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Aziz, Khan Naveed. "RF Magnetron Sputtered AlCoCrCu0.5FeNi High Entropy Alloy (HEA) and High Entropy Ceramic (HEC) Thin Films". Thesis, The University of Sydney, 2021. https://hdl.handle.net/2123/24615.
Pełny tekst źródłaLöbel, Martin, Thomas Lindner, Thomas Mehner i Thomas Lampke. "Microstructure and Wear Resistance of AlCoCrFeNiTi High-Entropy Alloy Coatings Produced by HVOF". Universitätsbibliothek Chemnitz, 2017. http://nbn-resolving.de/urn:nbn:de:bsz:ch1-qucosa-230210.
Pełny tekst źródłaBelous, V. A., S. A. Firstov, V. F. Gorban, A. S. Kuprin, V. D. Ovcharenko, E. N. Reshetnyak, G. N. Tolmachova i M. G. Kholomeev. "Properties of Coatings Deposited from Filtered Vacuum Arc Plasma with HEA Cathode". Thesis, Sumy State University, 2013. http://essuir.sumdu.edu.ua/handle/123456789/35323.
Pełny tekst źródłaSobol, O. V., A. A. Andreev i V. Gorban. "Structural-Strained State and Mechanical Characteristics of Single-Phase Vacuum-Arc Coatings of Multicomponent High Entropy System Ti-V-Zr-Nb-Hf and Nitrides Based On It". Thesis, Sumy State University, 2012. http://essuir.sumdu.edu.ua/handle/123456789/34808.
Pełny tekst źródłaSteneteg, Jakob. "Corrosion Resistant Multi-Component Coatings for Hydrogen Fuel Cells". Thesis, Linköpings universitet, Tunnfilmsfysik, 2021. http://urn.kb.se/resolve?urn=urn:nbn:se:liu:diva-174617.
Pełny tekst źródłaFunMat II
Тевосян, А. А. "Боридні покриття на основі високоентропійних сплавів". Master's thesis, Сумський державний університет, 2019. http://essuir.sumdu.edu.ua/handle/123456789/73025.
Pełny tekst źródłaЛяшко, В. О. "Карбідні покриття на основі високоентропійних сплавів". Master's thesis, Сумський державний університет, 2019. http://essuir.sumdu.edu.ua/handle/123456789/73026.
Pełny tekst źródłaHuser, Gautier. "Etude et sélection d’alliages à composition complexe sans cobalt à finalité tribologique". Thesis, université Paris-Saclay, 2020. http://www.theses.fr/2020UPAST051.
Pełny tekst źródłaCurrently, attempts are made to develop hardfacing cobalt-free alloys for coating the contact areas of moving parts of nuclear installations. In fact, under neutron flux, cobalt 59 is activated into cobalt 60, a highly radioactive isotope. Consequently, the coating debris generated by friction are likely to contaminate parts of the installation. Existing cobalt-free hardfacing alloys, nickel or iron bases, do not exhibit tribological properties competing with those of stellite®, a commonly used hardfacing cobalt base alloy. HEA (High Entropy Alloy) and CCA (Complex Concentration Alloy) may be good candidates. Indeed, compare to conventional alloys, they show vast composition domain giving access to a large range of properties. After an initial selection of elements, the phases of selected alloys were calculated by CALPHAD software (CALculation of PHAse Diagram). The compositions favoring the presence of hard intermetallic phases beneficial to tribological behavior were selected. Then several alloys were fabricated using different processes. From microstructural and tribological characterizations, one composition has been selected as the best potential cobalt-free hardfacing alloy candidate. Coatings of this composition were then fabricated by DLD (Direct Laser Deposition) and HIP (Hot Isostatic Pressing). Their microstructure and tribological behavior were measured and compared to those of stellite ®
Сухонос, Я. В. "Мікроструктура та фізико-механічні властивості боридних багатокомпонентних покриттів". Master's thesis, Сумський державний університет, 2019. http://essuir.sumdu.edu.ua/handle/123456789/76755.
Pełny tekst źródłaKushnerov, O. I. "MD simulation of AlCoCuFeNi high-entropy alloy nanoparticle". Thesis, Sumy State University, 2016. http://essuir.sumdu.edu.ua/handle/123456789/45791.
Pełny tekst źródłaПогребняк, Олександр Дмитрович, Александр Дмитриевич Погребняк, Oleksandr Dmytrovych Pohrebniak, Артем Анатолійович Багдасарян, Артем Анатольевич Багдасарян, Artem Anatoliiovych Bahdasarian, Вадим Миколайович Борисюк, Вадим Николаевич Борисюк, Vadym Mykolaiovych Borysiuk i J. Partyka. "Structure and Morphology of Nitride Coating (TiHfZrVNb)N After Thermal Annealing 600˚C". Thesis, Sumy State University, 2013. http://essuir.sumdu.edu.ua/handle/123456789/35400.
