Hans Brouwer

Mr. Hans Brouwer

orcid

Research Focus & Metrics

Academic Career Length

7Years (2020-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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15 January 2025 in Scripta Materialia
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Journal Article
Open access
ZYZhaorui Yan
Zhaorui Yan
Jianing ZhuJianing Zhu
Jianing Zhu
YYYi-Chieh Yang
Yi-Chieh Yang
HBHans Brouwer
Hans Brouwer
TRTon Riemslag
Ton Riemslag
VPVera Popovich
Vera Popovich

2 September 2025 in Materials Today
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Journal Article
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SSShiv Shankar
Shiv Shankar
BRBarak Ratzker
Barak Ratzker
ASAlisson Kwiatkowski da Silva
Alisson Kwiatkowski da Silva
TSTim M. Schwarz
Tim M. Schwarz
HBHans Brouwer
Hans Brouwer
DRDierk Raabe
Dierk Raabe

20 September 2022 in Materials
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Journal Article
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ATAnton Tuluk
Anton Tuluk
HBHans Brouwer
Hans Brouwer
Sybrand Van Der ZwaagSybrand Van Der Zwaag
Sybrand Van Der Zwaag
BiFeO3 is a multiferroic material with a perovskite structure that has a lot of potential for use in sensors and transducers. However, obtaining pure single-phase BiFeO3 ceramic with a low electrical conductivity via solid-state reactions remains a problem that limits its application. In this work, the suppression of secondary phases in BiFeO3 was studied by varying the compositional parameters and the sintering temperature. The addition of 1% Bi2O3 to the stoichiometric precursor mixture prevented the formation of secondary phases observed when sintering stoichiometric precursors. The pure phase ceramic had a p-type conductivity and a three-decade lower electrical conductivity as measured by impedance spectroscopy. Annealing of optimally synthesized material at different partial pressures of oxygen in an oxygen–nitrogen gas atmosphere showed that the reason for this type of conductivity lies in the high concentration of defects associated with oxygen. By annealing in various mixtures of nitrogen and oxygen, it is possible to control the concentration of these defects and hence the conductivity, which can go down another two decades. At a pO2 ≤10%, the conductivity is determined by intrinsic charge carriers in the material itself.

2 June 2020 in Metals
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JFJia Fu
Jia Fu
JSJurriaan van Slingerland
Jurriaan van Slingerland
HBHans Brouwer
Hans Brouwer
VBVitaliy Bliznuk
Vitaliy Bliznuk
IRIan Richardson
Ian Richardson
Marcel HermansMarcel Hermans
Marcel Hermans
Pulsed laser beam welding was used successfully to join the oxide dispersion-strengthened (ODS) Eurofer steel. The joining was conducted with a laser power of 2500 W and a pulsed duration of 4 ms. With the filler material being used, a minor material loss and microvoids were observed in the joint. The microstructure of the fusion zone consists of dual phase elongated structures. The heat-affected zone has a width of around 0.06 mm with finer grains. The transmission electron microscopy observation reveals that nanoprecipitates are finely distributed in the fusion zone. The tensile strength, yield strength and elongation of the joint are slightly inferior to the base material. The fractography results reveal a typical ductile fracture. The experimental results indicate a reasonable joint from the perspective of both the microstructure and mechanical behaviour.

8 November 2024 in Metals
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PLPhilipp Leerhoff
Philipp Leerhoff
HBHans Brouwer
Hans Brouwer
AAAmir Mohseni Armaki
Amir Mohseni Armaki
CZChristiaan Zeilstra
Christiaan Zeilstra
KMKoen Meijer
Koen Meijer
YYYongxiang Yang
Yongxiang Yang
In the pre-reduction cyclone of the HIsarna process, both thermal decomposition and gas reduction of the injected iron ores occur simultaneously at gas temperatures of 1723–1773 K. In this study, the kinetics of the thermal decomposition of three iron ores (namely OreA, OreB and OreC) for HIsarna ironmaking were analysed as an isolated process with a symmetrical thermogravimetric analyser (TGA) under an inert atmosphere. Using various methods, the chemical and mineralogical composition, particle size distribution, morphology and phase distribution of the ores were analysed. The ores differ in their mineralogy and morphology, where OreA only contains hematite as iron-bearing phase and OreB and OreC include goethite and hematite. To obtain the kinetic parameters in non-isothermal conditions, the Coats–Redfern Integral Method was applied for heating rates of 1, 2 and 5 K/min and a maximum temperature of 1773 K. The TGA results indicate that goethite and hematite decomposition occur as a two-stage process in an inert atmosphere of Ar. The proposed reaction mechanism for the first stage of goethite decomposition is chemical reaction with an activation energy ranging from 46.55 to 60.38 kJ/mol for OreB and from 69.90 to 134.47 kJ/mol for OreC. The proposed reaction mechanism for the second stage of goethite decomposition is diffusion, showing an activation energy ranging between 24.43 and 44.76 kJ/mol for OreB and between 3.32 and 23.29 kJ/mol for OreC. In terms of hematite decomposition, only the first stage was analysed. The proposed reaction mechanism is chemical reaction control. OreA shows an activation energy of 545.47 to 670.50 kJ/mol, OreB one of 587.68 to 831.54 kJ/mol and OreC one of 424.31 to 592.32 kJ/mol.

29 January 2023 in High Temperature Corrosion of Materials
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SAS. Aghaeian
S. Aghaeian
HBHans Brouwer
Hans Brouwer
WSW. G. Sloof
W. G. Sloof
AMArjan Mol
Arjan Mol
ABA. J. Böttger
A. J. Böttger
Since the oxidation reactions in the process of steel production occur in harsh conditions (i.e., high temperatures and gas atmospheres), it is practically impossible to observe in situ the compositional changes in the steel and the formed oxide scale. Hence, a coupled thermodynamic-kinetic numerical model is developed that predicts the formation of oxide phases and the composition profile of the steel alloy’s constituents in a short time due to external oxidation. The model is applied to high-temperature oxidation of Fe–Mn alloys under different conditions. Oxidizing experiments executed with a thermogravimetric analyzer (TGA) on Fe–Mn alloys with different Mn contents (below 10 wt %) are used to determine kinetic parameters that serve as an input for the model. The mass gain data as a function of time show both linear and parabolic regimes. The results of the numerical simulations are presented. The effect of different parameters, such as temperature, Mn content of the alloy, oxygen partial pressure, and oxidizing gas flow rate on the alloy composition and oxide phases formed, is determined. It is shown that increasing the temperature and decreasing the oxygen partial pressure both lead to a thicker depleted area.