| People | Locations | Statistics |
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| Naji, M. |
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| Motta, Antonella |
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| Aletan, Dirar |
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| Mohamed, Tarek |
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| Ertürk, Emre |
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| Taccardi, Nicola |
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| Kononenko, Denys |
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| Petrov, R. H. | Madrid |
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| Alshaaer, Mazen | Brussels |
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| Bih, L. |
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| Casati, R. |
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| Muller, Hermance |
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| Kočí, Jan | Prague |
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| Šuljagić, Marija |
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| Kalteremidou, Kalliopi-Artemi | Brussels |
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| Azam, Siraj |
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| Ospanova, Alyiya |
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| Blanpain, Bart |
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| Ali, M. A. |
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| Popa, V. |
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| Rančić, M. |
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| Ollier, Nadège |
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| Azevedo, Nuno Monteiro |
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| Landes, Michael |
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| Rignanese, Gian-Marco |
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Kumar, Deepak
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (17/17 displayed)
- 2024Tuning thermal and structural properties of nano‐filled <scp>PDMS</scp> elastomercitations
- 2024Exploring enhanced structural and dielectric properties in Ag-Doped Sr(NiNb) 0.5 O 3 perovskite ceramic for advanced energy storagecitations
- 2023Manufacturing of aluminium metal matrix composites by high pressure torsion.
- 2023Effect of nanoscale interface modification on residual stress evolution during composite processingcitations
- 2023Wear behavior of bare and coated 18Cr8Ni turbine steel exposed to sediment erosion: A comparative analysiscitations
- 2023Metal‐based nanomaterials and nanocomposites as promising frontier in cancer chemotherapycitations
- 2022The progress and roadmap of metal–organic frameworks for high-performance supercapacitorscitations
- 2022ProTheRaMon - a GATE simulation framework for proton therapy range monitoring using PET imagingcitations
- 2021New Insight into the development of deformation texture in face-centered cubic material
- 2021Reversal of favorable microstructure under plastic ploughing vs. interfacial shear induced wear in aged Co1.5CrFeNi1.5Ti0.5 high-entropy alloycitations
- 2021Microstructural anisotropy in Electron Beam Melted 316L stainless steels
- 2020Towards an improved understanding of plasticity, friction and wear mechanisms in precipitate containing AZ91 Mg alloycitations
- 2020Towards an improved understanding of plasticity, friction and wear mechanisms in precipitate containing AZ91 Mg alloycitations
- 2020Tip Induced Growth of Zinc Oxide Nanoflakes Through Electrochemical Discharge Deposition Process and Their Optical Characterization
- 2019Thin film growth by combinatorial epitaxy for electronic and energy applications ; Croissance de couches minces par épitaxie combinatoire pour applications énergétiques et électroniques
- 2016POLYVINYL BUTYRAL (PVB), VERSETILE TEMPLATE FOR DESIGNING NANOCOMPOSITE/COMPOSITE MATERIALS:A REVIEWcitations
- 2014Soft Colloidal Scaffolds Capable of Elastic Recovery after Large Compressive Strainscitations
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article
Tuning thermal and structural properties of nano‐filled <scp>PDMS</scp> elastomer
Abstract
<jats:title>Abstract</jats:title><jats:sec><jats:label/><jats:p>Increasing the thermal stability and thermal conductivity of polydimethylsiloxane (PDMS) is a crucial issue for thermal applications. This paper focuses on enhancing PDMS's thermal and structural properties by incorporating nanocomposite into the PDMS matrix. An investigation of the impact of rGO‐CaCO<jats:sub>3</jats:sub> nanocomposite on the thermal and structural properties of PDMS was performed using Field Emission Scanning Electron Microscopy (FESEM), X‐ray diffraction (XRD), the thermogravimetric analysis and differential thermal analysis (TGA‐DTA), and thermal analyzer tests. It was observed that PDMS doped with rGO‐CaCO<jats:sub>3</jats:sub> nanocomposite shows better thermal stability, thermal conductivity, and higher crystallinity. The thermal stability was enhanced significantly by adding a 5% rGO‐CaCO<jats:sub>3</jats:sub> nanocomposite, and the initial and end degradation temperatures rose to 492°C and 605°C, respectively. The thermal conductivity of pure PDMS is approximately 0.17 W/mK, whereas a conductive elastomer filled with 5% rGO‐CaCO<jats:sub>3</jats:sub> nanocomposite exhibits a thermal conductivity of 0.44 W/mK at a temperature of 20°C. In contrast, the thermal diffusivity is enhanced from 0.13 mm<jats:sup>2</jats:sup>/s to 0.366 mm<jats:sup>2</jats:sup>/s. Additionally, the Fourier Transform Infra‐Red (FTIR) spectrum at 1411 cm<jats:sup>−1</jats:sup> becomes sharp and noisy, and an additional peak arises at 1398 cm<jats:sup>−1</jats:sup>, corresponding to the vibrational rocking of the CC bond and COC bond in CaCO<jats:sub>3</jats:sub> and rGO.</jats:p></jats:sec><jats:sec><jats:title>Highlights</jats:title><jats:p><jats:list list-type="bullet"> <jats:list-item><jats:p>The manuscript focuses on the development of conductive elastomer by incorporating rGO‐CaCO<jats:sub>3</jats:sub> doped and its effect on the morphology, structure, and thermal properties of PDMS.</jats:p></jats:list-item> <jats:list-item><jats:p>The variation in peak intensity observed in XRD attributed to disparities in the crystalline structure of PDMS due to the inclusion of nanocomposite.</jats:p></jats:list-item> <jats:list-item><jats:p>The thermal degradation range is observed to shift toward the upper end. The degradation temperature at the beginning and end of the process is observed to move to 492°C and 605°C, respectively, upon introducing a 5% rGO‐CaCO<jats:sub>3</jats:sub> nanocomposite.</jats:p></jats:list-item> <jats:list-item><jats:p>The addition of 5% rGO‐CaCO<jats:sub>3</jats:sub> filled conductive elastomers shows a significant improvement of approximately 2.6 times in heat conductivity than bare PDMS.</jats:p></jats:list-item> </jats:list></jats:p></jats:sec>