In Gasturbinenbrennern kommen Nickelbasiswerkstoffe für thermisch hoch belastete Komponenten standardmäßig zum Einsatz. Die Bauteile liegen strömungstechnisch vor der stattfindenden Verbrennung, wodurch es zu einer stark einseitigen thermischen Belastung kommt. Ein wirtschaftlich effizienter Einsatz von Nickelbasiswerkstoffen kann daher in Kombination mit kostengünstigen warmfesten Stählen für die weniger stark thermisch belasteten Bauteilbereiche erreicht werden. Ziel der vorliegenden Arbeit ist die Prozessentwicklung zum Hochtemperaturlöten von im Brennerbau häufig verwendeten Nickelbasislegierungen und dem niedriglegierten warmfesten Stahl 16Mo3 (1.5415). Im Entwicklungsprozess wurden die Mikrostruktur der Verbunde charakterisiert, die Auswirkungen thermischer Ausdehnungsunterschiede evaluiert und die erreichbare Festigkeit erfasst. An einem Demonstrator wurden die Erkenntnisse im Rahmen der industriellen Fertigung getestet.:1 Einführung 1.1 Einleitung und Motivation 1.2 Stand von Wissenschaft und Technik 1.3 Schlussfolgerungen und Zielsetzung 2 Technologische Grundlagen 2.1 Der Hochtemperaturlötprozess 2.2 Thermische Ausdehnung 2.3 Diffusion 2.4 Metallurgische Prozesse 3 Experimentelle Durchführung 3.1 Grund- und Lotwerkstoffe 3.2 Lötprozesse und Probengeometrien 3.3 Mikrostrukturelle, thermische und mechanische Charakterisierung 4 Ergebnisse und Diskussion 4.1 Mikrostrukturcharakterisierung 4.1.1 Grundwerkstoffe 4.1.2 Lötsystem 16Mo3 – INCONEL 625 4.1.3 Lötsystem 16Mo3 – Nimonic 75 4.1.4 Lötsystem 16Mo3 – Hastelloy X 4.1.5 Lötsystem 16Mo3 – INCONEL 718 4.1.6 Normalisierungsgefüge von 16Mo3 4.1.7 Zusammenfassung der Mikrostrukturcharakterisierung 4.2 Thermische Ausdehnung 4.2.1 Maßänderung 4.2.2 Eigenspannungen 4.3 Mechanische Eigenschaften 4.3.1 Zugversuch 4.3.2 Zugscherversuch 4.3.3 Ermittlung der kritischen Überlapplänge 4.4 Demonstrator 5 Zusammenfassung und Ausblick / Nickel-base alloys for thermally high loaded components are widely used for gas turbine burner parts. By means of flow direction burner parts are located prior to the combustion. They are therefore one-sided thermally loaded. An economical efficient use of nickel based alloys can be achieved in combination with low alloyed steels for thermally less loaded components. The aim of this work is the development of brazing processes for GT-burner manufacturing related nickel based alloys and the low alloyed steel 16Mo3 (1.5415) using nickel based filler materials. The development includes a microstructural characterization of the brazed compounds, the evaluation of thermal expansion behavior and the maximum strength. A final test examines the feasibility by means of industrial manufacturing.:1 Einführung 1.1 Einleitung und Motivation 1.2 Stand von Wissenschaft und Technik 1.3 Schlussfolgerungen und Zielsetzung 2 Technologische Grundlagen 2.1 Der Hochtemperaturlötprozess 2.2 Thermische Ausdehnung 2.3 Diffusion 2.4 Metallurgische Prozesse 3 Experimentelle Durchführung 3.1 Grund- und Lotwerkstoffe 3.2 Lötprozesse und Probengeometrien 3.3 Mikrostrukturelle, thermische und mechanische Charakterisierung 4 Ergebnisse und Diskussion 4.1 Mikrostrukturcharakterisierung 4.1.1 Grundwerkstoffe 4.1.2 Lötsystem 16Mo3 – INCONEL 625 4.1.3 Lötsystem 16Mo3 – Nimonic 75 4.1.4 Lötsystem 16Mo3 – Hastelloy X 4.1.5 Lötsystem 16Mo3 – INCONEL 718 4.1.6 Normalisierungsgefüge von 16Mo3 4.1.7 Zusammenfassung der Mikrostrukturcharakterisierung 4.2 Thermische Ausdehnung 4.2.1 Maßänderung 4.2.2 Eigenspannungen 4.3 Mechanische Eigenschaften 4.3.1 Zugversuch 4.3.2 Zugscherversuch 4.3.3 Ermittlung der kritischen Überlapplänge 4.4 Demonstrator 5 Zusammenfassung und Ausblick

Um die Leistung und Lebensdauer von energietechnischen Komponenten weiter zu steigern, sind höhere Leistungen, Leistungsdichten sowie Prozesswirkungsgrade zentrale Bestandteile künftiger Entwicklungen. Mit steigernden Leistungsdichten erhöhen sich auch stetig die Belastungen der einzelnen Komponenten. Zusammen mit neuen Werkstoffen und technologischem Fortschritt, wie beispielsweise verbesserten Kühltechnologien oder strömungstechnischen Optimierungen ermöglicht auch eine verbesserte Kenntnis der Belastungsbedingungen und des Schädigungsverhaltens höhere Leistungen und Leistungsdichten. Aktuelle Gasturbinen und oft auch Kraftwerkskomponenten unterliegen zusätzlich zu den mechanischen und zeitlich variablen thermischen Beanspruchungen auch großen örtlichen thermischen Gradienten, die die