Multi-component coatings and high entropy alloys have in recent years attracted great interest for research, since they have shown to exhibit properties greater than the com- ponents of their parts. Today’s climate challenges requires transitioning from fossil fuels to renewable energy sources which demands use of new technology and new innovations. The hydrogen fuel cell is a technology which produces no carbon emissions, and the drive for innovation has led researchers to apply multi-component (high entropy alloys) coatings to invent the next generation hydrogen fuel cells and help the transition to renewable energy sources. This thesis has investigated the process-structure-property relationships of four deposi- tion growth parameters: target current (Itarget), argon pressure (PAr). substrate bias (Vsubstrate) and deposition time (tdeposition) on TiNbZrTa-coatings, grown by magnetron sputtering using an industrial deposition system. The range of the parameters have been: Itarget from 2.5 to 6 A, PAr from 1 to 17 mTorr, Vsubstrate from 30 to 200 V and tdeposition from 3.6 to 12 minutes (depending on Itarget). Coatings have been grown on Si (001) and stainless steel 304 and 316L substrates. The coating microstructure was analyzed by X-ray diffraction and electron microscopy. The results have yielded that all coatings are equimolar and that the coatings exhibit three different morphologies, two different topologies and two different corresponding structures. The different morphologies are wave, coarse columnar and fine columnar morphology. The two topologies are nodular and dune surface topology. The two different structures are a solid solution BCC (110) phase and an amorphous or nanocrystalline phase. The results indicate that parameters affecting the temperature of the substrate (Tsubstrate) is the prime decider for the final morphology of the coatings. High Itarget and Vsubstrate, low PAr and long tdeposition all increases Tsubstrate and results in a coating which exhibits a fine columnar morphology, dune topology and a solid solution BCC phase. These types of coatings have also proven to have improved corrosion resistance compared to the other type of coatings seen in this thesis. The other kind of coating is grown with low Itarget and Vsubstrate, high PAr and short tdeposition, which causes minimal increase of Tsubstrate. These growth parameters result in a coating with coarse columnar morphology, nodular topology and amorphous or nanocrystalline phase, with less corrosion resistance. / FunMat II

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No description available.

High entropy alloys (HEAs), also referred to as complex concentrated alloys (CCAs), are a relatively new class of alloys that have gained significant attention since 2010 due to their unique balance of properties that include high strength, ductility and excellent corrosion resistance. HEAs are usually based on five or more elements alloyed in near equimolar concentrations, and exhibit simple microstructures by the formation of solid solution phases instead of complex compounds. HEAs have great potential in the design of new materials; for instance, for lightweight structural applications and elevated temperature applications. The relation between grain size and yield strength has been a topic of significant interest not only to researchers but also for industrial applications. Though some research papers have been published in this area, consensus among them is lacking, as the studies yielded different results. Al atom being a large atom causes significant lattice distortion. This work attempts to study the Hall-Petch relationship for Al0.3CoFeNi and Al0.3CoCrFeNi and to compare the data of friction stress σ0 and Hall-Petch coefficient K with published data. The base alloys for both these alloys are CoFeNi and CoCrFeNi respectively. It was observed by atom probe tomography (APT) that clustering of Al-Ni atoms in these two base CCAs was responsible for imparting such high values of K. Additionally the high value of K in the CoCrFeNi HEA can also be attributed to the presence of Co-Cr clusters.