Pełny tekst źródłaNordin, Norhuda Hidayah. "Phase transformation in High Entropy Bulk Metallic Glass (HE-BMG) and Lamellar Structured-High Entropy Alloy (HEA)". Thesis, University of Sheffield, 2018. http://etheses.whiterose.ac.uk/21325/.
Pełny tekst źródłaLöbel, Martin, Thomas Lindner, Robert Pippig i Thomas Lampke. "High-Temperature Wear Behaviour of Spark Plasma Sintered AlCoCrFeNiTi0.5 High-Entropy Alloy". MDPI, 2019. https://monarch.qucosa.de/id/qucosa%3A34386.
Pełny tekst źródłaYe, Jingrui. "Fabrication and Microscopic Characterization of AlCoCrCu0.5FeNi High Entropy Alloy Thin Films". Thesis, The University of Sydney, 2021. https://hdl.handle.net/2123/25793.
Pełny tekst źródłaGwalani, Bharat. "Developing Precipitation Hardenable High Entropy Alloys". Thesis, University of North Texas, 2017. https://digital.library.unt.edu/ark:/67531/metadc1011755/.
Pełny tekst źródłaLiu, Kaimiao. "Linking Enhanced Fatigue Life to Design by Modifying the Microstructure". Thesis, University of North Texas, 2019. https://digital.library.unt.edu/ark:/67531/metadc1538654/.
Pełny tekst źródłaLöbel, Martin, Thomas Lindner i Thomas Lampke. "Enhanced Wear Behaviour of Spark Plasma Sintered AlCoCrFeNiTi High-Entropy Alloy Composites". MDPI AG, 2018. https://monarch.qucosa.de/id/qucosa%3A32461.
Pełny tekst źródłaHasan, Md Nazmul. "Microstructure and mechanical properties of a CrMnFeCoNi high-entropy alloy with gradient structures". Thesis, University of Sydney, 2020. https://hdl.handle.net/2123/23036.
Pełny tekst źródłaLiu, Zhijie. "Application of a pulsed cathodic arc for deposition of high entropy alloy thin films". Thesis, The University of Sydney, 2021. https://hdl.handle.net/2123/27518.
Pełny tekst źródłaAkbari, Azin. "COMBINATORIAL SCREENING APPROACH IN DEVELOPING NON-EQUIATOMIC HIGH ENTROPY ALLOYS". UKnowledge, 2018. https://uknowledge.uky.edu/cme_etds/87.
Pełny tekst źródłaEdris, Hossein. "Studies on high velocity oxy-fuel sprayed coatings of iconel 625 and Ni-Crâ†3Câ†2". Thesis, University of Nottingham, 1997. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.362891.
Pełny tekst źródłaMartin, Alexander Charles. "Initial Weldability of High Entropy Alloys for High Temperature Applications". The Ohio State University, 2019. http://rave.ohiolink.edu/etdc/view?acc_num=osu1555496040477991.
Pełny tekst źródłaJensen, Jacob K. "Characterization of a High Strength, Refractory High Entropy Alloy, AlMo0.5NbTa0.5TiZr". The Ohio State University, 2017. http://rave.ohiolink.edu/etdc/view?acc_num=osu1492175560975813.
Pełny tekst źródłaLöbel, Martin, Thomas Lindner, Thomas Mehner i Thomas Lampke. "Influence of Titanium on Microstructure, Phase Formation and Wear Behaviour of AlCoCrFeNiTix High-Entropy Alloy". Technische Universität Chemnitz, 2018. https://monarch.qucosa.de/id/qucosa%3A23475.
Pełny tekst źródłaLindner, Thomas, Martin Löbel, Thomas Mehner, Dagmar Dietrich i Thomas Lampke. "The Phase composition and microstructure of AlχCoCrFeNiTi alloys for the development of high-entropy alloy systems". Universitätsbibliothek Chemnitz, 2017. http://nbn-resolving.de/urn:nbn:de:bsz:ch1-qucosa-226527.
Pełny tekst źródłaHendrick, Michelle Renee. "The effects of combustion CVD-applied alumina coatings on the high temperature oxidation of a Ni-Cr alloy". Thesis, Georgia Institute of Technology, 1996. http://hdl.handle.net/1853/19635.
