Methods to Create Compressive Stress in High Strength Steel Components
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Surface Properties of 3D Transition Metals Marko P J Punkkinen, Qing-Miao Hu, Se Kyun Kwon, Borje Johansson, János Kollár, Levente Vitos
Surface properties of 3d transition metals Marko P J Punkkinen, Qing-Miao Hu, Se Kyun Kwon, Borje Johansson, János Kollár, Levente Vitos To cite this version: Marko P J Punkkinen, Qing-Miao Hu, Se Kyun Kwon, Borje Johansson, János Kollár, et al.. Surface properties of 3d transition metals. Philosophical Magazine, Taylor & Francis, 2011, 10.1080/14786435.2011.586953. hal-00714554 HAL Id: hal-00714554 https://hal.archives-ouvertes.fr/hal-00714554 Submitted on 5 Jul 2012 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Philosophical Magazine & Philosophical Magazine Letters For Peer Review Only Surface properties of 3d transition metals Journal: Philosophical Magazine & Philosophical Magazine Letters Manuscript ID: TPHM-11-Feb-0082.R1 Journal Selection: Philosophical Magazine Date Submitted by the 06-May-2011 Author: Complete List of Authors: Punkkinen, Marko; Royal Institute of Technology, Department of Materials Science and Engineering; University of Turku, Department of Physics and Astronomy Hu, Qing-Miao; Institute of Metal Research, Chinese Academy -
Residual Compressive Stress Strengthens Brittle Materials
Residual Compressive Stress Strengthens Brittle Materials Effect of retained residual compressive stress on the ductility of the still hot and ductile subsurface the surface layer of brittle materials in reducing applied surface glass. As cooling continues, the sub tensile stress. Spring test data demonstrate the beneficial effect surface glass contracts against the rela tively cool and rigid surfaces, resulting of residual compressive stress in· the surface of hard steel. in residual tensile stress in the core and corresponding resiqual compres sive stress in the surface.' JOHN 0. ALMEN with glass specimens. Among the · ad The relative static strength of a Research Consultant vantages of glass for evaluating resid specimen of normal glass, which was ual stresses is that at ordinary tem carefully annealed to avoid residual UNDER CONDITIONS of br:ttlc fracture, peratures glass is completely brittle. stresses, and that of a similar glass specimen surfaces are weaker than For this reason, the residual stress pat specimen_that had been quenched on sound subsurface material. When such tern remains unaltered by plastic flow both surfaces as described in the pre relatively weak surfaces are residually to the instant of fracture. Also, any c:!ding paragraph is shown in Fig. 1. stressed in compression, the specimens apparent unorthodox behavior of glass As shown by the insert in Fig. 1, these will support greater tensile loads and will not mistakenly be attributed to specimens were ordinary -! in. plate will exhibit greater ductility because cold work or altered structure. glass, 3 in. wide and 18 in. long. Each the applied surface tensile stress is re Residual compressive stress in glass was placed on supports spaced 12 in. -
Arxiv:1304.0144V1
Thermodynamics of coherent interfaces under mechanical stresses. I. Theory T. Frolov1, ∗ and Y. Mishin1, † 1Department of Physics and Astronomy, MSN 3F3, George Mason University, Fairfax, Virginia 22030, USA Abstract We present a thermodynamic theory of plane coherent solid-solid interfaces in multicomponent systems subject to non-hydrostatic mechanical stresses. The interstitial and substitutional chemical components are treated separately using chemical potentials and diffusion potentials, respectively. All interface excess quan- tities are derived using Cahn’s (1979) generalized excess method without resorting to geometric dividing surfaces. We present expressions for the interface free energy as an excess quantity and derive a general- ized adsorption equation and an interface Gibbs-Helmholtz equation which does not contain the interface entropy. The interface stress tensor emerges naturally from the generalized adsorption equation as an ap- propriate excess over bulk stresses and is shown to be generally non-unique. Another interface property emerging from the generalized adsorption equation is the interface excess shear. This property is specific to coherent interfaces and represents the thermodynamic variable conjugate to the shear stress applied parallel to the interface. The theory reveals a number of Maxwell relations describing cross-effects between ther- mal, chemical and mechanical responses of coherent interfaces. In Part II of this work this theory will be applied to atomistic computer simulations of grain boundaries. PACS numbers: 64.10.