The current work investigates how the interactions among constituent elements in high entropy alloys or complex concentrated alloys (HEA/CCAs) can lead to lattice instability and local chemical ordering which in turn affects the microstructure and properties of these alloys. Using binary enthalpies of mixing, the degree of ordering in concentrated multi-component solid solutions was successfully tailored by introducing Cr, Al and Ti in a CoFeNi HEA/CCA. CoFeNi was selected as the base alloy to achieve a close to random solid solution as indicated by the near-zero binary enthalpies in CoFeNi alloy system. The room temperature tensile properties of these alloys with varied degree of ordering follow a consistent trend where yield stress increased with degree of ordering. This novel approach provides a new alloy design strategy to obtain controlled ordering tendencies and consequently targeted mechanical properties. Further studies on specific alloys have been conducted to utilize this ordering tendency in attaining precipitation strengthening. For this purpose, Al, Ti and Ni were selected to promote ordering and Co, Fe, and Cr were chosen to strengthen the solid solution matrix. In Al0.25CoFeNi HEA/CCA, the ordering tendency between Al and Ni results in a competition between two long-range ordered phases, L12 and B2. While homogenous L12 precipitation takes place at an annealing temperature of 500oC, heterogeneous B2 precipitation occurs at 700oC. At 600oC, this competition between L12 and B2 phases results in a novel nano-lamellar microstructure. The alternating lamellae are mainly FCC and BCC based whose morphology is similar to pearlite in steels. However, the FCC lamella is made up of FCC and L12 phases and the BCC lamella is made up of BCC and B2 phases. A different thermomechanical processing route can be used to obtain the same phase composition but distributed in a nano-grained fashion. This nano-grained microstructure exhibits the best strength-ductility combination in this alloy. Thermomechanical processing can also be used to engineer the transformation pathway of L12 from homogenous to discontinuous precipitation. The homogenous and discontinuous L12 precipitation has been investigated in two different alloys namely, Al0.2Ti0.3Co1.5CrFeNi1.5 and Al0.3Ti0.2Co0.7CrFeNi1.7. While discontinuous precipitation (DP) is generally considered deleterious to mechanical properties, the results from this study suggests that microstructures with DP perform better compared to homogenous L12 up to 500oC. However, beyond 500oC, microstructures with homogenous L12 appears to perform better than discontinuously precipitated FCC+L12 microstructure.

Multicomponent high-entropy and amorphous alloys represent relatively new classes of structural materials with complex atomic configurations and exceptional mechanical properties. However, there are several knowledge gaps in the relationships between their atomic structure and mechanical properties. Understanding these critical relationships will enable novel alloy design and tailoring of their mechanical properties for desired engineering applications. In this dissertation, first-principles calculations and molecular dynamics simulations are applied to investigate the local atomic configurations and ordering in high-entropy and amorphous alloys. Our findings suggest that fluctuations in local atomic configurations for high- entropy alloys result in significant changes in stacking fault energy, twin energy, dislocation behavior, dislocation-twin interactions, and critical shear stress. For amorphous alloys or metallic glasses, the short-range order (SRO) and medium-range order (MRO) were found to play decisive roles in determination of their mechanical properties. Structural relaxation was found to lead to shear localization, which was attributed to free volume change and evolution of SRO and MRO to more brittle nature. In contrast, rejuvenated metallic glasses had relatively large and uniform free volume distribution giving rise to homogeneous flow and increased plasticity.

Um novo conceito para o desenvolvimento de ligas metálicas vem sendo estudado pela comunidade científica nos últimos anos, trata-se de ligas com elementos multiprincipais, também conhecidas como ligas de alta entropia (HEAs). HEAs constituídas de metais refratários e alumínio se destacam como possíveis ligas para utilização na indústria aeroespacial por apresentaram alta resistência específica. Dessa forma, torna-se necessário uma investigação das relações de fases envolvendo metais refratários e o alumínio. Para este trabalho, foi escolhido o sistema Al-Nb-V, uma vez que se encontrou apenas uma seção isotérmica experimental completa do sistema e nenhuma avaliação termodinâmica na literatura. Para o desenvolvimento do trabalho, foram produzidas ligas por fusão a arco. As amostras foram tratadas a 1200 °C por 10 dias para a determinação da seção isotérmica do sistema nessa temperatura. A caracterização microestrutural foi realizada por meio de difração de raios X (DRX), microscopia eletrônica de varredura (MEV) e microanálise eletrônica (EDS). Em relação à seção isotérmica disponível na literatura, foram observadas algumas diferenças. A seção da literatura, por exemplo, propõe a estabilidade do composto ternário NbVAl2, o qual não foi encontrado neste trabalho. Os resultados permitiram a determinação de boa parte da seção isotérmica a 1200 °C do sistema Al-Nb-V. Em paralelo, foi realizada uma revisão das avaliações