Lebensdauer der Komponenten stark beeinflussen. Diese thermischen Gradienten induzieren zum einen zusätzliche Beanspruchungen und die örtlich variablen Temperaturfelder führen zum anderen zu stark variierenden Werkstofffestigkeiten. In dieser Arbeit wird ein Prüfstand zur realistischen Prüfung eines typischen Gasturbinenschaufelmaterials Mar-M247 entwickelt und mit diesem eine systematische experimentelle Untersuchung des Einflusses thermischer Gradienten auf die niederzyklische Ermüdungsfestigkeit unter erhöhten Temperaturen durchgeführt. Im weiteren Teil der Arbeit wird ein visko-elasto-plastisches Materialmodell weiterentwickelt, um die lokal unsymmetrische Beanspruchung der Proben unter zyklischer Last realistisch abbilden zu können. Mit Hilfe von Experimenten aus der Literatur werden dabei zunächst die Grenzen und Möglichkeiten des Modells diskutiert, um es dann auf den konkreten Werkstoff anzupassen. Der wesentliche Vorteil des entwickelten Modells liegt in der verbesserten Beschreibung des zyklischen Kriechens und zyklischen Relaxierens (Ratcheting) insbesondere unter einachsiger Beanspruchung und in der nachträglichen Anpassungsmöglichkeit des spezifischen Ratchetingterms nach der Anpassung aller anderen Materialparameter. Die Analyse der experimentell ermittelten Lebensdauern erfolgt sowohl mit ingenieurmäßigen Methoden basierend auf der spannungsabhängigen Lebensdauerbeschreibung nach Basquinund Wöhler als auch mittels eines lokalen bruchmechanischen Ansatzes, der es ermöglicht,sowohl die Rissinitiierung als auch den Rissfortschritt unter variabler Temperatur und kombinierter Kriech- und Ermüdungsbeanspruchung zu beschreiben. Das Material- und Lebensdauermodell werden zusammen im letzten Teil der Arbeit eingesetzt, um das Verformungs- und Lebensdauerverhalten der untersuchten Proben zu berechnenund es kann gezeigt werden, dass sich die Versuche mit sehr guter Qualität wiedergeben lassen.:Versicherung i Abstract iii Kurzfassung v List of abbreviations and symbols xi 1 Introduction 1 2 Objective 5 3 State of the art 7 3.1 Thermal and mechanical loading of gas turbine components . . . . . . . . . . 7 3.2 Material characterisation of nickel-based superalloys . . . . . . . . . . . . . . 9 3.3 Deformation modelling based on constitutive material laws . . . . . . . . . . 13 3.3.1 Ramberg-Osgood material law . . . . . . . . . . . . . . . . . . . . . . 13 3.3.2 Strain and stress tensor . . . . . . . . . . . . . . . . . . . . . . . . . . 14 3.3.3 Thermodynamic principles . . . . . . . . . . . . . . . . . . . . . . . . 14 3.4 Elasto-visco-plastic material models . . . . . . . . . . . . . . . . . . . . . . . 15 3.4.1 Isotropic hardening . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 17 3.4.2 Kinematic hardening . . . . . . . . . . . . . . . . . . . . . . . . . . . . 17 3.4.3 Kinematic hardening for improved simulation of ratcheting . . . . . . 18 3.4.4 Viscosity . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 21 3.5 Failure at elevated temperatures . . . . . . . . . . . . . . . . . . . . . . . . . 22 3.5.1 Fundamental fatigue life models . . . . . . . . . . . . . . . . . . . . . 24 3.5.2 Creep . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 27 3.5.3 Crack growth models for fatigue loading . . . . . . . . . . . . . . . . . 28 3.5.4 Creep crack growth based on C(t) and C ∗ . . . . . . . . . . . . . . . . 33 3.5.5 Temperature dependency and normalization methods . . . . . . . . . 35 3.5.6 Lifetime under temperature variation . . . . . . . . . . . . . . . . . . . 37 3.5.7 Influence of mean stresses on lifetime . . . . . . . . . . . . . . . . . . . 38 3.5.8 Influence of oxidation on failure at elevated temperatures . . . . . . . 42 3.5.9 Constitutive damage and crack growth models . . . . . . . . . . . . . 45 3.6 Experimental methods for the generation of large homogeneously distributed heat flux densities . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 51 3.6.1 Resistance heating . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 51 3.6.2 Inductive heating . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 52 3.6.3 Convective heating . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 53 3.6.4 Laser based heating . . . . . . . . . . . . . . . . . . . . . . . . . . . . 54 3.6.5 Radiation heating . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 54 3.7 Conclusion on the state of the art . . . . . . . . . . . . . . . . . . . . . . . . . 