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Book Chapter

By Thomas W. Eagar
Series: ASM Handbook
Volume: 6
Publisher: ASM International
Published: 01 January 1993
DOI: 10.31399/asm.hb.v06.a0001332
EISBN: 978-1-62708-173-3
... Abstract Welding and joining processes are essential for the development of virtually every manufactured product. This article discusses the fundamentals of fusion welding processes, with an emphasis on the underlying scientific principles. It reviews the role of energy-source intensity...
Series: ASM Handbook Archive
Volume: 10
Publisher: ASM International
Published: 01 January 1986
DOI: 10.31399/asm.hb.v10.a0001762
EISBN: 978-1-62708-178-8
..., in principle, a data set can be obtained by using a fixed wavelength and scanning θ (angle dispersive) or by fixing θ and scanning the wavelength (energy dispersive). Most instruments scan θ; however, new radiation sources for x-rays and neutrons composed of a broad spectrum of high-intensity wavelengths...
Book Chapter

By Paul B. Farnsworth
Series: ASM Handbook Archive
Volume: 10
Publisher: ASM International
Published: 01 January 1986
DOI: 10.31399/asm.hb.v10.a0001728
EISBN: 978-1-62708-178-8
... Abstract This article discusses the general principles, optical systems, and emission sources of optical emission spectroscopy for elemental analysis. Changes in the energy of the valence or outer shell electrons result in the atomic lines used in emission spectroscopy. Each possible...
Book Chapter

By Thomas W. Eagar, Aaron D. Mazzeo
Series: ASM Handbook
Volume: 6A
Publisher: ASM International
Published: 31 October 2011
DOI: 10.31399/asm.hb.v06a.a0005577
EISBN: 978-1-62708-174-0
... of practical heat intensities used for fusion welding. It contains tables that present information on the thermal diffusivities of common elements and alloys from 20 to 100 °C. energy-source intensity fusion welding steel surface power density thermal diffusivity WELDING AND JOINING processes...
Book Chapter

By Tanjore V. Jayaraman
Series: ASM Handbook
Volume: 17
Publisher: ASM International
Published: 01 August 2018
DOI: 10.31399/asm.hb.v17.a0006448
EISBN: 978-1-62708-190-0
... MeV. Therefore, in addition to producing radiation that is more penetrating, high-energy sources produce a greater intensity of useful radiation for a given amount of electrical energy consumed. Fig. 9 Effect of tube voltage or electron energy on the efficiency of energy conversion...
Book Chapter

By S. Lampman
Series: ASM Handbook
Volume: 10
Publisher: ASM International
Published: 15 December 2019
DOI: 10.31399/asm.hb.v10.a0006645
EISBN: 978-1-62708-213-6
... as wave, then the proper meaning of the intensity of electromagnetic radiation is the energy per unit area per unit time. If the radiation is being described as particle interaction, then the intensity refers to the number of counts per unit time from the detector. X-rays occur from various sources...
Series: ASM Handbook
Volume: 6A
Publisher: ASM International
Published: 31 October 2011
DOI: 10.31399/asm.hb.v06a.a0005603
EISBN: 978-1-62708-174-0
... electrical resistance is also common for welding of thin material. However, fusion welding using internal joule heating, that is, resistance welding, does not involve the use of a direct heat source. The intensity or energy distribution associated with the direct heat sources may vary dramatically...
Book Chapter

By Arne Bengtson
Series: ASM Handbook
Volume: 10
Publisher: ASM International
Published: 15 December 2019
DOI: 10.31399/asm.hb.v10.a0006640
EISBN: 978-1-62708-213-6
...-lying excited states almost always produce the most intense emission. The higher the energy of such transitions, the hotter the source required for efficient excitation. The denominator on the right side of Eq 3 is the partition function for the species. The value of the partition function increases...
Book Chapter

Series: ASM Desk Editions
Publisher: ASM International
Published: 01 December 1998
DOI: 10.31399/asm.hb.mhde2.a0003238
EISBN: 978-1-62708-199-3
... are shorter and there are no extra costs for x-ray film and processing. Field inspection of thick sections is a time-consuming process. Portable x-ray sources generally emit relatively low-energy radiation, up to approximately 400 keV, and also are limited as to the intensity of radiation output...
Series: ASM Handbook
Volume: 24
Publisher: ASM International
Published: 15 June 2020
DOI: 10.31399/asm.hb.v24.a0006545
EISBN: 978-1-62708-290-7
... energy source to generate melt pool widths on the order of the laser spot size, typically ranging from hundreds of micrometers to several millimeters. E-beams are similar to lasers in that they also provide high intensities over a small spot size but add the additional capability of very rapid, magnetic...
Book Chapter