termodinâmicas dos binários disponíveis na literatura. Os dados da literatura e os resultados experimentais obtidos foram utilizados para construir uma base de dados termodinâmicos pelo método Calphad. A modelagem termodinâmica apresenta boa consistência com os resultados experimentais obtidos. / A new concept for the development of metallic alloys has been studied by the scientific community in recent years, which deals with multi-principal element alloys, also known as High Entropy Alloys (HEAs). HEAs with refractory metals and aluminium as constituents are possible alloys for use in the aerospace industry mainly due to their high specific resistance. In this way, the investigation of phase equilibria involving refractory metals and aluminium is required. For this work, the Al-Nb-V system was chosen, since only one complete experimental isothermal section of this system and no thermodynamic assessments were found in the literature. For the development of this work, 23 alloys were produced by arc melting. The alloys were treated at 1200 °C for 10 days to determine the isothermal section of the system at this temperature. The microstructural characterization was performed via X-ray diffractometry (XRD) scanning electron microscopy (SEM) and energy dispersive spectroscopy (EDS). Some discrepancies were observed between the isothermal section available in the literature and the results of the present work. The isothermal section found in the literature, for example, proposes the stability of the ternary compound NbVAl2, which was not found in this work. Based on the present work, a new isothermal section at 1200 °C is proposed for the Al-Nb-V system. Also, a review of the thermodynamic descriptions of the binary systems available in the literature was performed. The literature data and the experimental results were used to build a thermodynamic database using the Calphad method. This preliminary thermodynamic modelling shows good consistency with the experimental results.

abstract: The structural and electronic properties of compositionally complex semiconductors have long been of both theoretical interest and engineering importance. As a new class of materials with an intrinsic compositional complexity, medium entropy alloys (MEAs) are immensely studied mainly for their excellent mechanical properties. The electronic properties of MEAs, however, are less well investigated. In this thesis, various properties such as electronic, spin, and thermal properties of two three-dimensional (3D) and two two-dimensional (2D) compositionally complex semiconductors are demonstrated to have promising various applications in photovoltaic, thermoelectric, and spin quantum bits (qubits).3D semiconducting Si-Ge-Sn and C3BN alloys is firstly introduced. Density functional theory (DFT) calculations and Monte Carlo simulations show that the Si1/3Ge1/3Sn1/3 MEA exhibits a large local distortion effect yet no chemical short-range order. Single vacancies in this MEA can be stabilized by bond reformations while the alloy retains semiconducting. DFT and molecular dynamics calculations predict that increasing the compositional disorder in SiyGeySnx MEAs enhances their electrical conductivity while weakens the thermal conductivity at room temperature, making the SiyGeySnx MEAs promising functional materials for thermoelectric devices. Furthermore, the nitrogen-vacancy (NV) center analog in C3BN (NV-C3BN) is studied to explore its applications in quantum computers. This analog possesses similar properties to the NV center in diamond such as a highly localized spin density and strong hyperfine interactions, making C3BN suitable for hosting spin qubits. The analog also displays two zero-phonon-line energies corresponding to wavelengths close to the ideal telecommunication band width, useful for quantum communications. 2D semiconducting transition metal chalcogenides (TMCs) and PtPN are also investigated. The quaternary compositionally complex TMCs show tunable properties such as in-plane lattice constants, band gaps, and band alignment, using a high through-put workflow from DFT calculations in conjunction with the virtual crystal approximation. A novel 2D semiconductor PtPN of direct bandgap is also predicted, based on pentagonal tessellation. The work in the thesis offers guidance to the experimental realization of these novel semiconductors, which serve as valuable prototypes of other compositionally complex systems from other elements. / Dissertation/Thesis / Doctoral Dissertation Materials Science and Engineering 2020

This Master’s thesis is focused on theoretical study of the high entropy alloy CoCrNi using ab initio calculations. The focus was on the effect of short range order on the relative stability of FCC and HCP structures and the value of stacking fault energy.The results show increase of stability in both types of structures wtih decreasing number of Cr-Cr nearest neighbours. The effect of the number of Cr-Cr nearest neighbours on the stacking fault energy previously shown in literature was not observed. However the strong dependency was found on the change of short range order caused by the shift of (1 1 1) planes after the transformation from the FCC to HCP structure. The effect of interstitial atoms C a N was also studied. Both these interstitials stabilise FCC structure and thus cause the increase of stacking fault energy. Both interstitials prefer octahedral positions with higher amount of Cr in their nearest neighbour shell.