+h, 64.70.K-, 68.35.-p, 68.35.Md Keywords: interface thermodynamics, coherent interface, interface free energy, interface stress. arXiv:1304.0144v1 [cond-mat.mtrl-sci] 30 Mar 2013 1 I. INTRODUCTION Thermodynamics properties of interfaces can have a strong impact on microstructure de- velopment in materials by controlling phase nucleation, growth, coarsening and many other processes.1,2. -
In-Situ Measurement and Numerical Simulation of Linear
IN-SITU MEASUREMENT AND NUMERICAL SIMULATION OF LINEAR FRICTION WELDING OF Ti-6Al-4V Dissertation Presented in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy in the Graduate School of The Ohio State University By Kaiwen Zhang Graduate Program in Welding Engineering The Ohio State University 2020 Dissertation Committee Dr. Wei Zhang, advisor Dr. David H. Phillips Dr. Avraham Benatar Dr. Vadim Utkin Copyrighted by Kaiwen Zhang 2020 1 Abstract Traditional fusion welding of advanced structural alloys typically involves several concerns associated with melting and solidification. For example, defects from molten metal solidification may act as crack initiation sites. Segregation of alloying elements during solidification may change weld metal’s local chemistry, making it prone to corrosion. Moreover, the high heat input required to generate the molten weld pool can introduce distortion on cooling. Linear friction welding (LFW) is a solid-state joining process which can produce high-integrity welds between either similar or dissimilar materials, while eliminating solidification defects and reducing distortion. Currently the linear friction welding process is most widely used in the aerospace industry for the fabrication of integrated compressor blades to disks (BLISKs) made of titanium alloys. In addition, there is an interest in applying LFW to manufacture low-cost titanium alloy hardware in other applications. In particular, LFW has been shown capable of producing net-shape titanium pre-forms, which could lead to significant cost reduction in machining and raw material usage. Applications of LFW beyond manufacturing of BLISKs are still limited as developing and quantifying robust processing parameters for high-quality joints can be costly and time consuming. -
A Method for Calculating Surface Stress and Elastic Constants by Molecular Dynamics
A METHOD FOR CALCULATING SURFACE STRESS AND ELASTIC CONSTANTS BY MOLECULAR DYNAMICS Satoshi Izumi Dept. of Mechanical Engineering, Univ. of Tokyo., JAPAN Shotaro Hara Dept. of Mechanical Engineering, Univ. of Tokyo., JAPAN Tomohisa Kumagai Dept. of Mechanical Engineering, Univ. of Tokyo., JAPAN Shinsuke Sakai Dept. of Mechanical Engineering, Univ. of Tokyo., JAPAN Abstract 1 Introduction For nano-scale thin film, effects of The films used in the manufacture surface and interface, which can be ig- of semiconductors are less than 10 nm nored on a macro scale, become impor- thick. At this thickness, the effects of tant. For example, surface energy and surface and interface, which can be ig- stress are key parameters for predicting nored on a macro scale, become impor- the intrinsic stress of thin films. Sev- tant. For example, surface (interface) eral researchers have reported that the energy and stress are key parameters elastic constants of thin films are dif- for predicting the intrinsic stress of thin ferent from those of bulks. We have films, though the stress depends also on recently proposed new definitions and the microstructures and growth mode at calculation methods regarding surface atomic level[1][2]. However, it is difficult stress and elastic constants for thin films to obtain values of surface energy and by extending Martin's method, which surface stress experimentally. Therefore, is useful for obtaining the internal dis- numerical evaluation by molecular sim- placement and elastic constants within ulation has been attempted. In addi- the framework of the molecular dynam- tion, several researchers have reported ics method. We applied our method that the elastic properties (e.g. -
A Curvature-Dependent Interfacial Energy-Based Interface Stress Theory and Its Applications to Nano-Structured Materials: (I) General Theory
