Abstract

The plasma arc has a large arc force (regarded as the plasma force) and keyhole welding is generally performed by the formation of a small hole at the weld pool of a butt joint by making use of this plasma force. Under these circumstances, due to the small footprint area of the plasma heat source and welding by the formation of a keyhole, there is little melting at the joint zone and welding with a narrow bead width becomes feasible. Recently, a new type of plasma welding process has been proposed such that the welding tungsten electrode tip is brought close to the tip of the cooling chip and keyholeless welding is performed, similarly to TIG welding and this process has been made practicable.1 This process solves the disadvantages of keyhole welding while retaining the advantages of plasma welding and is capable of meeting the requirements of high speed welding. However, it is difficult to apply either method to fillet joints where keyhole formation is difficult due to the problems of the large plasma force and the torch structure. In either case, the large plasma force due to the plasma passing through the cooling chip small hole is surmised to be intimately associated with the weld morphology due to plasma welding.

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