56 4 Development of a test system for cyclic fatigue tests under homogeneous surface temperature conditions 59 4.1 Boundary conditions for the development . . . . . . . . . . . . . . . . . . . . 59 4.2 Concept for a test system with a new highly focusing heating . . . . . . . . . 60 4.2.1 Simulation of heat fluxes of different furnace geometries by ray-tracing 60 4.3 Definition of reflection and transmission coefficient . . . . . . . . . . . . . . . 64 4.3.1 Simulation of the radiation behaviour for the furnace concepts . . . . 66 4.4 Analytical calculation of heat transfer inside the hollow specimen . . . . . . . 71 4.5 Finite element calculation of temperature distribution in the specimen wall . 73 4.6 Design and evaluation of the specimen internal cooling system . . . . . . . . . 75 4.6.1 Installation of heating and development of the load train . . . . . . . 81 5 Experimental investigation 85 5.1 Measurement of surface temperatures and thermal gradients . . . . . . . . . . 87 5.1.1 Measurement of surface temperature . . . . . . . . . . . . . . . . . . . 87 5.1.2 Axial surface temperature distribution . . . . . . . . . . . . . . . . . . 90 5.1.3 Measurement of thermal gradients across specimen wall . . . . . . . . 92 5.2 Results of isothermal ratcheting tests . . . . . . . . . . . . . . . . . . . . . . . 96 5.3 Deformation behaviour of cyclic tests with superimposed thermal gradients . 98 5.3.1 Variation of mean strain and mean stress . . . . . . . . . . . . . . . . 98 5.4 Termination criteria for the tests . . . . . . . . . . . . . . . . . . . . . . . . . 100 5.4.1 Measurement of modulus of elasticity . . . . . . . . . . . . . . . . . . 101 5.5 Low cycle fatigue life of Mar-M247 with and without superimposed thermal gradient . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 104 5.6 Results of hollow cylindrical specimen testing with thermal gradients . . . . . 108 6 Microstructural investigation 113 7 Deformation modeling with improved ratcheting simulation based on small scale strain theory 123 7.1 Modeling of ratcheting behaviour of Mar-M247 . . . . . . . . . . . . . . . . 123 7.1.1 Improvement of uniaxial ratcheting description for the Armstrong- Frederick-model . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 124 7.1.2 Evaluation of the proposed model for multiaxiality . . . . . . . . . . . 129 7.2 Application of the deformation model on Mar-M247 . . . . . . . . . . . . . 132 8 Lifetime calculation of the nickel-base-superalloy Mar-M247 based on engineering and crack growth methods 139 8.1 Modification of the Krämer crack growth model . . . . . . . . . . . . . . . . 139 8.2 Choice of basic variable for the fatigue crack growth and crack initiation . . . 140 8.3 Oxidation based crack growth model . . . . . . . . . . . . . . . . . . . . . . . 142 8.4 Creep crack growth . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 148 8.5 Creep . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 149 8.6 Fatigue life . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 152 8.6.1 Extension of the Paris crack growth model based on intrinsic defect size152 8.6.2 Crack length independent formulation of J-integral . . . . . . . . . . . 154 8.7 Combined model for comprehensive description of the crack-initiation and -growth . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 156 8.7.1 Comparison to crack growth experiments . . . . . . . . . . . . . . . . 161 8.7.2 Comparison to fatigue experiments . . . . . . . . . . . . . . . . . . . . 164 9 Application of material and crack growth model to the experiments with superimposed thermal gradient 167 9.1 Geometry function for the hollow specimen investigated . . . . . . . . . . . . 167 9.2 Application of the crack growth model on non-isothermal tests . . . . . . . . 170 9.2.1 Calculation of the stress strain field of hollow cylindrical specimen subjected to thermally induced stress gradients with the elasto-visco- plastic model . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 172 9.2.2 Calculated crack growth behaviour under locally non-isothermal con- ditions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 176 10 Conclusion and outlook 181 Bibliography 185

