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Series: ASM Handbook
Volume: 2A
Publisher: ASM International
Published: 30 November 2018
DOI: 10.31399/asm.hb.v02a.a0006502
EISBN: 978-1-62708-207-5
... modes of laser welding: conduction-mode welding and deep-penetration mode welding. The article reviews the factors of process selection and procedure development for laser welding. The factors include power density, interaction time, laser beam power, laser beam diameter, laser beam spatial distribution...
Series: ASM Handbook
Volume: 6A
Publisher: ASM International
Published: 31 October 2011
DOI: 10.31399/asm.hb.v06a.a0005641
EISBN: 978-1-62708-174-0
... information on independent process variables such as incident laser beam power and diameter, laser beam spatial distribution, traverse speed, shielding gas, depth of focus and focal position, weld design, and gap size. Dependent variables, including depth of penetration, microstructure and mechanical...
Series: ASM Handbook
Volume: 6
Publisher: ASM International
Published: 01 January 1993
DOI: 10.31399/asm.hb.v06.a0001445
EISBN: 978-1-62708-173-3
... it is the power density that determines the depth of penetration and joining rate for the process, not the total power of the source. Therefore, beam diameter and spatial distribution of the laser-beam energy play an extremely important role because they determine the area of incidence. Two other variables...
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
... for defining the spatial distribution of energy as a Gaussian function, it is appropriate to use the radius that provides an area under the distribution equal to 1−(1/e 3 ). However, for laser beam welding, the beam radius representing the usable energy is often reported as 1−(1/e 2 ), which represents 86.5...
Series: ASM Handbook
Volume: 6
Publisher: ASM International
Published: 01 January 1993
DOI: 10.31399/asm.hb.v06.a0001481
EISBN: 978-1-62708-173-3
... of strength Q on the surface. The applicability of point sources to characterize energy input for laser-beam welding processes will be explored later in this article. Equation 1 describes the heat-input distribution from a stationary arc. Only the magnitude of the heat input, the distribution...
Series: ASM Handbook
Volume: 24A
Publisher: ASM International
Published: 30 June 2023
DOI: 10.31399/asm.hb.v24A.a0006976
EISBN: 978-1-62708-439-0
... manufacturing. CPU, central processing unit In discrete laser models, the path of the laser beam is still temporally and spatially resolved, and for lumped laser models, the laser beam is enlarged to speed up deposition. This method is also the most widely accessible approach and is typically available...
Series: ASM Handbook
Volume: 24
Publisher: ASM International
Published: 15 June 2020
DOI: 10.31399/asm.hb.v24.a0006564
EISBN: 978-1-62708-290-7
... Abstract This article covers in-line process monitoring of the metal additive manufacturing (AM) methods of laser and electron beam (e-beam) powder-bed fusion (PBF) and directed-energy deposition (DED). It focuses on methods that monitor the component directly throughout the build process...
Series: ASM Handbook
Volume: 23
Publisher: ASM International
Published: 01 June 2012
DOI: 10.31399/asm.hb.v23.a0005685
EISBN: 978-1-62708-198-6
... (<10 −7 Pa, or 1 × 10 −9 torr). Typical applications for AES include: Microscopic particle identification Passive oxide film thickness on metal components Thin films of contamination on components Quantification of light-element surface films Mapping spatial distribution...
Series: ASM Handbook
Volume: 24A
Publisher: ASM International
Published: 30 June 2023
DOI: 10.31399/asm.hb.v24A.a0006951
EISBN: 978-1-62708-439-0
... Abstract This article provides an introduction to architected cellular materials, their design, fabrication, and application domain. It discusses design decisions involving the selection, sizing, and spatial distribution of the unit cell, property-scaling relationships, and the integration...
Series: ASM Handbook
Volume: 5
Publisher: ASM International
Published: 01 January 1994
DOI: 10.31399/asm.hb.v05.a0001294
EISBN: 978-1-62708-170-2
... is sharply peaked with respect to the target normal, with some tilting of the distribution toward the incident laser beam. Early studies on the PLD of multicomponent films indicated that the spatial distribution of deposited material was also accompanied by a spatial variation in film composition. In thermal...
