Laser beam cutting of thick steel

Author(s):  
G. Sepold ◽  
R. Rothe
Keyword(s):  
2000 ◽  
Author(s):  
Takehiro Watanabe ◽  
Hiroyuki Kobayashi ◽  
Keiji Suzuki ◽  
Seiji Beppu

1993 ◽  
Vol 9 (04) ◽  
pp. 236-244
Author(s):  
Nick Eutizzi ◽  
P. E. Denney

The method most commonly used for cutting thick [1.90 cm (0.75 in.)] steel where edge quality is of no concern is flame cutting by oxyacetylene torch. This method provides the energy to heat the steel beyond its melting point, and gas pressure forces the molten material (dross) through the thickness of the material. Cutting torches typically remove a kerf of approximately 0.63 to 1.27 cm (0.25 to 0.5 in.). Gas cutting is noisy, generates large quantities of smoke into the environment and forms large pieces of dross which can travel up to 3.04 m (10 ft) and cause fires. Typically, when flame cutting shipboard, a fire watch is required. Also, if any type of flammable material exists on the opposite side of the cut, it must be removed for several inches on both sides of the cut line to preclude backside combustion. A search for a better method of cutting thick steel sections, including those with coating materials attached, centered around a high-powered CO2 laser. The CO2 laser had successfully demonstrated its ability to weld heavy sections of steel with 100% penetration from one side and create a very narrow heat-affected zone. It was decided to expand this welding process to cutting by introducing high-pressure assist gases. The gas would force the molten puddle created by the focused laser beam through the steel material, thereby creating a cut through the material as opposed to allowing the molten material to fuse back together without the assist gases (creating a welded joint). It was decided to take advantage of the laser's high-powered density to cut/vaporize non-metallic material attached to the steel plate. Also, there was interest in the effects of a laser beam on asbestos material.


Author(s):  
Susumu Shono ◽  
Osa Matsumoto ◽  
Seiji Beppu ◽  
Shunichi Sato ◽  
Hideaki Saito ◽  
...  
Keyword(s):  
Co Laser ◽  

Author(s):  
David W. Piston ◽  
Brian D. Bennett ◽  
Robert G. Summers

Two-photon excitation microscopy (TPEM) provides attractive advantages over confocal microscopy for three-dimensionally resolved fluorescence imaging and photochemistry. Two-photon excitation arises from the simultaneous absorption of two photons in a single quantitized event whose probability is proportional to the square of the instantaneous intensity. For example, two red photons can cause the transition to an excited electronic state normally reached by absorption in the ultraviolet. In practice, two-photon excitation is made possible by the very high local instantaneous intensity provided by a combination of diffraction-limited focusing of a single laser beam in the microscope and the temporal concentration of 100 femtosecond pulses generated by a mode-locked laser. Resultant peak excitation intensities are 106 times greater than the CW intensities used in confocal microscopy, but the pulse duty cycle of 10-5 maintains the average input power on the order of 10 mW, only slightly greater than the power normally used in confocal microscopy.


Author(s):  
Jean-Paul Revel

The last few years have been marked by a series of remarkable developments in microscopy. Perhaps the most amazing of these is the growth of microscopies which use devices where the place of the lens has been taken by probes, which record information about the sample and display it in a spatial from the point of view of the context. From the point of view of the biologist one of the most promising of these microscopies without lenses is the scanned force microscope, aka atomic force microscope.This instrument was invented by Binnig, Quate and Gerber and is a close relative of the scanning tunneling microscope. Today's AFMs consist of a cantilever which bears a sharp point at its end. Often this is a silicon nitride pyramid, but there are many variations, the object of which is to make the tip sharper. A laser beam is directed at the back of the cantilever and is reflected into a split, or quadrant photodiode.


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