Optical and thermal effects of air trap on cylindrical laser treatment of tubular stenosis

2022 ◽  
Author(s):  
Seonghee Lim ◽  
Van Gia Truong ◽  
HyunWook Kang
Keyword(s):  
Laser Treatment ◽  
Thermal Effects

X-ray analysis of mechanical and thermal effects induced by femtosecond laser treatment of aluminum single crystals

2006 ◽  
Vol 252 (13) ◽  
pp. 4691-4695 ◽  
Author(s):  
S. Valette ◽  
R. Le Harzic ◽  
E. Audouard ◽  
N. Huot ◽  
R. Fillit ◽  
...  
Keyword(s):  
Femtosecond Laser ◽  
Single Crystals ◽  
Laser Treatment ◽  
Thermal Effects ◽  
X Ray

Influence of Thermal Effects Produced by Laser Treatment on the Tribological Behavior of Porcelain Ceramic Tiles

2009 ◽  
Vol 423 ◽  
pp. 41-46 ◽  
Author(s):  
F. Gutiérrez Mora ◽  
Arturo Domínguez-Rodríguez ◽  
V.V. Lennikov ◽  
G.F. de la Fuente
Keyword(s):  
Experimental Data ◽  
Wear Rate ◽  
Laser Treatment ◽  
Thermal Effects ◽  
Tribological Behavior ◽  
Fracture Propagation ◽  
Ceramic Tiles ◽  
Severe Wear

Commercial porcelain ceramic tiles have been irradiated with a laser to evaluate the thermal effects on their surface and in their tribological behavior. Different irradiation patterns were followed, varying the density of points where the laser was focused, from 25 to 150 dots per inch. Hardness and toughness were evaluated using Vickers indentations. Tribological behavior was studied using a ball-on-flat apparatus with alumina balls. An increase in the wear rate was observed in the higher irradiated samples, which can be correlated to a decrease in their toughness. A mechanism of severe wear by fracture propagation and material pullout is proposed to explain the experimental data and the observed corresponding microstucture.

Thermal Considerations in Lens Regulator Systems

1970 ◽  
Vol 28 ◽  
pp. 358-359
Author(s):  
K.C. Newton
Keyword(s):  
Electron Microscope ◽  
Thermal Effects ◽  
Environmental Control ◽  
Reference Networks ◽  
Better Than

Thermal effects in lens regulator systems have become a major problem with the extension of electron microscope resolution capabilities below 5 Angstrom units. Larger columns with immersion lenses and increased accelerating potentials have made solutions more difficult by increasing the power being handled. Environmental control, component choice, and wiring design provide answers, however. Figure 1 indicates with broken lines where thermal problems develop in regulator systemsExtensive environmental control is required in the sampling and reference networks. In each case, stability better than I ppm/min. is required. Components with thermal coefficients satisfactory for these applications without environmental control are either not available or priced prohibitively.

Direct measurement of electron-diffraction-pattern intensities using an energy loss spectrometer

1989 ◽  
Vol 47 ◽  
pp. 668-669
Author(s):  
A. G. Jackson ◽  
M. Rowe
Keyword(s):  
Thermal Effects ◽  
Dynamic Range ◽  
Scattering Amplitude ◽  
Dynamical Theory ◽  
Site Symmetry ◽  
Proof Of Concept ◽  
Parallel Acquisition ◽  
Kinematic Approximation ◽  
Speed Up ◽  
Structure Calculations

Diffraction intensities from intermetallic compounds are, in the kinematic approximation, proportional to the scattering amplitude from the element doing the scattering. More detailed calculations have shown that site symmetry and occupation by various atom species also affects the intensity in a diffracted beam. [1] Hence, by measuring the intensities of beams, or their ratios, the occupancy can be estimated. Measurement of the intensity values also allows structure calculations to be made to determine the spatial distribution of the potentials doing the scattering. Thermal effects are also present as a background contribution. Inelastic effects such as loss or absorption/excitation complicate the intensity behavior, and dynamical theory is required to estimate the intensity value.The dynamic range of currents in diffracted beams can be 104or 105:1. Hence, detection of such information requires a means for collecting the intensity over a signal-to-noise range beyond that obtainable with a single film plate, which has a S/N of about 103:1. Although such a collection system is not available currently, a simple system consisting of instrumentation on an existing STEM can be used as a proof of concept which has a S/N of about 255:1, limited by the 8 bit pixel attributes used in the electronics. Use of 24 bit pixel attributes would easily allowthe desired noise range to be attained in the processing instrumentation. The S/N of the scintillator used by the photoelectron sensor is about 106 to 1, well beyond the S/N goal. The trade-off that must be made is the time for acquiring the signal, since the pattern can be obtained in seconds using film plates, compared to 10 to 20 minutes for a pattern to be acquired using the digital scan. Parallel acquisition would, of course, speed up this process immensely.

Laser treatment of multiple glomangiomas: progress report 13 years after treatment

1981 ◽  
Vol 117 (8) ◽  
pp. 451a-452 ◽  
Author(s):  
L. Goldman
Keyword(s):  
Laser Treatment ◽  
Progress Report

Q-switched ruby laser treatment of congenital nevi

1995 ◽  
Vol 131 (5) ◽  
pp. 621-623 ◽  
Author(s):  
D. J. Goldberg
Keyword(s):  
Laser Treatment ◽  
Ruby Laser

Identification of a new type of laser treatment (KM treatment) of diamonds

2001 ◽  
Vol 25 (5) ◽  
pp. 259-263 ◽  
Author(s):  
Y. Horikawa
Keyword(s):  
Laser Treatment ◽  
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