The present invention relates to continuous high frequency induction welding systems and more particularly to the system performance improvement by control of magnetic flux in an external area of such welding systems.
High frequency (HF) welding is the most popular technique for production of welded metallic tubes, pipes and closed profiles. According to this method HF current is applied to the edges of continuously moving preformed tube (skelp) with opening that must be closed in the process of welding. HF currents flow along the skelp edges in opposite directions on each side of the opening and heat them to or slightly below the tube metal melting temperature. Due to skin and proximity effects the heat sources are concentrated on the facing sides of the edges. Hot edges are squeezed by welding rolls in the apex point forming a continuous welding seam. The frequency in this type of welding is generally between 30 and 1000 kHz with preferred frequency range of 100-400 kHz, and two different techniques are employed.
The first technique is known as high frequency contact welding. In this technique HF current from the generator (HF welder) is supplied to the skelp through the contacts applied to the opposite edges upstream from the apex. One part of supplied current flows along the tube edges in V area (Vee) from the contacts to the apex. This part of the current heats the tube edges. Another portion of the current flows from the first contact to the second one along the inner surface of the skelp. This current known as a leakage current, causes additional losses in the tube wall. Special devices known as impeders are used to reduce this portion of the current. An impeder contains a magnetic core, a casing, a connector to attach the impeder to a holder and for accommodating cooling fluid, and, in some cases, an inlet for shielding gas.
Contact HF welding is widely used for non-closed profiles such as T or H profiles. It is used also for welding tubes, pipes and closed profiles of relatively large size, typically for tubes with diameter above 150 mm. Low life time and sensitivity to the tube surface conditions are the drawbacks of contact welding that limit their application in tube welding.
The second type of high frequency welding is known as high frequency induction welding. In high frequency induction welding, a single or multiple turn coil encircles a rolled tube or profile preform. Compared to the contact welding, the current is not supplied via contacts but induced in the skelp by the magnetic field of the inductor. All induced currents flow under the inductor around the skelp outer diameter and split into three parts when they reach the tube edges. One portion flows along the edges in Vee similar to contact welding. This is a desirable part of the current. The second portion travels from the outer circumference of the tube, across the edges of the tube cut and then along the internal tube circumference from one edge to another. This second portion of the current is similar to corresponding current in conduction welding. Losses due to this portion of the induced current are higher than in the case of conduction welding because the current flows around the tube outer surface under the coil, i.e. its path is much longer. The third portion flows along the edges in direction opposite to tube movement and then finds a close path along the internal surface of the tube from one edge to another. The third portion is only partially useful due to the edge preheating with prevailing negative effect of additional power losses on the outer and inner tube surfaces. Impeders are widely used to reduce the second and third portions of the induced current and maximize the current in Vee and therefore the system efficiency.
Existing induction welding systems do not contain any device for magnetic field control outside of the tube. Magnetic field surrounds the coil and attenuates with a distance from the coil. The part of field generated by the coil portion surrounding the tube is similar to the field of any cylindrical induction heating coil. The second part of the magnetic field, generated by the coil portion above the tube opening and by the induced current, penetrates inside the tube preform through the opening gap, flows along the impeder inside the tube preform, flows back to the outer space through the gap in Vee and returns in the surrounding space around the coil to the initial area. The magnetic field of the second part is stronger than of the first part.
The magnetic field in the external space causes several negative effects. The first effect is undesirable heating of welding rolls located in close proximity to the coil. The second effect is possible interference with the mill structure, measuring and control devices and the body of operators. The third effect is additional reactive power that requires higher current from the supplying circuit and increases losses in its components (busswork, transformer, compensating capacitor battery).
There were attempts to confine the external magnetic field and reduce field intensity in the surrounding space by applying external magnetic flux concentrators onto the induction coil. This method of magnetic flux control is widely used in induction heating, heat treating and brazing systems. Magnetic controller reduces the coil current demand and therefore reactive power, increases induced current and improves the process efficiency. However in induction welding systems, a positive effect of the external concentrator applied to the whole coil length is overcompensated by increased losses in the tube body under the coil and in the induction coil itself. In addition, it is difficult and expensive to manufacture external controllers from traditionally used in tube welding industry magnetic materials (ferrites) because of their poor mechanical properties. For these reasons, external magnetic flux concentrators are not used in the welding industry.
In spite of relatively high electrical efficiency and welding speeds reaching 1000 ft/min for tubes of small diameter, existing induction welding systems have several drawbacks. In addition to negative effects caused by external magnetic fields, heating of the tube edges is non uniform in thickness, which reduces welding speed and efficiency especially for tubes with thick wall; induction coils have high voltage and current and therefore apparent power, which must be supplied by the welder. The edge heating in Vee has limited controllability with the major part of heating power occurring at the final stage of heating, i.e. in close proximity of the apex. Any variation in length of Vee or in convergence angle can cause the welding quality variation. Finally, external magnetic field level in the work place may exceed Maximum Permissible Level and special screens may be necessary in order to meet the health standards.
In view of the foregoing, it would be desirable to provide a device or devices for magnetic field control in the external area of the welding space in order to increase the system efficiency and welding speed, improve welding quality and reduce or eliminate negative effects of the external magnetic field. It would also be desirable to provide such devices particularly suited for operating in the 100-400 kHz frequency range.
The above and other objects are provided by the magnetic bridge device of the present invention. The magnetic bridge device of the present invention provides magnetic flux control in the external area of the welding space. The magnetic bridge is a magnetic flux guide, which contains a magnetic body made from one or several plates of soft magnetic composite (magnetodielectric material) that has permeability of at least 15, preferably above 40, saturation flux density above 0.2 Telsa and service temperature of at least 180° C. Preferably, the device also comprises internal channels for water or gas cooling or one or several water-cooled plates, which are located in the middle of the magnetic body, on one side or both sides of the body. The device preferably has a fixture for its positioning above the edges of the welding tube or profile.
The magnetic bridge may be used as a separate device, in addition to the induction coil and impeders traditionally used in the induction welding systems or may be incorporated into the welding coil which provides mechanical support and cooling to the device.
Operation of the present invention, areas of applicability and provided effects will become apparent from the detailed description provided hereinafter. It should be understood that the detailed description and specific examples, while indicating the preferred embodiment of the invention, are intended for purposes of illustration only and are not intended to limit the scope of the invention.
The present invention will become more fully understood from the detailed description and the accompanying drawings, wherein:
The following description of the preferred embodiments is merely exemplary in nature and is in no way intended to limit the invention, its application, or uses.
Referring to
Cooling of the magnetic body 12 of the magnetic bridge may be performed by water, mill water or gas flowing inside the channels 11 in the body 12 as it is shown in
Referring to
In cross-section of
In the magnetic flux guide design shown in
As it is shown in
The description of the invention is merely exemplary in nature and, thus, variations that do not depart from the gist of the invention are intended to be within the scope of the invention. For example, variations in cooling methods and methods of fixturing of the magnetic bridge are not to be regarded as a departure from the spirit and scope of the invention.
This application claims the benefit of U.S. Provisional Application No. 60/934,340 filed Jun. 13, 2007.
Number | Date | Country | |
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60934340 | Jun 2007 | US |