The high entropy alloys (HEAs) have been developed based on the concept of entropic stabilization associated with a large number of constituent elements. The high configurational entropy in HEAs is expected to cause promising characteristic properties, i.e. high microstructural stability and high mechanical properties. In this study, the equiatomic fcc-structured FeNiCoCrMn and the bcc-structured TiNbHfTaZr single phase high entropy alloys (HEAs) were investigated regarding the effect of multiple atom species on microstructure, intrinsic lattice strain and mechanical properties. In a comparison with the HEAs, the sub-alloys having less chemical complexity were studied. The selected sub-alloys of the FeNiCoCrMn HEA were FeNiCoCr, FeNiCo, FeNi alloys and pure Ni, while equiatomic TiNbHfTa, TiNbHf, TiNb alloys and pure Nb were studied to compare with the TiNbHfTaZr HEA. The samples in this study were prepared by arc-melting, cold-crucible casting and thermomechanical treatment. The thermal phase stability of the FeNiCoCrMn HEA, TiNbHfTaZr HEA and their sub-alloys were observed and no second phase was formed between 300 - 1500 K. In high entropy alloys, the random arrangement of multiple atom species is assumed to cause large atomic displacements at lattice sites, which give rise to a severe lattice distortion. The evidences of lattice distortion in HEAs have been limitedly reported due to a difficulty of experimental investigation. In this work, the pair distribution function (PDF) method was used to assess local strain with analysis of diffuse intensities on total synchrotron X-ray scattering data. The current study found that the level of local lattice strain associated with atomic displacement was a function of atomic size misfit. The local lattice strain of the FeNiCoCrMn HEA was small and comparable to that of the sub-alloys which obtain similar values of the atomic size misfit. In contrast to the FeNiCoCrMn system, the magnitude of the local lattice strain increased with the value of atomic size misfit from the unary Nb sample to the quinary TiNbHfTaZr HEA. The lattice distortion was evident in the TiNbHfTaZr HEA due to large local lattice strain, but the local lattice strain of the FeNiCoCrMn HEA was not anomalously large. The level of lattice strain determines the solid solution hardening as a consequence of the elastic interaction between dislocations and atoms. The comparable level of the lattice strain in the FeNiCoCrMn HEA, its sub-alloys and Ni sample led to narrow range of hardness (64 – 132 HV) and tensile yield strength (60 – 192 MPa). For the bcc-structured samples, the hardness and the yield strength significantly varied depending on the level of local lattice strain, between 80 – 327 HV of hardness and 207 – 985 MPa of tensile yield strength. It is clear from the result that the atomic size misfit influences the level of the local lattice strain and the solid solution hardening. Cold rotary swaging was used to study the work hardening in the HEAs because it can delay fracture by large hydrostatic stresses. The large plastic deformability was observed in the FeNiCoCrMn and TiNbHfTaZr HEAs. The TiNbHfTaZr HEA was cold-swaged by 90% reduction of the cross-sectional area without intermediate annealing. The FeNiCoCrMn HEA was swaged until 85% reduction of the cross-sectional area; however, it was observed that it could be further deformed. The dislocation densities of the HEAs and its sub-alloys after the cold deformation were calculated as in the range between 1014 - 1015 m-2, in a good agreement with reported values of conventional metals after severe plastic deformation. This finding suggested that the level of dislocation density storage was