Journal of the Mechanics and Physics of Solids 66 (2014) 59–77 Contents lists available at ScienceDirect Journal of the Mechanics and Physics of Solids journal homepage: www.elsevier.com/locate/jmps A curvature-dependent interfacial energy-based interface stress theory and its applications to nano-structured materials: (I) General theory Xiang Gao a, Zhuping Huang a, Jianmin Qu b, Daining Fang a,n a LTCS and Department of Mechanics and Engineering Science, College of Engineering, Peking University, Beijing 100871, China b Department of Civil and Environmental Engineering, Northwestern University, Evanston, IL 60208, USA article info abstract Article history: Experimental observations have shown the size-dependent residual surface stresses on Received 24 July 2013 spherical nanoparticles and their influence on the effective modulus of heterogeneous Received in revised form nanostructures. Based on these experimental findings, this paper proposes a new interface 17 December 2013 stress theory that considers the curvature effect on the interfacial energy. To investigate Accepted 31 January 2014 this curvature-dependent interfacial energy, we use the Green elasticity theory to describe Available online 10 February 2014 the nonlinear constitutive relation of the interface at finite deformation, thus explicitly Keywords: demonstrating the curvature-dependent nature of the interface stress and bending Curvature-dependence moment. By introducing a fictitious stress-free configuration, we then propose a new Interfacial energy energy functional for heterogeneous hyperelastic solids with interfaces. For the first time, Interface constitutive relation both the Lagrangian and Eulerian descriptions of the generalized Young–Laplace equation, Generalized Young–Laplace equation Residual elastic field which describes the intrinsic flexural resistance of the interface, are derived from the newly developed energy functional. -
Experimental Determination of Surface Stress Changes in Electro- Chemical Systems – Possibilities and Pitfalls”, Chem
Experimental methods for the determination of stress changes at electrified solidliquid interfaces Gyözö G. Láng*, Noémi Kovács, Soma Vesztergom, Mária Ujvári, Dóra Zalka, Krisztina Sze- keres Eötvös Loránd University, Institute of Chemistry, Department of Physical Chemistry H-1117 Budapest, Pázmány P. s. 1/A Abstract: In the present study some of the methods developed for the experimental determina- tion of (interfacial or film) stress changes in electrochemical systems containing solid-liquid interfaces are briefly reviewed, as well as the kind and quality of information that can be ob- tained using these methods are discussed. The “bending beam” (“bending cantilever”, “laser beam deflection”, ”wafer curvature”) method and related techniques, the piezoelectric method, the extensometer method, and the method based on the measurement of contact angle are dis- cussed in detail. Special attention has been paid to problems related to the use of optical meth- ods for position sensing. Keywords: solid-liquid interface, solid electrode, electrocapillarity, interface stress 1 Introduction The intensive parameter conjugate to surface area [1] (often called the “surface tension”, “interfacial tension”, “surface stress”, “interface stress” or “specific surface energy”) is an im- portant parameter in the thermodynamic theory of electrodes, since most electrochemical sys- tems are, in fact, capillary systems, because any interaction between the bulk solid and the remainder of the system takes place via the interface region. The thermodynamic properties of this region (i.e. the electronic conductor | ionic conductor interface, for instance the interface between a metal and an electrolyte solution) directly influence the electrochemical processes, an understanding of the thermodynamics of interfaces is of importance to all surface scientists and electrochemists. -
11283: Engineered Residual Stress to Mitigate Stress Corrosion Cracking