Pełny tekst źródłaRAJESHWAR, REDDY ELETI. "Deformation Mechanisms and Microstructure Evolution in HfNbTaTiZr High Entropy Alloy during Thermo-mechanical Processing at Elevated Temperatures". Doctoral thesis, Kyoto University, 2019. http://hdl.handle.net/2433/242505.
Pełny tekst źródła0048
新制・課程博士
博士(工学)
甲第21767号
工博第4584号
新制||工||1714(附属図書館)
京都大学大学院工学研究科材料工学専攻
(主査)教授 辻 伸泰, 教授 乾 晴行, 教授 安田 秀幸
学位規則第4条第1項該当
Doctor of Philosophy (Engineering)
Kyoto University
DFAM
Wang, Hao. "In-situ transmission electron microscopy investigation of deformation-induced microstructural evolution of a FeCoCrNiMn high-entropy alloy". Thesis, The University of Sydney, 2018. http://hdl.handle.net/2123/20068.
Pełny tekst źródłaAnguo, Wang. "The effect of grain size on the low-cycle fatigue behaviours of a CrMnFeCoNi high entropy alloy". Thesis, The University of Sydney, 2019. http://hdl.handle.net/2123/21129.
Pełny tekst źródłaAyyagari, Venkata A. "Surface Degradation Behavior of Bulk Metallic Glasses and High Entropy Alloys". Thesis, University of North Texas, 2017. https://digital.library.unt.edu/ark:/67531/metadc1062863/.
Pełny tekst źródłaKushnerov, O. I., i V. F. Bashev. "Structure and mechanical properties of Al-Co-Cr-Fe-Mn-Ni-Si-V high-entropy films obtained by splat-quenching". Thesis, Sumy State University, 2015. http://essuir.sumdu.edu.ua/handle/123456789/42650.
Pełny tekst źródłaKuprin, A. S., O. M. Morozov, V. A. Belous, S. A. Firstov, V. F. Gorban, V. D. Ovcharenko, E. N. Reshetnyak, G. N. Tolmachova, V. I. Zhurba i V. O. Progolaieva. "Effects of Deuterium Implantation Dose on Hardness and Deuterium Desorption Temperature Range from High Entropy TiVZrNbHf and TiVZrNbHfN Coatings". Thesis, Sumy State University, 2013. http://essuir.sumdu.edu.ua/handle/123456789/35363.
Pełny tekst źródłaHuang, Ping-Kang, i 黃炳剛. "On High-Entropy Alloy and Nitride Coatings Sputtered from AlCrNbSiTiV Target". Thesis, 2009. http://ndltd.ncl.edu.tw/handle/45557558479597094755.
Pełny tekst źródłaLin, Shao-Yi, i 林少顗. "Nanomechanical Properties and Deformation Behavior of Multi-component High-entropy Alloy and Nitride Coatings". Thesis, 2015. http://ndltd.ncl.edu.tw/handle/38066806767302667335.
Pełny tekst źródła國立中興大學
材料科學與工程學系所
104
Our study could divide into three sections. First, we studied about (AlCrTaTiZr)Nx multi-component coatings. They were developed as protective hard coatings for tribological application. The mechanical properties, creep behaviors, deformation mechanisms and interface adhesion of the (AlCrTaTiZr)Nx coatings with different N contents were characterized. With increasing the N2-to-total flow ratio, RN, during sputtering deposition, the (AlCrTaTiZr)Nx coatings transformed from an amorphous metallic phase to a nanocomposite and finally a crystalline nitride structure. With increasing RN, the mechanical proerties was enhanced. The plastic deformation of the amorphous metallic coating proceeded through the formation and extension of shear bands, whereas dislocation activities dominated the deformation behavior of the crystalline nitride coatings. The secondary part of our stury was about (AlCrTaTiZr)NCy and (AlCrTaTiZr)NSiz multi-component coatings.It were developed by co-sputtering of alloy target and graphite/silicon in an Ar/N2 mixed atmosphere with the application of different substrate biases. All the coatings deposited in different conditions exhibited a simple face-centered cubic structure. With increasing substrate bias and graphite/silicon target power, the mechanical proerties was also enhanced, attributed to the densification of the coatings, the refinement of grains, the introduction of covalent-like carbide bonds, the formation of nanocomposite structure and the existence of large lattice distortions. Because of the severe distortions in the multi-component coatings caused by the addition of differently-sized atoms, the deformation mechanism was dominated by the activity of low-angle dislocations and/or stacking faults. In the deformed regions under indents, stacking faults or partial dislocations were formed, while in the stress-released regions, near-perfect lattices recovered. Final, we designed multi-component alloys whose nanomechanical properties and characterized their deformation behaviors. We control the lattice distortion and cohesive energy of all the multi-component alloys under the same level and observed the different mechanical properties of multi-element. The lattice volume increased with element number increased. Due to the expansion of lattice volume, there was deference between theoretical and experimental values, including elastic modulus and hardness. The quinary alloy showed a magnificent elastic recovery, revealing that the deformation mechanism of multi-componet materials (including nitrides) was dominated by partial dislocations or stacking faults.
