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I beams
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Image
Published: 01 June 2008
Image
Published: 30 November 2013
Fig. 1 Spontaneous residual stress fracture in a 40-ft-long I-beam under no external load. Source: Ref 1
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Image
Published: 01 November 2013
Image
in Common Causes of Failures
> Failure Analysis of Engineering Structures: Methodology and Case Histories
Published: 01 October 2005
Fig. 2.16 12 m long I-beam split along the web. Source: Ref 10 . With kind permission of Reinhold Publishing Company
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Image
Published: 01 December 1995
Book Chapter
Series: ASM Technical Books
Publisher: ASM International
Published: 01 December 1996
DOI: 10.31399/asm.tb.phtpclas.t64560263
EISBN: 978-1-62708-353-9
... Abstract Structural steels are used for components such as I-beams and automobile frames. This chapter focuses on processing these steels to attain a fine primary ferrite grain size to develop high strength. It first reviews the concepts and principles of recrystallization in plastically...
Abstract
Structural steels are used for components such as I-beams and automobile frames. This chapter focuses on processing these steels to attain a fine primary ferrite grain size to develop high strength. It first reviews the concepts and principles of recrystallization in plastically deformed metals. The chapter reviews the concepts of annealing of cold worked metals. It then looks at hot working and the grain size associated with it. Additionally, the chapter reviews the methods of strengthening in the steels that rely mainly on reduction in the primary ferrite grain size. It discusses basic methods used to develop a small austenite grain size, and hence a small primary ferrite grain size. Then, the chapter covers the processes involved in the precipitation hardening of the ferrite. Finally, it examines some commercial thermomechanical processes used on structural steels, namely hot deformation and controlled cooling.
Image
in Evaluation of Stress-Corrosion Cracking[1]
> Stress-Corrosion Cracking: Materials Performance and Evaluation
Published: 01 January 2017
Fig. 17.28 Configuration and K I calibration of a double-beam plate specimen. Normalized stress intensity K I plotted against a/H ratio. (W − a) indifferent, crackline-loaded, single-edge cracked specimen. Source: Ref 17.26
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Image
Published: 01 March 2006
Fig. 10.6 Schematic of decrease in reflected intensity (normalized) of a laser beam impinged at an angle to the surface of a metal being fatigued
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Image
Published: 30 September 2023
Series: ASM Technical Books
Publisher: ASM International
Published: 01 July 1997
DOI: 10.31399/asm.tb.wip.t65930141
EISBN: 978-1-62708-359-1
... edges Axial Corners 1(F) Plain plate, flame-cut edges Axial Edges 2 Rolled I-beam Bending Corners 2A Riveted I-beam Bending Holes 3 Longitudinally welded plate, as-welded Axial Ripple 3(G) Longitudinally welded plate, weld ground Axial Corners or discontinuity 4...
Abstract
This article is intended to help engineers understand why the fatigue behavior of weldments can be such a confusing and seemingly contradictory topic and hopefully to clarify this complex subject. It first reexamines the factors influencing the fatigue behavior of an individual weldment using extensive experimental data and a computer model that simulates the fatigue resistance of weldments. Next, the process of fatigue in weldments is discussed in general terms, and the service conditions that favor long crack growth and the conditions that favor crack nucleation are contrasted. The article then presents experimental data that show the effect of weldment geometry on fatigue resistance. Several useful geometry classification systems are compared. Finally, a computer model is employed to investigate the behavior of two hypothetical weldments: a discontinuity-containing ("Nominal") weldment and a discontinuity-free ("Ideal") weldment.
Book Chapter
Series: ASM Technical Books
Publisher: ASM International
Published: 01 October 2005
DOI: 10.31399/asm.tb.faesmch.t51270005
EISBN: 978-1-62708-301-0
... as assembly errors, abnormal operating conditions, and inadequate maintenance. It also describes the precise usage of terms such as defect, flaw, imperfection, and discontinuity. failure analysis hip implants I beams manufacturing defects piston heads porcelain insulators quill shafts shaft...
Abstract
This chapter identifies the primary causes of service failures and discusses the types of defects from which they stem. It presents more than a dozen examples of failures attributed to such causes as design defects, material defects, and manufacturing or processing defects as well as assembly errors, abnormal operating conditions, and inadequate maintenance. It also describes the precise usage of terms such as defect, flaw, imperfection, and discontinuity.
Book Chapter
Series: ASM Technical Books
Publisher: ASM International
Published: 30 November 2013
DOI: 10.31399/asm.tb.uhcf3.t53630055
EISBN: 978-1-62708-270-9
..., such as a thin-wall tube or a flange of a channel or I-beam section. A vital fact must be recognized in considering a part that has buckled, or in preventing buckling: the load at which a component buckles does not depend on the strength of the material, but on the dimensions of the part and the modulus...
Abstract
Distortion failures are readily identified by the inherent change in size and/or shape. They are serious because they can lead to other types of failure or may even cause complete collapse of structures, such as bridges, ladders, beams, and columns. Distortion failures may be classified in different ways. One way is to consider them either as dimensional distortion (growth or shrinkage) or as shape distortion (such as bending, twisting, or buckling). They may also be classified as being either temporary or permanent in nature. This chapter discusses the nature, causes, and effects of all of these types of failures as well as the methods to manage them.