Paper No. 2011 11283 Engineered Residual Stress to Mitigate Stress Corrosion Cracking of Stainless Steel Weldments Jeremy E. Scheel, N. Jayaraman, Douglas J. Hornbach Lambda Technologies 5521 Fair Lane Cincinnati, OH, 45227-3401 USA ABSTRACT Stress corrosion cracking (SCC) is the result of the combined influence of tensile stress and a corrosive environment on a susceptible material. Austenitic stainless steels including types 304L and 316L are susceptible alloys commonly used in nuclear weldments. An engineered residual stress field can be introduced into the surface of components that can reliably produce thermo-mechanically stable, deep compressive residual stresses to mitigate SCC. The stability of the residual stresses is dependant on the amount of cold working produced during surface enhancement processing. Three different symmetrical geometries of weld mockups were processed using low plasticity burnishing (LPB) to produce the desired compressive residual stress field on half of each specimen. SCC testing in boiling MgCl2 was performed to compare the LPB treated and un-treated 304L and 316L stainless steel weldments. X-ray diffraction residual stress analyses were used to document the respective residual stress fields and percent cold working of each condition. Testing was performed to quantify the thermo-mechanical stability of the residual stresses. The un-treated weldments suffered severe SCC damage due to the residual tension from the welding operation. The results show conclusively that LPB completely mitigated SCC in the tested weldments and provided thermo-mechanically stable, deep residual compression. KEYWORDS: Stress Corrosion Cracking, Low Plasticity Burnishing, Residual Stress, Weldments, Nuclear Reactor, Stainless Steel. ©2011 by NACE International. Requests for permission to publish this manuscript in any form, in part or in whole, must be in writing to NACE International, Publications Division, 1440 South Creek Drive, Houston, Texas 77084. -
Effect of Tensile Residual Stress on Brittle Fracture of Ferritic Steel
INFLUENCE OF RESIDUAL STRESSES ON BRITTLE FRACTURE OF FERRITIC STEELS A. Mirzaee Sisan, C. E. Truman and D. J. Smith Department of Mechanical Engineering, University of Bristol, Queen’s Building, University Walk, Bristol, BS8 1TR, UK. ABSTRACT An experimental and numerical study is presented which demonstrates the significant effect of tensile residual stress fields on the brittle fracture of ferritic steels. A residual stress field was introduced into laboratory specimens, specifically single edge notched bend, SEN(B), and round notched bars, RNB, using in-plane compression. In-plane compression consists of applying a compressive load along the longitudinal axis of a specimen containing a shallow notch and then unloading at room temperature. The specimens were then cooled to a temperature of -150oC and reloaded to fracture after introduction of a sharp notch. Numerical analyses utilizing ABAQUS finite element code were carried out to simulate the process of in-plane compression. The numerical studies demonstrated that a high tensile residual stress region was created at the notch tip. A considerable decrease in fracture stress and fracture toughness was observed as a result of in- plane compression. The results emphasise the significant role of residual stresses in the fracture behaviour of ferritic steels. 1 INTRODUCTION Residual stress fields have significant effect on the fracture load of structures [1]. Welding is one of the major causes of residual stresses. The magnitude of weld residual stress can be as high as the yield strength of the material [2]. The tensile residual stress field can be combined with in- service stresses and promote failure [2,3]. -
Equation of Motion for Viscous Fluids
1 2.25 Equation of Motion for Viscous Fluids Ain A. Sonin Department of Mechanical Engineering Massachusetts Institute of Technology Cambridge, Massachusetts 02139 2001 (8th edition) Contents 1. Surface Stress …………………………………………………………. 2 2. The Stress Tensor ……………………………………………………… 3 3. Symmetry of the Stress Tensor …………………………………………8 4. Equation of Motion in terms of the Stress Tensor ………………………11 5. Stress Tensor for Newtonian Fluids …………………………………… 13 The shear stresses and ordinary viscosity …………………………. 14 The normal stresses ……………………………………………….. 15 General form of the stress tensor; the second viscosity …………… 20 6. The Navier-Stokes Equation …………………………………………… 25 7. Boundary Conditions ………………………………………………….. 26 Appendix A: Viscous Flow Equations in Cylindrical Coordinates ………… 28 ã Ain A. Sonin 2001 2 1 Surface Stress So far we have been dealing with quantities like density and velocity, which at a given instant have specific values at every point in the fluid or other continuously distributed material. The density (rv ,t) is a scalar field in the sense that it has a scalar value at every point, while the velocity v (rv ,t) is a vector field, since it has a direction as well as a magnitude at every point. Fig. 1: A surface element at a point in a continuum. The surface stress is a more complicated type of quantity. The reason for this is that one cannot talk of the stress at a point without first defining the particular surface through v that point on which the stress acts. A small fluid surface element centered at the point r is defined by its area A (the prefix indicates an infinitesimal quantity) and by its outward v v unit normal vector n . -