Alvi, Sajid. "Synthesis and Characterization of High Entropy Alloy and Coating". Licentiate thesis, 2019. http://urn.kb.se/resolve?urn=urn:nbn:se:ltu:diva-73882.
Pełny tekst źródła陳家裕. "Development of multicomponent high-entropy alloys for thermal spray coating". Thesis, 2002. http://ndltd.ncl.edu.tw/handle/47099338451611909570.
Pełny tekst źródłaHuang, Ping-Kang, i 黃炳剛. "Research of multi-component high -entropy alloys for thermalspray coating". Thesis, 2003. http://ndltd.ncl.edu.tw/handle/32057932770890578348.
Pełny tekst źródłaLuo, Jin-Tai, i 羅錦泰. "Development of oxidation-resistant coating for refractory high-entropy alloys". Thesis, 2018. http://ndltd.ncl.edu.tw/handle/jcef2n.
Pełny tekst źródłaLu, Che-Wei, i 呂哲維. "Electrochemical properties of CoCrFeMnNi high entropy alloy- a comparison with Fe5Mn3CoCr medium entropy alloy". Thesis, 2018. http://ndltd.ncl.edu.tw/handle/6z56du.
Pełny tekst źródła國立臺灣大學
材料科學與工程學研究所
106
In recent years, Fe5Mn3CoCr medium entropy alloy (MEA) has been reported as an alloy system which shows transformation-induced plasticity effect during deformation. The excellent strength and ductility combination of this alloy is even better than CoCrFeMnNi high entropy alloy (HEA), but the corrosion behavior is still unknown. In this study, the corrosion behavior of CoCrFeMnNi HEA and Fe5Mn3CoCr MEA were investigated. The environments chose for the cyclic polarization measurement were 3.5wt% NaCl solution with different pH values (pH=3, 6, 9, 12) and temperatures (10oC, 40oC, 70oC) and 0.1M H2SO4 solution. The results show that, compared with CoCrFeMnNi HEA, Fe5Mn3CoCr MEA the had smaller passivation region in every test environment, but the two substrate had almost the same corrosion current density value in 3.5wt% NaCl solution without any adjustment. In 0.1M H2SO4 solution, the corrosion current density of Fe5Mn3CoCr MEA is higher than CoCrFeMnNi HEA. The surface morphologies of CoCrFeMnNi HEA after polarization measurement in 3.5wt% NaCl solution exhibited a pitting appearance, which was resulted from the disintegration of inclusions on surface; Fe5Mn3CoCr MEA showed “lath-shaped” corrosion morphologies which were caused by the connection of pits. After cyclic polarization in 0.1M H2SO4 solution, CoCrFeMnNi HEA showed intergranular corrosion and galvanic corrosion morphologies; Fe5Mn3CoCr MEA showed “branch-like” corrosion morphologies which is attributed to the dissolution of ε martensite.
Kao, Yih-Farn, i 高逸帆. "High-entropy alloy mediated growth of graphene". Thesis, 2014. http://ndltd.ncl.edu.tw/handle/55042565088569128165.
Pełny tekst źródła國立清華大學
材料科學工程學系
102
Pyrolysis of acetylene over thin films made of CuxFeCoNiMn yields graphene and sheet dimension is found to control by x. Monolayer structure forms at x = 0.5 and sheet size reaches a value as large as 600 m2. Layer number increases as x rises and turbostratic graphite forms at x = 1.5. The x-controlled growth mechanism involves five consecutive steps and each is supported by experimental data.
Tsao, Te Kang, i 曹德綱. "Alloy Design Cast High Entropy Superalloys for High Temperature Applications". Thesis, 2016. http://ndltd.ncl.edu.tw/handle/7277mt.