By Donald E. Leyden
Series: ASM Handbook Archive
Volume: 10
Publisher: ASM International
Published: 01 January 1986
DOI: 10.31399/asm.hb.v10.a0001733
EISBN: 978-1-62708-178-8
... found wide application in elemental identification and determination. The technique depends on the emission of characteristic x-radiation, usually in the 1 - to 60-keV energy range, following excitation of atomic electron energy levels by an external energy source, such as an electron beam, a charged...
Book Chapter

By K.H. Eckelmeyer
Series: ASM Desk Editions
Publisher: ASM International
Published: 01 December 1998
DOI: 10.31399/asm.hb.mhde2.a0003250
EISBN: 978-1-62708-199-3
... and the intensities of the various characteristic energies Qualitative analysis (determination of which elements are present) is done by comparing the energies of the x-rays emitted from the sample with the known characteristic x-ray spectra of each element ( Fig. 3 ). Quantitative determination...
Series: ASM Handbook Archive
Volume: 10
Publisher: ASM International
Published: 01 January 1986
DOI: 10.31399/asm.hb.v10.a0001768
EISBN: 978-1-62708-178-8
... volume in an iron target with a beam energy of 20 keV. Source: Ref 7 Most of the energy imparted to the specimen is in the form of heat. However, a small but important fraction of the interactions ionizes the inner shells of the target atoms. The ionized atoms emit x-rays and Auger electrons...
Book Chapter

By Binayak Panda
Series: ASM Handbook
Volume: 10
Publisher: ASM International
Published: 15 December 2019
DOI: 10.31399/asm.hb.v10.a0006639
EISBN: 978-1-62708-213-6
... compared with other common microanalytical techniques that use electron and ion excitation sources. Polymers and plastics can be analyzed because the binding energies of saturated and unsaturated bonds in atoms can be separated. Extremely thin layers, including materials with layered structures, can...
Series: ASM Handbook
Volume: 17
Publisher: ASM International
Published: 01 August 2018
DOI: 10.31399/asm.hb.v17.a0006459
EISBN: 978-1-62708-190-0
... for an x-ray source. A cobalt-60 source with an activity of 3700 GBq (100 Ci) generates 60,000 photons per second per square millimeter at 1 m with energies of 1.1 and 1.3 MeV. After passing through a 100 mm (4 in.) thick steel specimen, the radiation is attenuated in intensity by a factor of 15. Therefore...
Image
Published: 15 December 2019
Fig. 3 Chart of principal Auger electron energies. Data points indicate the electron energies of the principal Auger peaks from each element. Larger data points represent the most intense peaks for each element. Source: Ref 1 . Courtesy of Physical Electronics, USA More
Image
Published: 31 October 2011
Fig. 5 Schematic illustrations of the three basic ways in which electrical energy, supplied by a power source, can be used to heat and fusion weld a metal, including (a) use of the kinetic energy of electrons and positive ions in an arc to bombard the workpiece and produce heat (in arc welding More
Book Chapter

By Linda B. McGown
Series: ASM Handbook Archive
Volume: 10
Publisher: ASM International
Published: 01 January 1986
DOI: 10.31399/asm.hb.v10.a0001732
EISBN: 978-1-62708-178-8
... of broad bands, resulting in a high degree of spectral overlap. Source: Ref 1 Quantitative Analysis The fluorescence emission intensity I F for a particular species is directly proportional to its molar concentration, c, according to: (Eq 10) I F = I 0 k Φ F ϵ b c...
Book Chapter

By J.B. Lumsden
Series: ASM Handbook Archive
Volume: 10
Publisher: ASM International
Published: 01 January 1986
DOI: 10.31399/asm.hb.v10.a0001771
EISBN: 978-1-62708-178-8
... be used for compound identification. Fig. 8 The iron 2 p 3/2 spectrum showing a model calculation of the deconvolution into component lines whose intensity and energy were rationalized on the basis of multiplet splitting. CG, center of gravity. Source: Ref 14 Shake-up Satellites When...
Image
Published: 01 January 1986
Fig. 8 Plot of all the x-ray lines in the energy range from 1 to 10 keV observed in practical EDS. The escape peak associated with the highest intensity line in each family is also plotted. The approximate peak width (FWHM) produced at each keV unit of energy across the spectrum is plotted More