Residual Stress Measurement by the Introduction of Slots Or Cracks I
Transactions on Engineering Sciences vol 13, © 1996 WIT Press, www.witpress.com, ISSN 1743-3533 Residual stress measurement by the introduction of slots or cracks I. Finnic, W.Cheng Department of Mechanical Engineering, University of California, Abstract A relatively new approach for the experimental measurement of residual stress is outlined and extended. In essence, it makes use of strain measurement as a slot of progressively increasing depth is introduced into a body. For near- surface residual stress measurement the Nisitani "body force method" is used to determine residual stresses from strain measurement In cases in which through-the-thickness stress measurement is desired it is shown that many solutions may be obtained from procedures based on linear elastic fracture mechanics. Although the method requires more extensive prior numerical computation than traditional methods, it involves a simple experimental pro- cedure and in many cases leads to much greater precision in prediction of resi- dual stresses than traditional methods. 1 Introduction Residual stress is a topic of major importance in any discussion of the mechan- ical behavior of materials. In many important applications residual stresses have led to premature failure. By contrast, compressive residual stresses are often introduced deliberately to extend the life of parts. As a result there is an extensive literature on the measurement of residual stress. More recently, with enhanced computational ability, the numerical simulation of residual stress has received increasing -
Residual Stress Effects on Fatigue Life Via the Stress Intensity Parameter, K
University of Tennessee, Knoxville TRACE: Tennessee Research and Creative Exchange Doctoral Dissertations Graduate School 12-2002 Residual Stress Effects on Fatigue Life via the Stress Intensity Parameter, K Jeffrey Lynn Roberts University of Tennessee - Knoxville Follow this and additional works at: https://trace.tennessee.edu/utk_graddiss Part of the Engineering Science and Materials Commons Recommended Citation Roberts, Jeffrey Lynn, "Residual Stress Effects on Fatigue Life via the Stress Intensity Parameter, K. " PhD diss., University of Tennessee, 2002. https://trace.tennessee.edu/utk_graddiss/2196 This Dissertation is brought to you for free and open access by the Graduate School at TRACE: Tennessee Research and Creative Exchange. It has been accepted for inclusion in Doctoral Dissertations by an authorized administrator of TRACE: Tennessee Research and Creative Exchange. For more information, please contact [email protected]. To the Graduate Council: I am submitting herewith a dissertation written by Jeffrey Lynn Roberts entitled "Residual Stress Effects on Fatigue Life via the Stress Intensity Parameter, K." I have examined the final electronic copy of this dissertation for form and content and recommend that it be accepted in partial fulfillment of the equirr ements for the degree of Doctor of Philosophy, with a major in Engineering Science. John D. Landes, Major Professor We have read this dissertation and recommend its acceptance: J. A. M. Boulet, Charlie R. Brooks, Niann-i (Allen) Yu Accepted for the Council: Carolyn R. Hodges Vice Provost and Dean of the Graduate School (Original signatures are on file with official studentecor r ds.) To the Graduate Council: I am submitting herewith a dissertation written by Jeffrey Lynn Roberts entitled “Residual Stress Effects on Fatigue Life via the Stress Intensity Parameter, K.” I have examined the final electronic copy of this dissertation for form and content and recommend that it be accepted in partial fulfillment of the requirements for the degree of Doctor of Philosophy, with a major in Engineering Science.