correlated with the number of the constituent elements, the level of lattice distortion associated with atomic size misfit and the intrinsic properties (i.e. the stacking fault energy and the melting point). Whereas the intrinsic lattice strains of the FeNiCoCrMn HEA and its sub-alloys were comparable, the levels of dislocation storage were different possibly due to a difference of stacking fault energy. For the bcc-structured samples, the dislocation densities of the TiNbHfTaZr HEA, TiNbHfTa and TiNbHf alloys were large due to the large atomic size misfits. The high dislocation density leads to strong interactions between dislocations, which results in high resistance to dislocation motions. The high mechanical properties (hardness and yield strength) in the as-deformed FeNiCoCrMn and TiNbHfTaZr HEA were presented with the evidence of high dislocation densities. Moreover, the hardness and yield strength of the FeNiCoCrMn HEA significantly increased by the deformation, while those of the TiNbHfTaZr HEA after the deformation were slightly changed from the undeformed HEA. The large work hardenability of the FeNiCoCrMn HEA is possibly caused by small solid solution hardening and ease of twin formation. The research results suggest a further step towards designing an alloy composition for a development of microstructure and mechanical properties of high entropy alloys. It is evidently clear from the findings that the large number of constituent elements (in a term of high configurational entropy) is not only a factor in the determination of lattice distortion, microstructure and mechanical properties, but the type and the combination of constituent elements including the atomic interactions (i.e. atomic size misfit) have also an effect.:Abstract v Zusammenfassung ix Contents xiii 1. Motivation and objectives 1 2. Fundamentals 5 2.1 Concept of high entropy alloys 5 2.1.1 Phase formation and thermodynamic 5 2.1.2 Four core effects 10 2.2 Alloy classification of high entropy alloys 13 2.3 Mechanical properties of high entropy alloys 14 3. Experiments 19 3.1 Alloy preparation 19 3.1.1 Alloy selection 19 3.1.2 Melting and casting 21 3.1.3 Thermomechanical treatment 23 3.2 Sample characterization 27 3.2.1 Chemical analyses 27 3.2.2 Differential scanning calorimetry (DSC) 27 3.2.3 Scanning electron microscopy and microstructural analyses 28 3.2.4 X-ray diffraction (XRD) 29 3.2.5 High energy synchrotron X-ray diffraction 29 3.2.6 Mechanical Properties 33 4. Thermal phase stability of single phase high entropy alloys 35 5. An assessment of lattice strain in single phase high entropy alloys 49 5.1 Analysis of micro lattice strain on fcc- and bcc-structured high entropy alloys 50 5.2 Analysis of local lattice strain on fcc- and bcc-structured high entropy alloys 56 6. Solid solution hardening in single phase high entropy alloys 65 6.1 Hardness of fcc- and bcc-structured high entropy alloys 65 6.2 Tensile strength of fcc- and bcc-structured high entropy alloys 70 6.3 Correlation between atomic size misfit and solid solution hardening in Ti-Nb-Hf-Ta-Zr system 82 7. Work hardening in single phase high entropy alloys 91 7.1 Work hardenability of fcc- and bcc-structured high entropy alloys 91 7.2 Dislocation density of fcc- and bcc-structured high entropy alloys after cold swaging 93 8. Summary and outlook 109 8.1 Summary 109 8.2 Outlook 112 References 113 Acknowledgements 131 Erklärung 133 / Die Hochentropielegierungen (HELen) wurden auf der Grundlage des Konzepts der entropischen Stabilisierung entwickelt, was eine große Anzahl von Legierungselementen beinhaltet. Es wird erwartet, dass die hohe Konfigurationsentropie in HELen vielversprechende charakteristische Eigenschaften