Pełny tekst źródła國立清華大學
材料科學工程學系
105
In this study, high entropy alloys have been developed toward high temperature applications. According to the most widely used high temperature material superalloys, the microstructure of face-centered cubic (FCC) γ matrix with uniformly distributed L12 γ′ precipitates implies the more balanced high temperature strength and ductility. So, the thermal stability and strength of highly alloyed Ni3Al were studied initially. The strengthening effect on developing a γ′ composition toward higher entropy is significant, due to higher anti-phase boundary energy of the order phase. However, the order-disorder transition temperature would be decreased with the more random atomic distribution in γ′ lattice. The microstructure stability of the γ - γ′ alloys with medium to high mixing entropy were then studied. It was found that the high temperature alloys cannot be solely designed by entropy term, but should also enhance the ordering enthalpy of γ′ phase, to avoid lowering the thermal stability of γ′ phase. Through alloy designs, we have also found that present alloys are quite different from the conventional Ni-, Co- or Fe-based alloy design, but is within a range of stable (Ni, Co, Fe)-rich system. This composition space has rarely been studied through the development of superalloys. In addition, such highly-soluted (Ni-Co-Fe) matrix can exhibit an enlarged solubility of alloying contents, while remains good phase stability till high temperatures. Therefore, they have been named as high entropy superalloys (HESA). Since grain boundaries might be drawbacks to the thermal properties, HESAs have been successfully casted into the directionally-solidified (DS) structure by Bridgeman method. In terms of the high temperature mechanical properties, HESAs can exhibit comparable high temperature hardness, tensile strength and creep resistance to that of commercial superalloys due to the stable γ - γ′ microstructure, high volume fraction of γ′ precipitates, high anti-phase boundary energy for γ′ strengthening and low stacking fault energy to hinder dislocation climb. Good surface stability of HESA in high temperature oxidizing and corrosive environments were also demonstrated, which can be attributed to the rapid formation of continuous Chromia or Alumina for surface protection. Furthermore, with less alloying of refractory elements, HESAs exhibit the apparent advantages in lower density and cost of materials. Nevertheless, there are still concerns such as the directional coarsening of γ′ for HESAs cannot contribute to the creep resistance, and the strength of γ matrix is still lower than that of superalloys. As a result, further rooms for composition optimization of HESA exist. To summary, the novel high entropy superalloys are with unique composition, good thermal properties and improved cost-performance, thus can be promising as a new type of high temperature alloy.
Huang, Wen-Wei, i 黃文威. "Effect of Al0.5CoCrFeNi2 high entropy alloy particle on strength of AZ91 alloy". Thesis, 2019. http://ndltd.ncl.edu.tw/handle/48e979.
Pełny tekst źródła國立臺灣科技大學
機械工程系
107
In this study, 10 wt. % of Al0.5CoCrFeNi2 high entropy powder with the size of 10 μm and 90 μm were added to AZ91 alloy by powder metallurgy. According to the result of hardness and compression strength, particle size of 10 μm was the best candidate. Magnesium-based composites were then fabricated with four different addition amount (5 wt. %, 10 wt. %, 15 wt. %, 30 wt. %) to study the effect. The analysis was then carried out using SEM, XRD, MTS dynamic testing and Vickers hardness. The experimental results showed that the phase composition of magnesium-based composites with different addition amounts are composed of α-Mg, Mg17Al12, Al-Mn precipitates and Al0.5CoCrFeNi2. The microscopic results show that the high entropy powder did not change the phase structure within the composite during the powder metallurgy process. In the compression test results, addition of 5wt. % 10 μm will increase the maximum compressive strength and yield strength from 45.73MPa to 150.45Mpa and 42.5MPa to 149.9Mpa, respectively. The hardness test showed that the hardness of the composite with high entropy powder were enhanced. The hardness of adding 10 μm is enhanced from 55.4 HV to 139.3 HV, while the addition of 90 μm result the lower hardness of 108.6HV.
Chen, Yi-Hung, i 陳翊閎. "Structural Transition in High Entropy Alloy CoCrFeMnNi Subjected to High Pressure". Thesis, 2017. http://ndltd.ncl.edu.tw/handle/s3mbgv.
