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Like a beam of high velocity electrons, a laser beam is also capable of producing very high power density. Laser is a highly coherent (in space and time) beam of electromagnetic radiation with wavelength varying operation from 0.1 – 0.7µm. However, the power requirement for machining operation restricts the effectively usable wavelength range to 0.4 – 0.6µm. Because of the fact that the rays of a laser beam area perfectly parallel and monochromatic, it can be focused to a very small diameter and can produce a power density as high as 107w/mm2. For developing a high power, normally a pulsed ruby laser is used. The continuous CO2-N2 laser has also been successfully used in machining operations. Fig. 15-6 shows a typical pulsed ruby laser. A coiled xenon flash tube is placed around the ruby rod and the internal surface of the container walls is made highly reflecting so that maximum light falls on the ruby rod for the pumping operation. The capacitor is charged and a very high voltage is applied to the triggering electrode for initiation of the flash. The emitted laser beam is focused by a lens system and the focused beam meets the work surface, removing a small portion of the material by vaporization and high speed ablation. A very small fraction of the molten metal is vaporized so quickly that a substantial mechanical impulse is generated, throwing out a large portion of the liquid metal. Since the energy released by the flash tube is much more than the energy emitted by the laser head in the form of a laser beam, the system must be properly cooled.