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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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Roche, Virginie
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (33/33 displayed)
- 2024The study of passive film's resistivity distribution to crystalline Fe-based pseudo high entropy alloys: The use of measurement model and Cole-Cole regressioncitations
- 2024The study of passive film's resistivity distribution to crystalline Fe-based pseudo high entropy alloys: The use of measurement model and Cole-Cole regressioncitations
- 2024Severe plastic deformation for producing superfunctional ultrafine-grained and heterostructured materials: An interdisciplinary review
- 2024Design, structure/microstructure evolution, mechanical and corrosion properties of newly-developed pseudo-high entropy amorphous alloys
- 2024Passive film's resistivity distribution of crystalline Fe-based pseudo high entropy alloys
- 2024Fe–Ni-based alloys as highly active and low-cost oxygen evolution reaction catalyst in alkaline mediacitations
- 2024Severe plastic deformation for producing Superfunctional ultrafine-grained and heterostructured materials: An interdisciplinary reviewcitations
- 2023Newly-developed pseudo-high entropy amorphous alloys: Structure/microstructure evolution, mechanical and corrosion properties.citations
- 2023Newly-developed pseudo-high entropy amorphous alloys: Structure/microstructure evolution, mechanical and corrosion properties.citations
- 2023Passive film characterization of a novel FeCrMoNbB alloy by combined EIS and XPS
- 2023Erosion-corrosion properties of two novel Fe-based multicomponent alloys for marine applications
- 2022Passive film formation on the new biocompatible non-equiatomicTi 21 Nb 24 Mo 23 Hf 17 Ta 15 high entropy alloy before and after resting in simulated body fluidcitations
- 2022Passive film formation on the new biocompatible non-equiatomicTi 21 Nb 24 Mo 23 Hf 17 Ta 15 high entropy alloy before and after resting in simulated body fluidcitations
- 2022Novel FeCrMoNbB alloy for marine applications: corrosion behavior
- 2022Novel FeCrMoNbB alloy for marine applications: corrosion behavior
- 2021On the effect of plastic pre-straining on the corrosion behaviour of a duplex stainless steel and how the emergence of slip steps affects the hydrogen evolution reaction kineticscitations
- 2021Hydrogen storage in MgAlTiFeNi high entropy alloycitations
- 2021Hydrogen storage in MgAlTiFeNi high entropy alloycitations
- 2021Corrosion behavior and bioactivity of equimolar high entropy alloy TiNbZrHfTa : growth of nanotubes oxides
- 2021Corrosion behaviour of biomedical β-titanium alloys with the surface-modified by chemical etching and electrochemical methodscitations
- 2021Hot Deformation Behavior of a Beta Metastable TMZF Alloy: Microstructural and Constitutive Phenomenological Analysiscitations
- 2021Assessment of anodization conditions and annealing temperature on the microstructure, elastic modulus, and wettability of β-Ti40Nb alloycitations
- 2021Corrosion resistance investigation of surface modified biocompatible β-titanium alloys
- 2020Cathodic protection modeling of a covered and uncovered steel immerse in seawater: Corrosion characterizations
- 2019On the intrinsic passivating ability of Belite-Ye’elimite-Ferrite towards carbon steel: A straightforward comparison with ordinary Portland cementcitations
- 2017Sulfide stress corrosion study of a super martensitic stainless steel in H 2 S sour environments: Metallic sulfides formation and hydrogen embrittlementcitations
- 2017Sulfide stress corrosion study of a super martensitic stainless steel in H<font size=-1><sub>2</sub></font>S sour environments: Metallic sulfides formation and hydrogen embrittlementcitations
- 2017Synergy between molybdenum and nitrogen on the pitting corrosion and passive film resistance of austenitic stainless steels as a pH-dependent effectcitations
- 2017Effect of cold rolling on the structure and hydrogen properties of AZ91 and AM60D magnesium alloys subjected to ECAPcitations
- 2017Molybdenum effect on the Sulfide Stress Corrosion of a super martensitic stainless steel in sour environment highlighted by Electrochemical Impedance Spectroscopycitations
- 2014Corrosion properties of Fe–Cr–Nb–B amorphous alloys and coatingscitations
- 2010CGO-based electrochemical catalysts for low temperature combustion of propenecitations
- 2009Physicochemical Origins of Electrochemical Promotion of LSM/YSZcitations
Places of action
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document
Cathodic protection modeling of a covered and uncovered steel immerse in seawater: Corrosion characterizations
Abstract
As underwater structure, ships are protected by a suitable cathodic protection system to prevent and reduce significantly the corrosion phenomenon. This protective system, called Impressed Current Cathodic Protection (ICCP), creates an underwater electrical current. Then, this current generates an electromagnetic field also referred as electrical signature that could be detectable by sensors. Therefore, this work refers to the electrochemical characterization of the materials used in the naval framework in addition to a better comprehension of the corrosion phenomenon. The final goal is to predict electrical signatures of ships under different corrosion conditions. These predictions will be done by numerical simulations using the models of material that we work on and the simulation software developed by the G2Elab.In a first time, polarization laws of different materials present on the immersed hull and electrically connected are obtained: the hull material DH36 steel (coated and uncoated), the propeller with different material possibilities (stainless steel 316L, martensitic or Nickel Aluminum bronze alloy) and zinc for sacrificial anodes to complete the cathodic protection system. The first step of this project is to be able to model the metal/electrolyte interface following the environmental conditions: speed, temperature, polarization state, aging coating and galvanic coupling. The second step will be to test theses founded models at bigger scale on a ship model. To achieve these goals, it’s important to understand what happens physically at the interface and to model the different corrosion phenomena which take place at the interface. To model interface experimentally, Electrical Equivalent Circuits are used. These Electrical Equivalent Circuits, commonly called EEC, are obtained by fitting Electrochemical Impedance Spectroscopy measurementsdata. To complete EIS investigations and confirm the different models, potentiodynamic curves and Scanning Electron Microscopy with EDX analyses were also performed.From the first results, Electrical Equivalent Circuits (EEC) of the behavior of metallic interface (hull) are proposed for different polarizations and environmental conditions: anodic, corrosion potential and cathodic (ICCP potential: -0,8 VECS). In complement EEC investigations will be made under temperature variations and dynamic conditions for hull steel samples at its corrosion potential. In future experimentations, the propeller material will be characterized following the same type of parameters variations (temperature, speed, polarization state ...)Painted hull steel samples give equivalent results. Whatever experimental conditions, freshly painted hull steel samples show an almost pure capacitance behavior. To model this behavior a simple Randle circuit, which only take into account the impedance of the paint, is used. In case of uncoated hull steel, EEC are more complex and change following the polarization and experimental conditions. In all cases, a deposit is formed but its nature and protective behavior change with polarization: a formation of calcareous deposit under cathodic polarization and corrosion products deposit under anodic polarization. That requires in consequence to include additional impedances in the EEC modeling: impedance of a deposit or diffusion impedance for example. Temperature variation and dynamic conditions influence the kinetic of the different interfacial phenomena.