Pełny tekst źródła國立交通大學
材料科學與工程學系所
105
An equal-molar CoCrFeMnNi high-entropy alloy has the cubic crystal system of face-centered-cubic (FCC) at room temperature and atmospheric pressure. The recent research believed that the high-entropy has the property of low stacking fault energy, and excellent mechanic property because of the structure of nanocrystalline in low temperature. However, there was no phase-changing observed. This research used Angular-dispersive X-ray Diffraction (ADXRD) under high-pressure, pressurized the CoCrFeMnNi high-entropy alloy system to 20GPa. After analyzing diffraction data, there was phase transformation from FCC to Hexagonal Close Packing (HCP) when the pressure reached 7.1GPa. Both phases existed until the maximum pressure of 20GPa. When the pressure was unloaded to atmospheric pressure, there are remaining HCP-phase in the alloy, which shows the phase transformation is a non-reversible phenomenon. Besides observing phase transformation under high-pressure and the remaining HCP phase, this research will also calculate the lattice constant, ratio and full width at half maximum (FWHM) of both phases. Then, the result of the analysis will be compared with other theses, and to ensure that high-entropy alloy will not be affected by hydrostatic pressure in a high-pressure environment and non-isotropic compression. During the transformation of the material, there was corresponding texture and slip system. After comparison with other thesis, we discovered that when the phase of that alloy was transformed to HCP, the texture distribution is similar with Zine under pressurized. And confirmed the final phase of the alloy should be a uniform single phase. Finally, this research will investigate the phase transformation mechanism under high-pressure environment.
Yang, Chien-chang, i 楊健章. "Environments Corrosion Behavior of FeCoNiCrAl0.5 Bulky High Entropy Alloy". Thesis, 2009. http://ndltd.ncl.edu.tw/handle/16631098985979736826.
Pełny tekst źródła國立臺灣科技大學
機械工程系
97
The corrosion behavior of FeCoNiCrAl0.5 bulky high entropy alloy was studied. The homogenization treatment of the as-cast alloy specimen was processed. After water quenching serial heat-treatment processes were carried out. The corrosion properties, mechanical properties and microstructures of the specimens had been evaluated after the immersion tests with the NaCl, NaOH and H2SO4 solutions, respectively. The alloy has higher corrosion rate in 3.5 wt% NaCl aqueous solutions due to significant segregation of Cr-riched phase. Because of the active sensitivity zone of appreciable potential difference the alloy was preferentially attacked along the Cr-riched phase. The alloy exhibits excellent hardness after the immersion tests in NaOH and H2SO4 solution.
Lin, Szu Yen, i 林思延. "Electrochemical Corrosion Properties of the High Entropy Alloy ( Al5Cr12Fe35Mn28Ni20 )". Thesis, 2011. http://ndltd.ncl.edu.tw/handle/73102611505623444288.
Pełny tekst źródła中國文化大學
材料科學與奈米科技研究所
99
This research aims to explore the corrosion behavior and electrochemical properties of the high entropy alloy (HEA) AlCrFeMnNi ,to see whether increasing the amount of cold work (0% ,30% and 60%) would increase the pitting corrosion resistance ,and to achieve the critical pitting temperature (CPT) of the alloy in a specific aqueous environment containing chloride (Cl-) or fluoride (F-) through increasing the bath temperature (20-90℃). Experiments were conducted separately in sulfuric acid sodium chloride,ammonium chloride and sodium fluoride solutions and the result showed that under the room temperature the type 304 stainless steel showing a better pitting corrosion resistance than the HEA ;judging from the anodic polarization curves and SEM observations ,higher degree of cold work of the HEA has a better pitting corrosion resistance. Exposing AlCrFeMnNi alloy in acidic or in chloride environment showed that the component Al would easily react with the solution and be damaged by pitting corrosion leaving large amount of pits on the surface of the specimen . In dealing with such HEA it is possible to enhance the surface passivity for corrosion protection by means of increasing the degree of cold work .It is also observed that the CPT of this particular alloy increases with the increasing concentration of the fluoride solution and the highest CPT was achieved for the HEA with the highest degree of cold work. Keyword:high entropy alloy、critical pitting temperature
Peng, Bo-Sen, i 彭柏森. "Alloy design and mechanical properties study of titanium-rich light-weight high-entropy alloy". Thesis, 2019. http://ndltd.ncl.edu.tw/handle/x6z675.
Pełny tekst źródła國立中央大學
材料科學與工程研究所
107
High-entropy alloys (HEA) attract great attention in past few decades. Most HEA researches mainly concentrate on the heavier multi-principal elements with equiatomic or near-equiatomic alloys. In this study, we focus on the light-weight and non-equiatomic medium-entropy alloys (MEA) system with low density (below 5g/cm3). Series of non-equiatomic quaternary alloy system, Ti-Al-Cr-Nb、Ti-Al-Cr-V were firstly designed by using calculating parameter (∆S、∆H、δr), then further modified into quinary Ti-Al-Cr-Nb-V alloy system. All samples were prepared by vacuum arc melting and rapidly cooling process. The XRD results of Ti-Al-Cr-Nb 、Ti-Al-Cr-V and Ti-Al-Cr-Nb-V MEA reveal the single BCC structure. The hardness value of Ti60-Al-Cr-Nb reduced from 480Hv to 365Hv with decreasing the Al content which implies that the ratio of Ti/ Al elements plays an important role on the alloy hardness. The optimum mechanical performance occurs at Ti60-Al-Cr-Nb-V MEA with tensile yield strength of 1009 MPa, fracture strength of 1223 MPa, and plastic strain of 27.1%. In summary. the Ti60-Al-Cr-Nb-V MEA not only possesses higher mechanical properties than the commercial Ti6Al4V alloy, but also has similar density, wear resistance, and oxidation behavior to commercial Ti alloys. Therefore, it is believed that the Ti60-Al-Cr-Nb-V MEA can be a promising light-weight structure material for the applications of transportation vehicles and sport equipment.
