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in Basic Inspection Methods (Pulse-Echo and Transmission Methods)[1]
> Nondestructive Evaluation of Materials
Published: 01 August 2018
Fig. 5 Structure of a piezoelectric-based longitudinal (compression) wave transducer. Courtesy of Iowa State University Center for Nondestructive Evaluation
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Published: 01 January 2001
Book Chapter
Book: Composites
Series: ASM Handbook
Volume: 21
Publisher: ASM International
Published: 01 January 2001
DOI: 10.31399/asm.hb.v21.a0003383
EISBN: 978-1-62708-195-5
... describes the damping characteristics of unidirectional composites, when they are subjected to longitudinal shear, longitudinal tension/compression, and transverse tension/compression. It presents equations that govern the overall damping capacity of beams that are cut from laminated plates. The article...
Abstract
Damping is the energy dissipation properties of a material or system under cyclic stress. The vibrational and damping characteristics of composites are important in many applications, including ground-based and airborne vehicles, space structures, and sporting goods. This article describes the damping characteristics of unidirectional composites, when they are subjected to longitudinal shear, longitudinal tension/compression, and transverse tension/compression. It presents equations that govern the overall damping capacity of beams that are cut from laminated plates. The article discusses the effect of temperature on damping and provides information on the relationship between damping and strength.
Book: Composites
Series: ASM Handbook
Volume: 21
Publisher: ASM International
Published: 01 January 2001
DOI: 10.31399/asm.hb.v21.a0003379
EISBN: 978-1-62708-195-5
... in which they are used. The characterization of fiber failures in laminates is presented first. Then situations in which the matrix fails first either by intent, by design error, or because of impact damage follow. It is shown that the longitudinal compressive strength of embedded fibers can be limited...
Abstract
This article presents a comprehendable and comprehensive physics-based approach for characterizing the strength of fiber-reinforced polymer composites. It begins with background information on the goals and attributes of this method. The article then addresses the characterization of fiber failures in laminates, because these are at the highest strengths that can be attained and, therefore, are usually the design objective. An exception would be if the design goal is to maximize energy absorption, rather than static strength. The discussion proceeds to situations in which the matrix fails first, either by intent, by design error, or because of impact damage. The state of the modeling propagation and arrest of matrix damage follows. Comparisons of this physics-based approach are then made to empirically based failure theories.
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Published: 01 January 2005
Fig. 26 Measured localized strains during the rolling of lead bars. Left side shows longitudinal tensile strain versus vertical compressive strain. Right side shows longitudinal strain versus cross-sectional area reduction at room temperature.
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Published: 01 January 2005
Fig. 24 Measured localized strains during the rolling of lead bars. Left side shows longitudinal strain versus vertical compressive strain. Right side shows longitudinal strain versus cross-section reduction of area at room temperature. Source: Ref 28
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Published: 01 January 2005
Fig. 35 Measured localized strains during rolling of lead bars. Left side shows longitudinal tensile strain versus vertical compressive strain. Right side shows longitudinal strain versus cross-sectional area reduction at room temperature. Source: Ref 37
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Published: 01 January 2005
Fig. 8 Effect of draft design on the compressive strain distribution. Solid line indicates compressive strain; broken line, longitudinal strain. (a) 5% reduction increments. (b) 8% reduction increments. (c) 10% reduction increments
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Book Chapter
Series: ASM Desk Editions
Publisher: ASM International
Published: 01 December 1998
DOI: 10.31399/asm.hb.mhde2.a0003236
EISBN: 978-1-62708-199-3
... mm ( 1 4 in.). Improved resolution can be obtained by using shear waves, because these have shorter wavelengths than compression waves of the same frequency in the solid. (The velocity of a longitudinal wave in a solid is greater than that of the shear wave of the same frequency.) Large...
Abstract
Ultrasonic inspection is a nondestructive method in which beams of high-frequency acoustic energy are introduced into a material to detect surface and subsurface flaws, to measure the thickness of the material, and to measure the distance to a flaw. This article provides a detailed account of ultrasonic flaw detectors, including ultrasonic transducers and types of search units and couplants. The article describes pulse-echo and transmission inspection methods and data interpretation. The general characteristics of ultrasonic waves and the factors influencing ultrasonic inspection are also addressed. The article concludes with a review of the advantages and disadvantages of ultrasonic inspection compared with other methods applications of the technique.
Series: ASM Handbook
Volume: 6
Publisher: ASM International
Published: 01 January 1993
DOI: 10.31399/asm.hb.v06.a0001475
EISBN: 978-1-62708-173-3
... transverse to σ x , designated σ y , which are called the transverse stresses. The distribution of the longitudinal stress is shown in Fig. 3(b) . Near the weld, tensile stresses of high magnitude are produced. These taper off quickly and become compressive at a distance equal to several times the width...
Abstract
This article describes the formation of residual stresses and distortion, providing information on the techniques for measuring residual stresses. It presents a detailed discussion on the magnitude and distribution analysis of the residual stresses and distortion in weldments. The article briefly explains the effects of residual stresses and distortion on the brittle fracture and fatigue fracture of welded structures. It also provides information on the thermal treatments of weldments.
Series: ASM Handbook
Volume: 6A
Publisher: ASM International
Published: 31 October 2011
DOI: 10.31399/asm.hb.v06a.a0005617
EISBN: 978-1-62708-174-0
... transverse to σ x , designated σ y , which are called the transverse stresses. The distribution of the longitudinal stress is shown in Fig. 3 . Near the weld, tensile stresses of high magnitude are produced. These taper off quickly and become compressive at a distance equal to several times the width...