<div>In this thesis, the role of location-specific microstructural features in the fatigue performance of the safety-critical aerospace components made of Nickel (Ni)-base superalloys and linear friction welded (LFW) Titanium (Ti) alloys has been studied using crystal plasticity finite element (CPFE) simulations, energy dispersive X-ray diffraction (EDD), backscatter electron (BSE) images and digital image correlation (DIC).</div><div><br></div><div>In order to develop a microstructure-sensitive fatigue life prediction framework, first, it is essential to build trust in the quantitative prediction from CPFE analysis by quantifying uncertainties in the mechanical response from CPFE simulations. Second, it is necessary to construct a unified fatigue life prediction metric, applicable to multiple material systems; and a calibration strategy of the unified fatigue life model parameter accounting for uncertainties originating from CPFE simulations and inherent in the experimental calibration dataset. To achieve the first task, a genetic algorithm framework is used to obtain the statistical distributions of the crystal plasticity (CP) parameters. Subsequently, these distributions are used in a first-order, second-moment method to compute the mean and the standard deviation for the stress along the loading direction (σ_load), plastic strain accumulation (PSA), and stored plastic strain energy density (SPSED). The results suggest that an ~10% variability in σ_load and 20%-25% variability in the PSA and SPSED values may exist due to the uncertainty in the CP parameter estimation. Further, the contribution of a specific CP parameter to the overall uncertainty is path-dependent and varies based on the load step under consideration. To accomplish the second goal, in this thesis, it is postulated that a critical value of the SPSED is associated with fatigue failure in metals and independent of the applied load. Unlike the classical approach of estimating the (homogenized) SPSED as the cumulative area enclosed within the macroscopic stress-strain hysteresis loops, CPFE simulations are used to compute the (local) SPSED at each material point within polycrystalline aggregates of 718Plus, an additively manufactured Ni-base superalloy. A Bayesian inference method is utilized to calibrate the critical SPSED, which is subsequently used to predict fatigue lives at nine different strain ranges, including strain ratios of 0.05 and -1, using nine statistically equivalent microstructures. For each strain range, the predicted lives from all simulated microstructures follow a log-normal distribution; for a given strain ratio, the predicted scatter is seen to be increasing with decreasing strain amplitude and are indicative of the scatter observed in the fatigue experiments. Further, the log-normal mean lives at each strain range are in good agreement with the experimental evidence. Since the critical SPSED captures the experimental data with reasonable accuracy across various loading regimes, it is hypothesized to be a material property and sufficient to predict the fatigue life.</div><div><br></div><div>Inclusions are unavoidable in Ni-base superalloys, which lead to two competing failure modes, namely inclusion- and matrix-driven failures. Each factor related to the inclusion, which may contribute to crack initiation, is isolated and systematically investigated within RR1000, a powder metallurgy produced Ni-base superalloy, using CPFE simulations. Specifically, the role of the inclusion stiffness, loading regime, loading direction, a debonded region in the inclusion-matrix interface, microstructural variability around the inclusion, inclusion size, dissimilar coefficient of thermal expansion (CTE), temperature, residual stress, and distance of the inclusion from the free surface are studied in the emergence of two failure modes. The CPFE analysis indicates that the emergence of a failure mode is an outcome of the complex interaction between the aforementioned factors. However, the possibility of a higher probability of failure due to inclusions is observed with increasing temperature, if the CTE of the inclusion is higher than the matrix, and vice versa. Any overall correlation between the inclusion size and its propensity for damage is not found, based on inclusion that is of the order of the mean grain size. Further, the CPFE simulations indicate that the surface inclusions are more damaging than the interior inclusions for similar surrounding microstructures. These observations are utilized to instantiate twenty realistic statistically equivalent microstructures of RR1000 – ten containing inclusions and remaining ten without inclusions. Using CPFE simulations with these microstructures at four different temperatures and three strain ranges for each temperature, the critical SPSED is calibrated as a function of temperature for RR1000. The results suggest that critical SPSED decreases almost linearly with increasing temperature and is appropriate to predict the realistic emergence of the competing failure modes as a function of applied strain range and temperature.