1-20 of 180

Search Results for incident laser beam power

Follow your search
Access your saved searches in your account

Would you like to receive an alert when new items match your search?
Close Modal
Sort by
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
... variables for laser welding include incident laser-beam power, incident laser-beam diameter, traverse speed, absorptivity, shielding gas, depth of focus and focal position, and weld design and gap size. The important dependent variables are depth of penetration, microstructure and mechanical properties...
Series: ASM Handbook
Volume: 6
Publisher: ASM International
Published: 01 January 1993
DOI: 10.31399/asm.hb.v06.a0001370
EISBN: 978-1-62708-173-3
... beam power Incident laser beam diameter Absorptivity Traverse speed of the laser beam across the substrate surface Parameters such as weld design, shielding gas, gap size for butt welds, and depth of focus with respect to the substrate also play important roles. These parameters...
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
... is the selection of optimum independent and dependent processes. The independent process variables for laser welding include incident laser beam power, incident laser beam diameter, traverse speed, absorptivity, shielding gas, depth of focus and focal position, and weld design and gap size. The important dependent...
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
... materials such as copper and gold. It is currently unclear if powers of hundreds of watts will be possible with commercial green laser systems. Fig. 7 Optical reflection coefficient of titanium as a function of wavelength, assuming normal incidence. Based on data from Ref 38 , 39 In terms...
Series: ASM Handbook
Volume: 6
Publisher: ASM International
Published: 01 January 1993
DOI: 10.31399/asm.hb.v06.a0001398
EISBN: 978-1-62708-173-3
... configurations of production lasers were of the “blind” (no feedback) type. The system included a laser programmed for power, as well as length of heat injection time. The focal spot of the laser beam was brought to impinge on the target by moving either the target itself or the laser beam, or a combination...
Series: ASM Handbook
Volume: 6A
Publisher: ASM International
Published: 31 October 2011
DOI: 10.31399/asm.hb.v06a.a0005618
EISBN: 978-1-62708-174-0
..., and radiative heat transfer. The resulting accumulation of heat energy raises the temperature of the workpiece material so as to melt and even vaporize it. In the case of laser cutting, the torch consists of a highly focused laser light beam that reaches power densities on the workpiece of more than 100 times...
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
... region have high average beam power, better beam quality, and efficiency. They are good for cutting thicker sections (>10 mm, or 0.4 in.) with high speed. The Nd:YAG laser is more suitable in the pulse mode, in which it gives high power that allows the fine cutting of metals at thicknesses...
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
... welding electrons focused beam diameter high energy density electron welding keyhole-mode welding laser beam welding photons power density boundary HIGH ENERGY DENSITY BEAM WELDING refers to electron or laser processes where a beam of electrons or photons, respectively, can be focused to power...
Series: ASM Handbook
Volume: 17
Publisher: ASM International
Published: 01 August 2018
DOI: 10.31399/asm.hb.v17.a0006471
EISBN: 978-1-62708-190-0
...). It is important to match impedances when selecting a search unit for a particular instrument. Both the ultrasound energy transmitted into the material being inspected (radiated power) and beam divergence are directly related to the size (active area) of the transducer element. Thus, it sometimes is advisable...
Series: ASM Handbook
Volume: 6A
Publisher: ASM International
Published: 31 October 2011
DOI: 10.31399/asm.hb.v06a.a0005631
EISBN: 978-1-62708-174-0
... welding of tube and pipe. Wire Joints The joint configurations for wires shown in Fig. 2 were developed by the electronics industry. For wire-to-wire joints, the two wires must share the incident laser energy. In a cross joint, for example, the laser beam should be directed at the intersection...
Series: ASM Handbook
Volume: 13A
Publisher: ASM International
Published: 01 January 2003
DOI: 10.31399/asm.hb.v13a.a0003681
EISBN: 978-1-62708-182-5
... to promote corrosion resistance. surface composition ion implantation rapid melt quenching corrosion resistance energy beams high-power laser melting surface modification SURFACE MODIFICATION, in the context of this article, is the alteration of surface composition or structure by the use...
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
.... The attenuation of the laser beam in the vertical direction has been accounted for ( Ref 26 ) by calculating the temperature at a depth, d , below the surface. If the temperature at depth, d , exceeds the boiling point of the material, then point d is deemed to be transparent. The incident power...
Series: ASM Handbook
Volume: 24A
Publisher: ASM International
Published: 30 June 2023
DOI: 10.31399/asm.hb.v24A.a0006955
EISBN: 978-1-62708-439-0
... . Sample images are shown at Z = 22 and 26 mm (0.87 and 1.02 in.). (b) Two-dimensional Gaussian fit for a laser beam image Laser Power Control For a standard laser unit, the laser power is set by two voltage inputs: a digital input (DI) to turn the laser power on/off, and an analog input (AI...
Series: ASM Handbook
Volume: 6A
Publisher: ASM International
Published: 31 October 2011
DOI: 10.31399/asm.hb.v06a.a0005620
EISBN: 978-1-62708-174-0
... from the bottom of the roller. Incident angles of the laser beam were 45 μin. CO 2 laser and 30 μin. fiber laser, respectively. Laser Roll Welding of Dissimilar Metals Steel and Aluminum Sheet Joining Fusion welding of aluminum to steel is impractical, because brittle intermetallic compounds...
Series: ASM Handbook
Volume: 17
Publisher: ASM International
Published: 01 August 2018
DOI: 10.31399/asm.hb.v17.a0006461
EISBN: 978-1-62708-190-0
... to generate ultrasound directly on a material without the requirement for a couplant ( Ref 13 , 15 , 28 , 29 , 30 ) and can be operated in the thermal or ablative regimes ( Ref 14 ); at low incident powers, the laser heats a small region of the sample, leading to a stress wave due to thermal expansion...
Series: ASM Handbook
Volume: 13A
Publisher: ASM International
Published: 01 January 2003
DOI: 10.31399/asm.hb.v13a.a0003710
EISBN: 978-1-62708-182-5
... for these measurements. The incident beam is typically an Ar + or a Kr + laser. For SERS the choice of the laser frequency that coincides with the electronic structure of the species of interest allows for thousand-fold signal enhancement. Thus SERS becomes an advantageous technique compared to Raman spectroscopy...
Series: ASM Handbook
Volume: 21
Publisher: ASM International
Published: 01 January 2001
DOI: 10.31399/asm.hb.v21.a0003436
EISBN: 978-1-62708-195-5
... from media 1 to media 2 for a normal incidence sound beam is given by: (Eq 3) T = 4 Z 2 Z 1 / ( Z 2 + Z 1 ) 2 and (Eq 4) R = [ ( Z 2 − Z 1 ) / ( Z 2 + Z 1 ) ] 2 respectively, where Z 1 and Z 2...
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
... ( r r ′ ) 2 ] where f is the bulk energy-transfer coefficient, Q is the magnitude of the heat input per unit time ( Q being the product of the welding current and voltage for arc processes and laser power for laser beam welding), r is the distance from the center of the heat...
Series: ASM Handbook
Volume: 22B
Publisher: ASM International
Published: 01 November 2010
DOI: 10.31399/asm.hb.v22b.a0005513
EISBN: 978-1-62708-197-9
..., or a mixture thereof. For example, in laser and electron beam deposition, the incoming material can be powder or wire, which is melted by the energy of the beam. The material enters into a melt pool, which solidifies to fuse with the substrate when the beam moves away. In spray forming, a thin stream of molten...