Electric heating – Metal heating – By arc
Reexamination Certificate
2002-08-16
2004-02-03
Paschall, Mark (Department: 3742)
Electric heating
Metal heating
By arc
C219S121470, C219S076160, C219S121520, C315S111510, C427S446000, C427S569000
Reexamination Certificate
active
06686555
ABSTRACT:
This application claims the priority of German Application No. 101 40 298.8-34, filed Aug. 16, 2001, the disclosure of which is expressly incorporated by reference herein.
BACKGROUND AND SUMMARY OF THE INVENTION
The invention relates to a method for plasma jet welding.
In recent years, a variety of efforts have been undertaken to particularly increase and refine the performance capacity of conventional plasma jet welding processes, such as tungsten inert gas welding (TIG) or active-gas metal arc welding (MAG).
In TIG welding, an electric arc burns between a non-melting tungsten electrode and the subject, so that the subject is melted open. The electric arc has an angle of divergence of about 45°. This means that the distance between the TIG welding torch and the subject significantly affects the power density, which on the whole is relatively low. Due to the high heat conductivity of the metals, a substantial portion of the heat escapes into the area surrounding the weld seam. A power level that is limited by the life of the electrode and the resulting limited electric arc output leads to relatively slow welding speeds.
The plasma beam can be restricted in various plasma jet welding processes by means of water-cooled expansion jets. This can reduce electric arc divergence to about 10° (visual). As a result, a higher power density and, at identical electric arc power, a resulting faster welding speed can be achieved when working with technically conventional distances between the plasma welding torch and the subject. In addition, the more stable and less divergent plasma beam, as compared with the conventional TIG process, reduces the impact of the welding parameters on the shape of the electric arc.
If significantly more energy is applied to the electric arc by increasing the intensity of current, given a suitable array of electrodes, the so-called plug effect is achieved. If the subject is of the appropriate thickness, it is melted open in a perforated manner and, when the plasma welding torch is continuously advanced, the molten metal flows around the plasma beam and back together behind it.
A disadvantage of the method described above is that the possible intensity of current, and therefore the welding speed, is limited by the life of the electrodes. This results in high thermal stress on the component and broad thermal impact zones, as well as considerable lag in the subject.
The technical options for further increasing welding speed have been essentially exhausted. In addition to the resulting economic consequences, this means that in the future it will not be possible to substantially lower the limits currently reached in terms of section energy, lag, and the adverse effects on properties of a relatively broad thermal impact zone. This is especially disadvantageous in that the inherent potential of modern, high-strength materials, whose properties can only be attained with specific thermal treatments, are largely underutilized at the current level of development of conventional welding methods.
Another disadvantage of conventional plasma jet welding methods lies in the limited accessibility of and opportunity to observe the welding site, due to the relatively large jet diameter and the small distance from the subject (about 5 mm).
The object of the invention is to provide a new method for plasma jet welding in which the disadvantages of the state of the art are avoided.
According to the invention, a free radio frequency- rf-)induced plasma beam is used, which is generated during a hybrid welding torch process by using the following steps:
generation of a stationary high-pressure plasma, referred to in the following as pilot plasma, by igniting a first process gas with a pilot plasma welding torch;
introduction of the pilot plasma into an rf-transparent working tube including a gas inflow and a gas outflow opening, with the working tube being wrapped in a coupling coil;
introduction of a second process gas into the rf-transparent tube at a pressure of p≧1 bar, with the second process gas being introduced into the tube in such a way that it exhibits a tangential flow component in the tube;
generation of an rf-plasma in the rf-transparent tube by electrode-free ignition of the gas mixture comprising the pilot plasma and the second process gas; and
generation of a plasma beam by introduction of the rf plasma into a working space through a metal expansion jet arranged at the gas outflow opening of the tube.
In this process, the ignition of the gas mixture takes place especially by absorption of electromagnetic radiation in the radio frequency range. However, it is also possible to ignite the gas mixture by absorption of electromagnetic radiation in the microwave range. The incorporation of the radio frequency energy into the gas mixture is accomplished inductively by means of the coupling coil wrapped around the rf-transparent tube. The coupling coil can be configured in such a way so as to ensure optimal incorporation of the electromagnetic energy into the gas mixture.
The pilot plasma can advantageously be generated in a peak current arc discharge or in an electrode-free microwave discharge.
Through the pilot plasma, an already ionized gas is introduced into the rf-transparent tube, where the ionized gas is mixed with the second process gas. As a result of the interaction between the electromagnetic radiation, which is coupled into the tube through coupling coil, and the ionized gas, the ignition threshold for ignition of the gas mixture from the pilot plasma gas and the second process gas is reduced. As a result, an energy-rich plasma is generated into which virtually the entire radio frequency energy can be incorporated.
The rf-transparent tube is advantageously a tube with dielectric properties. In particular, a tube made of SiO
2
or Al
2
O
3
, both in pure form and without dopant, is used as the rf-transparent tube.
Especially advantageous plasma properties result from the plasma jet welding method of the invention. For example, the specific enthalpy of the rf plasma and the related enthalpy flow density of the rf plasma are increased. Consequently, the plasma temperature of the rf plasma and of the plasma beam is also increased. This leads to advantages over the plasma jet welding methods known in the art with respect to increased welding speed and lower weld seam costs. Thus, the plasma jet welding method of the invention provides a welding method that offers considerable economic and application-related advantages while at the same allowing for a wide range of application for the welding method.
The properties of the plasma beam are also improved in terms of reduced diameter and reduced beam angle divergence. In addition, the cylindrically symmetrical plasma beam expands in parallel form in the method of the invention, which reduces the effects of changing the distance between the welding torch and the subject on the fusion shape of the plasma beam in the subject. Another advantage is the improved accessibility to the plasma beam, because it allows for a greater possible distance between the welding torch and the subject. Consequently, distances of 30 mm to 100 mm between the welding torch and the subject, at a plasma beam diameter of 1 mm to 3 mm on the subject, can be achieved with the method of the invention. Thus, power densities above 1.5×10
5
W/cm
2
can be generated.
The tangential introduction of the second process gas supports the generation, according to the invention, of a plasma beam with a small beam angle divergence. Due to the radial acceleration caused by the tangential introduction of the second process gas, which is further amplified by the cross-sectional narrowing of the expansion jet in the direction of the jet opening, the unevenly accelerated free charged particles move on increasingly narrow spiral paths in the direction of the expansion jet opening, which causes the centripetal acceleration of the charged particles to increase. The charged particles retain this movement, even after exiting the expansion jet and entering the workin
Bayer Erwin
Laure Stefan
Steinwandel Jürgen
Crowell & Moring LLP
MTU Aero Engines GmbH
Paschall Mark
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