It utilizes an impurity in a host material as the active medium. Thus, the neodymium ion (Nd+++) is used as a ‘dopant’, or purposely added impurity in either a glass or YAG crystal and the 1.06 μm output wavelength is dictated by the neodymium ion. The lasing material or the host is in the form of a cylinder of about 150 mm long and 9 mm in diameter. Both ends of the cylinder are made flat and parallel to very close tolerances, then polished to a good optical finish and silvered to make a reflective surface. The crystal is excited by means of an intense krypton or xenon lamp. A simplified schematic arrangement of the rod, lamp and mirrors is as shown in Fig.
The electric discharge style CO2 gas lasers are the most efficient type currently available for high power laser beam material processing. These lasers employ gas mixtures primarily containing nitrogen and helium along with a small percentage of carbon dioxide, and an electric glow discharge is used to pump this laser medium (i.e., to excite the CO2 molecule). Gas heating produced in this fashion is controlled by continuously circulating the gas mixture through the optical cavity area and thus CO2 lasers are usually categorized according to the type of gas flow system they employ; slow axial, fast axial or transverse.
Slow Axial Flow Gas Laser
They are the simplest of the CO2 gas lasers. Gas flow is in the same direction as the laser resonator’s optical axis and electric excitation field, or gas discharge path. These are capable of generating laser beams with a continuous power rating of approximately 80 watts for every meter of discharge length. A folded tube configuration is used for achieving output power levels of 50 to 1000 watts, maximum.
Fast Axial Flow (FAF) Gas Laser:
They have similar arrangement of components as that of slow axial flow gas laser, except that in the case of the FAF Laser, a roots blower or turbo pump is used to circulate the laser gas at high speed through the discharge region and corresponding heat exchangers. The FAF lasers with continuous wave (CW) output power levels of between 500 to 6000 watts are available
LBW Process Advantages
1) Heat input is close to the minimum required to fuse the weld metal, thus heat affected zones are reduced and workpiece distortions are minimized.
2) Time for welding thick sections is reduced and the need for filler wires and elaborate joint preparations is eliminated by employing the single pass laser welding procedures.
3) No electrodes are required; welding is performed with freedom from electrode contamination, indentation or damage from high resistance welding currents.
4) LBM being a non-contact process, distortions are minimized and tool wears are eliminated.
5) Welding in areas that are not easily accessible with other means of welding can be done by LBM, since the beams can be focused, aligned and directed by optical elements.
6) Laser beam can be focused on a small area, permitting the joining of small, closely spaced components with tiny welds.
7) Wide variety of materials including various combinations can be welded.
8) Thin welds on small diameter wires are less susceptible to burn back than is the case with arc welding.
9) Metals with dissimilar physical properties, such as electric resistance can also be welded.
10) No vacuum or X-Ray shielding is required.
11) Laser welds are not influenced by magnetic fields, as in arc and electron beam welds. They also tend to follow weld joint through to the root of the work-piece, even when the beam and joint are not perfectly aligned.
12) Aspect ratios (i.e., depth-to-width ratios) of the order of 10:1 are attainable in LBM