Chen, Hong-Siang, i 陳泓翔. "Microstructure and characterisation of high entropy alloy (TiVCrZrNbMoHfTaWAlSi) Nitride film". Thesis, 2017. http://ndltd.ncl.edu.tw/handle/qzq779.
Pełny tekst źródła國立勤益科技大學
機械工程系
105
In this study, a high-entropy alloy nitride film was prepared by a DC sputtering machine. A nitride film was deposited on a silicon wafer and quartz glass (SiO2) without applying a substrate bias. The working pressure was 4x10-3 Torr and the sputtering was fixed at 300W The temperature and temperature of the substrate were fixed at 300 ° C, and the film composition and microstructure were controlled by adjusting the nitrogen and argon flow rate (RN) in the vacuum. The film thickness was 1000 nm ± 50 nm, , Scanning electron microscopy, visible spectrophotometer, Hall effect analyzer, chemical analysis electron spectrometer, atomic force microscope, nano indentation tester and wear tester (Rub Tester) and other instruments were analyzed and compared to explore the different nitrogen flow On the microstructure, chemical composition, electrical properties, optical and mechanical properties of the film. Component analysis, the high entropy alloy due to the composition of a variety of elements, the majority of its composition is uneven distribution, which is due to high entropy effect caused. It is known that the microstructure of the film is amorphous phase structure at the beginning of the observation. When the flow rate of nitrogen and argon is more than 15%, the microstructure is transformed into the crystalline phase. When the RN is 15%, it belongs to the FCC structure, and its preferred direction is (200) , When the RN increases to 20%, the crystallinity of the film increases, because the film nitrogen content increases, contributing to the formation of nitride phase, in addition to the preferred direction into (111), when RN to 49%, (200) peak appears For the final preferred direction, which is due to sputtering atoms kinetic energy is too high, may lead to recrystallization effect, but too high kinetic energy will damage the film structure, to produce re-nucleation effect, reduce grain size. And RN = 49% when the surface aggregates have been reduced much, and the grain size also decreased, mainly the atomic kinetic energy decreased, the film compressive stress decreased. In the mechanical properties, it was found that when the RN = 49%, the hardness of the film was the highest, and the hardness was 34 GPa. The Young's modulus was 276 GPa. The film will rise with the rise of the resistivity of the RN, which may be due to N increase → the number of electrons → lead to increased resistivity caused. The optimum friction coefficient of this nitride film was found to be about 0.5 ± 0.08, and the friction coefficient was related to the ratio of nitrogen to argon, grain and hardness. Finally, in the cutting, compared with the general naked knife, this high entropy nitride film also has a better hardness and cutting properties.
Fang, Shuang, i 方雙. "Microstructures and Mechanical Properties of CoCrFeMnNiVx High Entropy Alloy Films". Thesis, 2019. http://ndltd.ncl.edu.tw/handle/hbe4ev.
Pełny tekst źródła國立臺灣大學
材料科學與工程學研究所
107
In the present work, CoCrFeMnNiVx (x = 0, 0.07, 0.3, 0.7, 1.1) high entropy alloy films were fabricated by magnetron co-sputtering. For low contents of V, typical face-centered cubic (fcc) peaks were identified in X-ray diffraction patterns. With the increasing V content, the diffraction peaks became broadening and the formation of amorphous phase was promoted. TEM observations showed abundant nanotwins in films with low V contents and the transition from fcc to amorphous structure with the increasing V content. The 3D APT reconstruction results revealed no precipitate in the as-deposited films (x = 0, 0.07). Mechanical properties of the films were studied using nanoindentation and micro-pillar compression tests. The films exhibited high hardness ranging from 6.8 to 8.7 GPa. The serrated flow associated with shear banding showed in the stress-strain curves for films with x ≥ 0.3. When x = 0.07, excellent yield strength of ~3.8 GPa and ultimate compressive strength of ~4.9 GPa were achieved with little sacrifice in ductility. The presence of nanotwins contributed to the strain hardening effect.