Image
in Metallographic Technique—Electron Microscopy and Other Advanced Techniques
> Metallography of Steels: Interpretation of Structure and the Effects of Processing
Published: 01 August 2018
side of the region to be sampled by sputtering using a high-energy ion beam (b–e). Images (d) and (e) are top views. The sample is separated from one edge using the ion beam, welded to a needle using an ion beam–assisted platinum deposition, separated from the other edge (f–i), and lifted out (j
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Book Chapter
Series: ASM Technical Books
Publisher: ASM International
Published: 01 June 2008
DOI: 10.31399/asm.tb.emea.t52240631
EISBN: 978-1-62708-251-8
... the h , k , and l indices, there is a fourth index, i , that is used for hexagonal systems. In the Miller-Bravais system, the three axes in the basal plane are denoted by a 1 , a 2 , and a 3 indices, while l is used to denote the intercept with the z -axis. Thus, a plane will have...
Abstract
This appendix explains how to identify crystallographic planes and directions. It shows how Miller indices, a system for specifying crystallographic planes within a unit cell, are determined for cubic and hexagonal systems. It also explains how x-ray diffraction techniques are used in the study of crystalline structures.
Series: ASM Technical Books
Publisher: ASM International
Published: 23 January 2020
DOI: 10.31399/asm.tb.stemsem.t56000001
EISBN: 978-1-62708-292-1
... be obtained (Ref 13). The boundaries defining low-, medium-, and high-angle are not rigidly defined, and different imaging modes are obtained simply by changing the inner and outer acceptance angles, i and o. Note that BF and DF signals can be, and are often mixed to obtain useful information. FIG. 5...
Abstract
This chapter discusses the principles of scanning transmission electron microscopy (STEM) as implemented using conventional scanning electron microscopes (SEMs). It describes the pros and cons of low-energy imaging and diffraction, addresses basic hardware requirements, and provides information on imaging modes, detector positioning and alignment, and the effect of contrast reversal. It also discusses beam convergence and angular selectivity, the use of application-specific masks, and how to generate grain orientation maps for different material systems.
Series: ASM Technical Books
Publisher: ASM International
Published: 01 November 2019
DOI: 10.31399/asm.tb.mfadr7.t91110379
EISBN: 978-1-62708-247-1
... and tilt the sample perpendicular to the ion beam (I-beam). Under appropriate I-beam working conditions, insert the gas needle and start the FIB milling as shown in fig. 11 . Repeat as required to delayer to the desired level. Typically the area of milling can achieve up to 30 μm × 30 μm...
Abstract
With semiconductor device dimension continuously scaling down and increasing complexity in integrated circuits, delayering techniques for reverse engineering is becoming increasingly challenging. The primary goal of delayering in semiconductor failure analysis is to successfully remove layers of material in order to locate and identify the area of interest. Several of the top-down delayering techniques include wet chemical etching, dry reactive ion etching, top-down parallel lapping (including chemical-mechanical polishing), ion beam milling and laser delayering techniques. This article discusses the general procedure, types, advantages, and disadvantages of each of these techniques. In this article, two types of different semiconductor die level backend of line technologies are presented: aluminum metallization and copper metallization.
Book
Series: ASM Technical Books
Publisher: ASM International
Published: 23 January 2020
DOI: 10.31399/asm.tb.stemsem.9781627082921
EISBN: 978-1-62708-292-1
Book Chapter
Series: ASM Technical Books
Publisher: ASM International
Published: 30 September 2024
DOI: 10.31399/asm.tb.pmamfa.t59400391
EISBN: 978-1-62708-479-6
... lattice strain; activation energy for crystallization G gravitational acceleration Η viscosity of solvent; height of powder heap I incident beam current I a intensity of amorphous peak I c intensity of crystalline peak K shape factor K T constant (kinetic...
Series: ASM Technical Books
Publisher: ASM International
Published: 01 November 2019
DOI: 10.31399/asm.tb.mfadr7.t91110434
EISBN: 978-1-62708-247-1
... ionizations that result in a particular x-ray line. Thus the maximum depth for creation of an x-ray produced by a transition with initial ionization energy Ei will be: R max = R ( E o ) − R ( E i ) For example, R(E i ) for the Si K-shell is R KO (E i =1.84 keV) = 0.09...
Abstract
This article provides an overview of the most common micro-analytical technique in the failure analysis laboratory: energy dispersive X-ray spectroscopy (EDS). It discusses the general characteristics, advantages, and disadvantages of some of the X-ray detectors attached to the scanning electron microscope chamber including the lithium-drifted EDS detector, silicon drift detector (SDD), and wavelength dispersive X-ray detector. The article then provides information on qualitative and quantitative X-ray analysis programs followed by a discussion on EDS elemental mapping. The discussion includes a comparison of scanning transmission electron microscope-EDS elemental mapping and mapping with an SDD. A brief section is devoted to the discussion on the artifacts that occur during X-ray mapping.
Series: ASM Technical Books
Publisher: ASM International
Published: 01 January 2017
DOI: 10.31399/asm.tb.sccmpe2.t55090367
EISBN: 978-1-62708-266-2
... intensity on the kinetics of SCC. Stages I and II may not always be straight lines but may be strongly curved, and one or the other may be absent in some systems. Stage III is of little interest and is absent in K -decreasing tests. Source: Ref 17.2 Standardization of SCC Tests Standardization...
Abstract
This chapter addresses the challenge of selecting an appropriate stress-corrosion cracking (SCC) test to evaluate the serviceability of a material for a given application. It begins by establishing a generic model in which SCC is depicted in two stages, initiation and propagation, that further subdivide into several zones plus a transition region. It then discusses SCC test standards before describing basic test objectives and selection criteria. The chapter explains how to achieve the required loading conditions for different tests and how to prepare test specimens to determine elastic strain, plastic strain, and residual stress responses. It also describes the difference between smooth and precracked specimens and how they are used, provides information on slow-strain-rate testing and how to assess the results, and discusses various test environments and procedures, including tests for weldments. The chapter concludes with a section on how to interpret time to failure, threshold stress, percent survival, stress intensity, and propagation rate data, and assess the precision of the associated tests.
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