Series: ASM Handbook
Volume: 24
Publisher: ASM International
Published: 15 June 2020
DOI: 10.31399/asm.hb.v24.a0006546
EISBN: 978-1-62708-290-7
... power of the laser per unit area, H ( x , y , z ). As the laser scans a line, radiant power is distributed over a finite area, because beams are not infinitesimal. Assuming that the laser scans along the x -axis, while the z -axis is oriented perpendicular to the resin surface and into the resin...
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
... is known as the 1/ e 2 beam width. In Gaussian beams, the intensity distribution is preserved as the beam travels through space. That is, if a beam is Gaussian at the output of a laser, it should remain Gaussian as it propagates through space and simple optics. This property simplifies optical...
Series: ASM Handbook
Volume: 24A
Publisher: ASM International
Published: 30 June 2023
DOI: 10.31399/asm.hb.v24A.a0006994
EISBN: 978-1-62708-439-0
... are a collection of random variables with a joint Gaussian distribution with a mean value of zero or adjusted to a mean of zero. This allows the covariance parameter to be tweaked as a smoothing kernel. Therefore, the covariance between each distinct parameter is reflected in the spatial distance between any two...
Series: ASM Handbook
Volume: 2A
Publisher: ASM International
Published: 30 November 2018
DOI: 10.31399/asm.hb.v02a.a0006532
EISBN: 978-1-62708-207-5
... in continuous wave (CW) mode and pulse mode. The spatial mode profile of the beam is characterized by transverse electromagnetic (TEM) mode ( Ref 19 ). There are various spatial modes that differ due to different resonator design. The Gaussian power distribution with fundamental TEM 00 (the subscripts denote...
Series: ASM Handbook
Volume: 24A
Publisher: ASM International
Published: 30 June 2023
DOI: 10.31399/asm.hb.v24A.a0006977
EISBN: 978-1-62708-439-0
... conventional manufacturing process for bulk-scale materials. In the case of fusion AM processes (electron beam melting, or EBM; selective laser melting, or SLM; and directed-energy deposition, or DED), this richness arises from the process-specific thermal conditions associated with the liquid-to-solid phase...
Series: ASM Handbook Archive
Volume: 10
Publisher: ASM International
Published: 01 January 1986
DOI: 10.31399/asm.hb.v10.a0001774
EISBN: 978-1-62708-178-8
.... A situation that can be most detrimental to depth resolution is shown in Fig. 12(b) . This crater-edge effect is the result of nonuniform erosion of the specimen caused by nonuniform distribution of ions in the primary beam. The detection system will simultaneously filter and count secondary ions over...
Series: ASM Handbook
Volume: 6A
Publisher: ASM International
Published: 31 October 2011
DOI: 10.31399/asm.hb.v06a.a0005627
EISBN: 978-1-62708-174-0
... in the past ( Ref 12 , Ref 13 , 14 ). These diagnostics are on par with diagnostics used for measuring power density distributions in continuous-wave laser beams and allow the two processes to be quantitatively compared. The number of electron beam welders appears to be approaching a steady-state value...
Series: ASM Handbook
Volume: 17
Publisher: ASM International
Published: 01 August 2018
DOI: 10.31399/asm.hb.v17.a0006456
EISBN: 978-1-62708-190-0
... demonstrated with a number of different types of energy beams, such as ultrasound, electrons, protons, α-particles, lasers, and microwaves. In industrial nondestructive evaluations (NDEs), however, only x-ray computed tomography (XCT) is considered to have widespread value. For this reason, XCT is also...
Series: ASM Handbook
Volume: 11A
Publisher: ASM International
Published: 30 August 2021
DOI: 10.31399/asm.hb.v11A.a0006838
EISBN: 978-1-62708-329-4
... level of compatibility with the laser beam itself. Powder characterization (sizing, morphology, distribution) is a critical consideration not only in the synthesis phase of design but also in the analysis of failures ( Ref 11 – 15 ). Design also may be limited by various AM manufacturing constraints...
Series: ASM Handbook
Volume: 10
Publisher: ASM International
Published: 15 December 2019
DOI: 10.31399/asm.hb.v10.a0006683
EISBN: 978-1-62708-213-6
... caused by nonuniform distribution of ions in the primary beam. The detection system simultaneously filters and counts secondary ions over a range of depths in the sample, and depth resolution is severely degraded. The practical consequence of this in the measured depth profile is a gross broadening...