hervorruft, d.h. hohe mikrostrukturelle Stabilität und hohe mechanische Eigenschaften. In dieser Studie wurden die äquiatomare kfz-strukturierte FeNiCoCrMn und die krz-strukturierte TiNbHfTaZr Einphasen-Hochentropielegierung hinsichtlich der Wirkung mehrerer Atomarten auf das Gefüge, die intrinsische Gitterdehnung und die mechanischen Eigenschaften untersucht. Im Vergleich zu den HELen wurden die Sublegierungen mit geringerer chemischer Komplexität untersucht. Die ausgewählten Sublegierungen der FeNiCoCrMn HEL waren FeNiCoCr, FeNiCo, FeNi-Legierungen und reines Ni, während äquiatomare TiNbHfTa, TiNbHf, TiNbHf, TiNb-Legierungen und reines Nb im Vergleich zur TiNbHfTaZr HEL untersucht wurden. Die Proben in dieser Studie wurden durch Lichtbogenschmelzen, Kalttiegelguss und thermomechanische Behandlung hergestellt. Die thermische Phasenstabilität der FeNiCoCrMn HEL, der TiNbHfTaZr HEL und ihrer Sublegierungen wurde untersucht und es wurde keine zweite Phase zwischen 300 - 1500 K gebildet. Bei Hochentropielegierungen wird angenommen, dass die zufällige Anordnung mehrerer Atomarten zu großen Atomverschiebungen an den Gitterplätzen führt, die eine starke Gitterverzerrung hervorrufen. Aufgrund der Schwierigkeit der experimentellen Untersuchung wurden Beweise für Gitterverzerrungen bei HELen nur begrenzt berichtet. In dieser Studie wurde die Methode der Paarverteilungsfunktion (PDF) verwendet, um die lokale Dehnung mit Analyse der diffusen Intensitäten der gesamten Synchrotron-Röntgenstreuungsdaten zu beurteilen. Die aktuelle Studie ergab, dass die Höhe der lokalen Gitterdehnung, die mit der atomaren Verschiebung einhergeht, eine Funktion der Differenz der Atomgröße ist. Die lokale Gitterdehnung der FeNiCoCrMn HEL war klein und vergleichbar mit der der Sublegierungen, für die ähnliche Werte für die Atomgrößen-Unterschiede ermittelt wurden. Im Gegensatz zum FeNiCoCrMn-System stieg die Größe der lokalen Gitterdehnung mit dem Wert der Atomgrößendifferenz von der unären Nb-Probe bis zur quinären TiNbHfTaZr HEL. Die Gitterverzerrung war in der TiNbHfTaZr HEL aufgrund der großen lokalen Gitterdehnung offensichtlich, wohingegen die lokale Gitterdehnung der FeNiCoCrMn HEL nicht ungewöhnlich groß war. Die Höhe der Gitterdehnung bestimmt die Mischkristallverfestigung als Folge der elastischen Wechselwirkung zwischen Versetzungen und Atomen. Der vergleichbare Wert der Gitterdehnung in der FeNiCoCrMn HEL, seinen Sublegierungen und den Ni-Proben führte zu einem engen Härte- (64 - 132 HV) und Streckgrenzenbereich (60 - 192 MPa). Für die krz-strukturierten Proben variierten die Härte und die Streckgrenze dagegen je nach Höhe der lokalen Gitterdehnung signifikant, d.h zwischen 80 - 327 HV hinsichtlich der Härte und zwischen 207 - 985 MPa hinsichtlich der Streckgrenze. Aus dem Ergebnis ist ersichtlich, dass die Differenz der Atomgröße einen Einfluss auf die Höhe der lokalen Gitterdehnung und die Mischkristallverfestigung hat. Das Kalthämmen wurde für die Untersuchung der Kaltverfestigung in den HELen genutzt, da es den Bruch durch die großen hydrostatischen Spannungen verzögern kann. Die große plastische Verformbarkeit wurde bei den FeNiCoCrMn und TiNbHfTaZr HELen beobachtet. Die TiNbHfTaZr HEL wurde ohne Zwischenglühen um 90% der Querschnittsfläche kaltgehämmert. Die FeNiCoCrMn HEL wurde bis zu einer Verkleinerung der Querschnittsfläche von 85% gehämmert, wobei jedoch eine weitere Verformung möglich gewesen wäre. Die Versetzungsdichten der HELen und ihrer Sublegierungen wurden nach dem Verformung in einem Bereich zwischen 1014 - 1015 m-2 berechnet, was in guter Übereinstimmung mit den berichteten Werten konventioneller Metalle nach starker plastischer Verformung ist. Dieses