</div><div><br></div><div>LFW process leads to the development of significant residual stress in the components, and the role of residual stress in the fatigue performance of materials cannot be overstated. Hence, to ensure fatigue performance of the LFW Ti alloys, residual strains in LFW of similar (Ti-6Al-4V welded to Ti-6Al-4V or Ti64-Ti64) and dissimilar (Ti-6Al-4V welded to Ti-5Al-5V-5Mo-3Cr or Ti64-Ti5553) Ti alloys have been characterized using EDD. For each type of LFW, one sample is chosen in the as-welded (AW) condition and another sample is selected after a post-weld heat treatment (HT). Residual strains have been separately studied in the alpha and beta phases of the material, and five components (three axial and two shear) have been reported in each case. In-plane axial components of the residual strains show a smooth and symmetric behavior about the weld center for the Ti64-Ti64 LFW samples in the AW condition, whereas these components in the Ti64-Ti5553 LFW sample show a symmetric trend with jump discontinuities. Such jump discontinuities, observed in both the AW and HT conditions of the Ti64-Ti5553 samples, suggest different strain-free lattice parameters in the weld region and the parent material. In contrast, the results from the Ti64-Ti64 LFW samples in both AW and HT conditions suggest nearly uniform strain-free lattice parameters throughout the weld region. The observed trends in the in-plane axial residual strain components have been rationalized by the corresponding microstructural changes and variations across the weld region via BSE images. </div><div><br></div><div>In the literature, fatigue crack initiation in the LFW Ti-6Al-4V specimens does not usually take place in the seemingly weakest location, i.e., the weld region. From the BSE images, Ti-6Al-4V microstructure, at a distance from the weld-center, which is typically associated with crack initiation in the literature, are identified in both AW and HT samples and found to be identical, specifically, equiaxed alpha grains with beta phases present at the alpha grain boundaries and triple points. Hence, subsequent fatigue performance in LFW Ti-6Al-4V is analyzed considering the equiaxed alpha microstructure.</div><div><br></div><div>The LFW components made of Ti-6Al-4V are often designed for high cycle fatigue performance under high mean stress or high R ratios. In engineering practice, mean stress corrections are employed to assess the fatigue performance of a material or structure; albeit this is problematic for Ti-6Al-4V, which experiences anomalous behavior at high R ratios. To address this problem, high cycle fatigue analyses are performed on two Ti-6Al-4V specimens with equiaxed alpha microstructures at a high R ratio. In one specimen, two micro-textured regions (MTRs) having their c-axes near-parallel and perpendicular to the loading direction are identified. High-resolution DIC is performed in the MTRs to study grain-level strain localization. In the other specimen, DIC is performed on a larger area, and crack initiation is observed in a random-textured region. To accompany the experiments, CPFE simulations are performed to investigate the mechanistic aspects of crack initiation, and the relative activity of different families of slip systems as a function of R ratio. A critical soft-hard-soft grain combination is associated with crack initiation indicating possible dwell effect at high R ratios, which could be attributed to the high-applied mean stress and high creep sensitivity of Ti-6Al-4V at room temperature. Further, simulations indicated more heterogeneous deformation, specifically the activation of multiple families of slip systems with fewer grains being plasticized, at higher R ratios. Such behavior is exacerbated within MTRs, especially the MTR composed of grains with their c-axes near parallel to the loading direction. These features of micro-plasticity make the high R ratio regime more vulnerable to fatigue damage accumulation and justify the anomalous mean stress behavior experienced by Ti-6Al-4V at high R ratios.</div><div><br></div>