Tsai, Chih-Fang, i 蔡致芳. "High-Entropy Alloy Nanoparticles as Electrocatalysts for Direct Methanol Fuel Cells". Thesis, 2007. http://ndltd.ncl.edu.tw/handle/50943003627171622233.
Pełny tekst źródła國立交通大學
材料科學與工程系所
95
In this study, fabrication and electrochemical characterization of high-entropy electrocatalyst on noncatalyzed gas diffusion electrode by RF sputter deposition was reported. XRD analysis of the as-deposited film exhibited a crystalline FCC phase while EDS confirmed its composition as Pt52Fe10Co9Ni9Cu12Ag8. SEM images revealed nanoparticles nodules growing on the carbon particles. Cyclic voltammetry (CV) was used to analyze its performance as anode electrocatalyst for direct methanol fuel cell. The area under CV curve was proportional to the amount of electrocatalyst deposited. However, in specific activity sample with 5 nm electrocatalyst demonstrated the highest values, 400~600 mA/cm2•mg. Our work presents invaluable information on electrochemical performance of high-entropy electrocatalyst. High-entropy nanoparticles of PtxFe(100-x)/5Co(100-x)/5Ni(100-x)/5Cu(100-x)/5Ag(100-x)/5 (x = 22, 29, 52, 56) were then prepared by sputter deposition on pretreated carbon cloth. XRD patterns indicated crystalline FCC phases and SEM images revealed nanoparticulate nodules grown on surface of carbon particles with their average sizes increasing with deposition time. Cyclic voltammetry demonstrated enhancements of catalytic performance with increasing Pt amount. However, in specific activity Pt52Fe11Co10Ni11Cu10Ag8 exhibited the highest capability, reaching values as high as 504 and 462 mA/cm2•mg. This work provides invaluable information in unique electrocatalyst design using high-entropy concept. Comparison of the properties of six-component alloys and binary alloys Pt-M (M= Fe, Co, Ni, Cu, Ag) were studied in last part. All the phases of binary alloys were fcc as identified by XRD. In addition, the morphologies of PtFe, PtCo, and PtCu were similar in their nodules structure to that of Pt52Fe10Co9Ni9Cu12Ag8. In contrast, PtAg formed a large particle on carbon black. The PtCu showed the highest catalytic activity, and PtAg was the poorest because of its large of particles size and weak strength of M-O bonding. The six-component alloy exhibited characteristics between each binary alloys, imply the mixing effects of the multi-components.
Chen, Huang-Jen, i 陳皇仁. "A study of phase transformations in an Al0.5CoCrFeNi2 high entropy alloy". Thesis, 2005. http://ndltd.ncl.edu.tw/handle/13260718801691617600.
Pełny tekst źródła國立臺灣科技大學
材料科技研究所
93
We have studied the microstructures of the constituent phases of a Al0.5CoCrFeNi2 multi-component alloy in two conditions which one was in the as-cast condition and the other wais in hot forged, cold rolled, annealed at 1050℃, then heat treatment at lower temperatures. For the alloy in the as-cast condition, the dendrites appeared in the OM observation, and only FCC peaks were observed from the XRD analysis; however, L12 phase was the major phase confirmed by the TEM study. The L12 phase was the derivative phase from the FCC parent phase. The mechanism for the phase transformation was FCC → L12 during the solidification process. For the alloy in the as-quenched condition, the major phase of the alloy is FCC. The minor B2 phase precipitated from the FCC matrix and had the K-S orientation relationship with the FCC matrix: [10 ]FCC // [11 ]B2,(111) FCC // (101) B2. For the alloy in the annealing conditions at 1000, 900, and 850℃, the microstructure of the alloy is similar to that in the as-quenched condition. However, for the annealing temperature below 800℃ we found the matrix phase had changed from FCC to L12 phase. Therefore the upper limit temperature for the existence of the B2 phase is between 800 and 850℃. For the annealing temperature at 700 and 600℃, we found a new FCC phase with high Al content precipitated from the L12 matrix. The lattice constant of the new FCC phase is a = 0.6785 nm which is higher than that of pure Al and different from those of Al2O3. For the annealing temperatures at 600 and 500℃, we found another new coherent FCC phase precipitated from the L12 matrix. The lattice constant of the new FCC phase is three times larger than that of L12 phase. The mechanism of the phase transformation of the new coherent FCC phase is FCC→L12→new coherent FCC phase. Both new FCC phases have never been observed in the multi-component alloy systems.