Ergebnis deutete darauf hin, dass die Höhe der gespeicherten Versetzungsdichte mit der Anzahl der beinhaltenden Elemente, dem Grad der Gitterverzerrung im Zusammenhang mit der Differenz der Atomgröße und den intrinsischen Eigenschaften (d.h. der Stapelfehlerenergie und dem Schmelzpunkt) korreliert. Obwohl die intrinsischen Gitterdehnungen der FeNiCoCrMn HEL und seiner Sublegierungen vergleichbar waren, waren die Werte der gespeicherten Versetzungen unterschiedlich, was möglicherweise an einer Differenz der Stapelfehlerenergie lag. Für die krz-strukturierten Proben waren die Versetzungsdichten der TiNbHfTaZr HEL, der TiNbHfTa- und der TiNbHf-Legierungen aufgrund der großen Atomgrößenunterschiede hoch. Die hohe Versetzungsdichte bewirkt starke Wechselwirkungen zwischen den Versetzungen, was zu einem hohen Widerstand gegen Versetzungsbewegungen führt. Die hohen mechanischen Eigenschaften (Härte und Streckgrenze) in den verformten FeNiCoCrMn und TiNbHfTaZr HELen wurden mit dem Nachweis hoher Versetzungsdichten belegt. Darüber hinaus wurden die Härte und die Streckgrenze des FeNiCoCrMn HEL durch das Kalthämmern deutlich erhöht, während die der TiNbHfTaZr HEL nach dem Hämmerprozess nur leicht gegenüber der unverformten HEL verändert wurden. Die große Kaltverfestigung der FeNiCoCrMn HEL ist möglicherweise auf eine geringe Mischkristallhärtung und eine geringfügige Zwillingsbildung zurückzuführen. Die Forschungsergebnisse empfehlen für die Entwicklung des Gefüges und der mechanischen Eigenschaften von Hochentropielegierungen weitere Schritte hinsichtlich eines zielführenden Legierungsdesigns durchzuführenhin. Aus den Ergebnissen geht eindeutig hervor, dass die große Anzahl an Legierungselementen ( hinsichtlich einer hochkonfigurativen Entropie) nicht die einzige Einflussgrößebei der Bestimmung von Gitterverzerrungen, dem Gefüge und der mechanischen Eigenschaften darstellt, sondern auch die Art und die Kombination der Legierungselementen einschließlich der atomaren Wechselwirkungen (d.h. Atomgrößenunterschiede) einen Effekt haben.:Abstract v Zusammenfassung ix Contents xiii 1. Motivation and objectives 1 2. Fundamentals 5 2.1 Concept of high entropy alloys 5 2.1.1 Phase formation and thermodynamic 5 2.1.2 Four core effects 10 2.2 Alloy classification of high entropy alloys 13 2.3 Mechanical properties of high entropy alloys 14 3. Experiments 19 3.1 Alloy preparation 19 3.1.1 Alloy selection 19 3.1.2 Melting and casting 21 3.1.3 Thermomechanical treatment 23 3.2 Sample characterization 27 3.2.1 Chemical analyses 27 3.2.2 Differential scanning calorimetry (DSC) 27 3.2.3 Scanning electron microscopy and microstructural analyses 28 3.2.4 X-ray diffraction (XRD) 29 3.2.5 High energy synchrotron X-ray diffraction 29 3.2.6 Mechanical Properties 33 4. Thermal phase stability of single phase high entropy alloys 35 5. An assessment of lattice strain in single phase high entropy alloys 49 5.1 Analysis of micro lattice strain on fcc- and bcc-structured high entropy alloys 50 5.2 Analysis of local lattice strain on fcc- and bcc-structured high entropy alloys 56 6. Solid solution hardening in single phase high entropy alloys 65 6.1 Hardness of fcc- and bcc-structured high entropy alloys 65 6.2 Tensile strength of fcc- and bcc-structured high entropy alloys 70 6.3 Correlation between atomic size misfit and solid solution hardening in Ti-Nb-Hf-Ta-Zr system 82 7. Work hardening in single phase high entropy alloys 91 7.1 Work hardenability of fcc- and bcc-structured high entropy alloys 91 7.2 Dislocation density of fcc- and bcc-structured high entropy alloys after cold swaging 93 8. Summary and outlook 109 8.1 Summary 109 8.2 Outlook 112 References 113 Acknowledgements 131 Erklärung 133