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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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Khan, Imran
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (18/18 displayed)
- 2023The impact of plasmonic electrodes on the photocarrier extraction of inverted organic bulk heterojunction solar cellscitations
- 2023The impact of plasmonic electrodes on the photocarrier extraction of inverted organic bulk heterojunction solar cells
- 2023Dodecyltrimethylammonium bromide-styrene microemulsion dielectric investigation in aqueous media
- 2022Biogenic Synthesis of Silver Nanoparticles Using Catharanthus roseus and Its Cytotoxicity Effect on Vero Cell Linescitations
- 2021Correlation between the microstructure and corrosion performance of the HIPIMS nitrided bio-grade CoCrMo alloycitations
- 2021Development of Cd (II) Ion Probe Based on Novel Polyaniline-Multiwalled Carbon Nanotube-3-aminopropyltriethoxylsilane Compositecitations
- 2021A new approach towards performing plasma nitriding of CrCoMo medical grade alloys using HIPIMS dischargecitations
- 2021Efficient Synthesis and Characterization of Polyaniline@Aluminium–Succinate Metal-Organic Frameworks Nanocomposite and Its Application for Zn(II) Ion Sensingcitations
- 2021TiN/NbN nanoscale multilayer coatings deposited by High Power Impulse Magnetron Sputtering to protect medical grade CoCrMo alloyscitations
- 2021TiN/NbN Nanoscale Multilayer Coatings Deposited by High Power Impulse Magnetron Sputtering to Protect Medical-Grade CoCrMo Alloyscitations
- 2020Dry sliding wear mechanisms of HIPIMS plasma nitrided CoCrMo alloy for medical implant applicationscitations
- 2020Surface plasmon resonance excited electron induction greatly extends H<sub>2</sub> evolution and pollutant degradation activity of g‐C<sub>3</sub>N<sub>4</sub> under visible light irradiationcitations
- 2020Low pressure plasma nitrided CoCrMo alloy utilising HIPIMS discharge for biomedical applicationscitations
- 2020Effect of Nitriding Voltage on the Impact Load Fatigue and Fracture Toughness Behaviour of CoCrMo Alloy Nitrided Utilising a HIPIMS Dischargecitations
- 2020Investigation on the effects of the processing parameters and the number of passes on the flexural properties of polymer nanocomposite fabricated through FSP method
- 2019The exploitation of polymer based nanocomposites for additive manufacturing: a prospective reviewcitations
- 2018Rubber-Based Nanocomposites and Significance of Ionic Liquids in Packaging Applications
- 2016Development of superlattice CrNNbN coatings for joint replacements deposited by High Power Impulse Magnetron Sputteringcitations
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article
Dodecyltrimethylammonium bromide-styrene microemulsion dielectric investigation in aqueous media
Abstract
<jats:p> In this paper, we report the complex permittivity of aqueous microemulsions of N-dodecyltrimethylammonium bromide and styrene. The studies were carried out at 298.15 K while varying the styrene to surfactant concentration ratio, S0 (0.16 ≤ So ≤ 0.71) and the surfactant concentration, c (0.1032 ≤c (mol•dm-3 ) ≤ 0.7806). The frequencies ranged from 100 MHz to 89 GHz. An analysis of a particular solution is conducted over the temperature range of 278.15 to 328.15K in order to calculate the energy of the activation parameters. At 298.15 K, the spectra are fitted to a total of five Debye processes for concentration dependency series and three Debye processes for temperature dependence series. Br- surface and bulk diffusion surrounding the micelles best describes the two low frequency dispersions, at 100 MHz and 0.8 GHz, respectively. These mechanisms were examined using Grosse theory. The Maxwell-Wagner relaxation process is equivalent to high frequency micelle dispersion at 0.8 GHz. The thickness of the conducting shell of the micelle is determined by using the electrical conductivity of the particles and parameters taken from the Grosse theory, and the results are comparable to those from an examination of the Pauly and Schwan model. The Grosse model and solvent dispersion analysis were used to calculate the volume fractions of micelles. Both approaches were in agreement. The surfactant head group non-rotationally hydrates almost ~7±1 water molecules. Styrene addition allows for the non-rotationally bound accommodation of an additional ~7±1 water molecules. </jats:p>