Abstract
This article describes the formation of residual stresses and distortion and the techniques for measuring residual stresses. It provides a discussion on the magnitude and distribution analysis of residual stresses and distortion in weldments. The article considers the effects of residual stresses and distortion on the brittle fracture and fatigue fracture of welded structures. The thermal treatments of weldments are also discussed.
Book Chapter
Series: ASM Handbook
Volume: 2B
Publisher: ASM International
Published: 15 June 2019
DOI: 10.31399/asm.hb.v02b.a0006746
EISBN: 978-1-62708-210-5
... incumbent 7 x 75 and 7150 alloys. It is one of the highest strength alloys with longitudinal yield strength of 600 MPa (87 ksi) in the peaked aged (T6) and 580 MPa (84) in sections under 40 mm (1.5 in.) in the T79 tempers. Toughness and stress-corrosion cracking (SCC) resistance are comparable with other...
Abstract
This datasheet provides information on key alloy metallurgy and processing effects on mechanical and corrosion performance properties of aluminum alloy 7449. A comparison of toughness and stress-corrosion cracking resistance of alloy 7449 with other alloys is also provided.
Series: ASM Handbook
Volume: 17
Publisher: ASM International
Published: 01 August 2018
DOI: 10.31399/asm.hb.v17.a0006470
EISBN: 978-1-62708-190-0
... Waves Longitudinal waves, sometimes called compression waves, are the type of ultrasonic waves most widely used in the inspection of materials. These waves travel through materials as a series of alternate compressions and rarefactions in which the particles transmitting the wave vibrate back...
Abstract
Ultrasonic inspection is a family of nondestructive methods in which beams of high-frequency mechanical waves are introduced into materials, using transducers, for the detection and characterization of both surface and subsurface anomalies and flaws in the material. This article describes the basic equipment in ultrasonic inspection systems, and lists the advantages and disadvantages of these systems. It discusses the applications of ultrasonic inspection and also the general characteristics of ultrasonic waves in terms of wave propagation, longitudinal waves, transverse waves, surface waves, and lamb waves. The article reviews the major variables in ultrasonic inspection, including frequency, acoustic impedance, angle of incidence, and beam intensity. It discusses the attenuation of ultrasonic beams and provides information on the pulse-echo and transmission methods for implementing ultrasonic inspection.
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Published: 01 January 2000
Fig. 4 Tensile and compressive modulus at half-hard and full-hard type 301 stainless steel in the transverse and longitudinal directions. Source: Ref 5
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Published: 01 August 2018
Fig. 4 Schematic of longitudinal ultrasonic waves. (a) Particle oscillation and resultant rarefaction and compression. (b) Amplitude of particle displacement versus distance of wave travel. The wavelength, λ, is the distance corresponding to one complete cycle.
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Published: 01 December 1998
Fig. 11 Schematic representation of longitudinal ultrasonic waves. (a) Particle oscillation and resultant rarefaction and compression. (b) Amplitude of particle displacement versus distance of wave travel. The wavelength (λ) is the distance corresponding to one complete cycle.
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Series: ASM Handbook
Volume: 8
Publisher: ASM International
Published: 01 January 2000
DOI: 10.31399/asm.hb.v08.a0003304
EISBN: 978-1-62708-176-4
... for transverse tensile stresses at the rear surface of the specimen. These amplitudes are of the order of 15% of the longitudinal compressive stress in the incident plane wave. It should be pointed out that this amplitude represents an upper bound for such stresses. First, in real experiments there is a lack...
Abstract
Impact tests are used to study dynamic deformation and failure modes of materials. This article discusses low-velocity impact experiments in single-stage gas guns. It describes surface velocity measurements with laser interferometric techniques. The article details plate impact soft-recovery experiments, pressure-shear friction experiments, and low-velocity penetration experiments. It reviews two types of plate impact soft-recovery experiments: normal plate impact and pressure-shear plate impact experiments. The article provides information on low-velocity penetration experiments, which include the setup for direct penetration experiment (rod-on-plate) and the reverse penetration experiment (plate-on-rod). It also considers high-temperature plate impact testing and impact techniques with in-material stress and velocity measurements.
Series: ASM Handbook
Volume: 4B
Publisher: ASM International
Published: 30 September 2014
DOI: 10.31399/asm.hb.v04b.a0005936
EISBN: 978-1-62708-166-5
... and the thermal conductivity of the material, leading to higher thermal/cooling stresses in the case of water quenching in comparison to oil. As a consequence, the surface layers of the cylinder are subjected to tensile stresses in longitudinal and tangential directions, whereas compressive stresses arise...
Abstract
In the case of steels, heat treatment plays a fundamental role because no other process step can manipulate the microstructure in order to fulfill such a wide variety of possible in-service conditions. This article addresses heat treatment with regard to hardening and subsequent tempering of steel components in order to optimize tribological properties. It focuses on the heat treatment of tempering and bearing steels and on volume changes that take place due to phase transformations. Plastic deformations that occur due to shrinking and phase transformation are also discussed. The article also describes the generation of thermal, transformation, and hardening residual stresses.
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Published: 01 January 2005
Fig. 3 Transmission electron micrographs of foils taken in the longitudinal through thickness plane of specimens of commercial purity Al-1%Mg deformed in plane strain compression at 385 °C (725 °F) and 2.5/s to equivalent strains of (a) 0.7 and (b) 1.0 ( Ref 2 )
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Published: 01 January 2005
Fig. 4 Transmission electron micrograph of a foil in the longitudinal through thickness plane of a specimen of Fe-30%Ni-0.1%Nb steel deformed in plane strain compression at 950 °C (1740 °F) and 10/s in two steps to a total strain of 0.9 ( Ref 3 )
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