippers while testing a chicken sciatic nerve (biopreparate).</p>
Full article ">Figure 3
<p>Representative superimposed tensile strength measurements stress–strain curve of different suture materials: (<b>A</b>): 4/0 absorbable polyglycolide-poly (e-caprolactone) copolymer suture material (Simfra, Kollsut, North Miami Beach, FL, USA) which we usually use for bowel anastomosis; (<b>B</b>): 5/0 non-absorbable silk suture material (Silk, SMI, Vith, Belgium) using for teaching purposes. (n = 5 per group; L<sub>0</sub> = 8 mm; motor speed: 1.95 mm/s).</p>
Full article ">Figure 4
<p>Representative tensile strength measurement stress–strain curves of different tissue biopreparates. The different mechanical properties are easily recognizable, even within a single tissue, as separate ruptures of serosa and mucosa layers (motor speed: 1.95 mm/s).</p>
Full article ">Figure 5
<p>Analysis of force–elongation (stress–strain) curve. The initial part of the curve (red) was not included in the slope calculation due to its irregularity (femoral artery biopreparate of a rat; L<sub>0</sub> = 8 mm; motor speed: 1.95 mm/s).</p>
Full article ">Figure 6
<p>Representative analysis of the exported data. There were some irregularities in the beginning (even some negative values) so after the gram/newton conversion we applied a filter (0.0196–maximum). The entire filtered curves were divided into two parts: the first-third (0–33%) and the remaining two-thirds (34–100%). The slope of these curves was determined using the following formula in Excel = SLOPE(known_y’s, known_x’s) where x = LΔ and y = applied force. The calculation was equal to the slope of the regression line: slope = tgα = <math display="inline"><semantics> <mrow> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mo>∑</mo> <mfenced separators="|"> <mrow> <mi>x</mi> <mo>−</mo> <mover accent="true"> <mrow> <mi>x</mi> </mrow> <mo>¯</mo> </mover> </mrow> </mfenced> <mo>∗</mo> <mfenced separators="|"> <mrow> <mi>y</mi> <mo>−</mo> <mover accent="true"> <mrow> <mi>y</mi> </mrow> <mo>¯</mo> </mover> </mrow> </mfenced> </mrow> <mrow> <mo>∑</mo> <msup> <mrow> <mfenced separators="|"> <mrow> <mi>x</mi> <mo>−</mo> <mover accent="true"> <mrow> <mi>x</mi> </mrow> <mo>¯</mo> </mover> </mrow> </mfenced> </mrow> <mrow> <mn>2</mn> </mrow> </msup> </mrow> </mfrac> </mstyle> </mrow> </semantics></math>. (5/0 non-absorbable silk suture material (Silk, SMI, Belgium); L<sub>0</sub> = 8 mm; motor speed: 1.95 mm/s.)</p>
Full article ">
Back to TopTop