The subject of this present invention is a method of bending metal objects, such as plates, bars, etc., along straight lines. By this method it is possible to bend objects with constant and varying thickness, and also objects made of brittle materials and of materials with high hardness.
The hitherto known methods of bending objects of such type, being made of metals, involve the plastic deformation of the material of the object being bent by applying external forces appropriate as to size and direction. The bending is effected by means of the bending machines, bending dies and bending presses adapted to that purpose, frequently very powerful.
Elastic compressive and tensile stresses appear in the material bent and they cause the shape to be changed after the operation of the force has ceased. This affects the accuracy of the intended deformation and makes it difficult to control that process.
In addition to the above these stresses cause a decrease in the service life of the bent objects during their operation. The known methods cannot be used for bending brittle as well as high-strength and high-hardness materials.
The purpose of this present invention has been to develop a method of changing the curvature of metal objects, in the way that would not require the application of heavy equipment and, simultaneously, should make it possible to apply a controlled bending precess with a high accuracy of deformation.
The essence of this present invention involves subjecting the objects to the repetitive, two-phase process of heating and cooling the material along a selected line.
In the first phase, the material is subjected to heating with a concentrated stream of energy causing a thermal effect. The heating either takes place simultaneously along the entire line, or the stream of energy is moving along the line at a predetermined speed.
Consequently, the material is locally plasticised and partially melted in the region of the heating line.
The local nature of the action of the stream of energy together with the heating speed cause the material undergo plastic deformation in that region due to the phenomenon of thermal expansion. The heating mentioned is conducted in such a way that the zone of the material in which the deformation occurs reaches a depth smaller than the thickness of the object.
Next, during the second phase, the object is cooled at ambient temperature or, additionally, in a stream of blown gas, so as to reach the condition in which the material ceases to be plastic throughout the entire region. During cooling the previously deformed zone of the material becomes shorter along the fibres perpendicular to the heating lines due to the thermal shrinkage of the material. Since the shrinking fibres of the material form the zone which does not cover the entire thickness of the object, the object bends at an angle along the line of the original heating.
By repeating the above-mentioned operation many times, the object is given the required curvature.
It is recommended that the heating and cooling process take place under a protective gas atmosphere for the purpose of eliminating the harmful effect of air on the heated area. It is advantageous to carry out the heating process by means of a layer of a substance increasing the coefficient of absorption of the stream of energy.
A high-power laser or electron beam is used as the source of energy.
The method as per this present invention makes it possible to bend metal objects without the need of employing external forces. By this method, the curvature of objects can be changed from a distance under the conditions in which the access to that object is impossible. Besides, the same method allows bending of objects made of brittle and high-hardness materials, for which the previously known methods could not be employed.
Brief Description of the Drawing
In the accompanying drawings, in which are shown serveral of the various possible embodiments of the present invention:
FIG. 1a shows a view of a schematic diagram illustrating the plastic stresses Re versus temperature T and the maximum elongation A versus temperature T,
FIG. 1b shows a view of a schematic diagram illustrating a simplified model of the plastic stresses Re versus temperature T,
FIG. 2a shows a side view of plate being bent,
FIG. 2b shows a front elevetational view of the embodiment of FIG. 2a,
FIG. 3 shows a perspective view of a plate being bent,
FIG. 4 shows a sectional view of a heating phase of the plate to be bent,
FIG. 5 shows a schematic diagram illustrating the bending process of the embodiment of FIG. 4,
FIG. 6 shows a diagram of a temperature distribution versus depth of a plate during a bending procedure,
FIG. 7 shows a diagram of plotting stresses versus the depth of the plate during the bending process,
FIG. 8 shows a schematic diagram of a section perpendicular to the plate with a distribution of isotherms illustrating a temperature distribution during bending,
FIG. 9a shows a schematic diagram similar to the diagram of FIG. 8 of a section perpendicular to the plate with a distribution of isotherms illustrating a temperature distribution during bending together with a plot of the temperature during bending versus depth location,
FIG. 9b shows a schematic diagram illustrating an isotherm distribution at a cooling stage shown in FIG. 5,
FIG. 10 shows a diagram illustrating a stress distribution within a bent plate,
FIG. 11a is a perspective view of the bending plate showing the process of bending wherein the energy stream SE is moving along the bending line with the velocity V,
FIG. 11b is a sectional view of the bending plate of FIG. 11a along the section line B--B,
FIG. 12a shows a diagram of a circular sector with the dimensions for being bend to a cone sector,
FIG. 12b shows a diagram of the cone sector, which diagram is derived from the circular sector as shown in FIG. 12a.
FIG. 13 shows a schematic diagram illustrating the plastic stresses Re versus temperature T and the maximum elongation A versus temperature T.
During the first phase, the material of the object being bent is subject to heating with concentrated stream of energy SE of of laser radiation. Application of the stream of energy SE of laser radiation, moving at speed V along the bending line AA entails a local change in the condition of the material characterised by different properties at depth G.
Within that region, two zones can be observed, the material being liquid in the first zone S1 and plasticised in the second zone S2, with the boundary of the area encompassing the melting and plasticising zones shown with the line U.
The temperature distribution of the heated material, as shown schematically in FIG. 5 as a function of thickness L of the object indicates additionally the material melting temperature T.sub.m. In the heating stage the material of the first, S1, and the second, S2, zones, flows out to occupy an increased volume as a result of the stresses caused by the effect of thermal expansion. This temperature distribution related to melting temperature T.sub.m determines the size of the first, S1, and the second, S2, zones relative to material thickness L.
During the second phase the material is cooled at ambient temperature or, additionally, in the stream of a blown gas. The material within the region of the bending line, i.e. the liquid in first zone S1 and the plasticised material in the second zone, S2, is transformed into solid state. The boundary of the region encompassing the plasticising and melting zone in the heating phase has been marked with line U in FIG. 4.
Due to internal stresses .sigma..sub.t caused by the shrinkage of the cooled material, it becomes shorter along the fibres marked with arrow, which is shown through the stress distribution along the thickness L of the object in FIG. 6.
In this diagram, the values of limit compression .sigma..sub.s and of limit tensile stress .sigma..sub.r are marked. Should the limit tensile stress, .sigma..sub.r, for example, be exceeded, the brittle materials may crack.
The heating and cooling conditions are selected so that the tensile and compressive stresses created in the material should be much smaller than are their limit stresses.
By changing the heating and cooling parameters, such as the stream movement speed, the stream power, the absence or presence, and nature of a layer absorbing the stream of energy, etc., one may affect the temperature distribution in the heating phase [FIG. 5] and the stress distribution in the cooling phase [FIG. 6].
In the above-mentioned manner, control is exercised on the magnitude of the stresses created in the material in order to obtain the desired angle .delta. of bending [FIGS. 1 and 4] during one cycle of heating and cooling along the bending line. In one of the possible embodiments, a flat parallel slab shown in FIGS. 1 and 2 has been subjected to a process of bending according to this present invention. The slab, 0.7 mm thick and 20 mm wide, is made of 50 HSA steel and heated with a radiation beam of a continuously operating 300 W CO.sub.2 laser, the source of energy moving along line AA [FIG. 2] at the speed of 2.5 cm/sec. The beam is directed perpendicularly to the surface of the slab.
The heating takes place under a protective argon atmosphere. The slab was cooled in the ambient atmosphere within about 1 second. With such conditions of the method employed and after a single heating and cooling cycle, the slab was bent at the angle of 2.8.degree..
The method of bending objects according to this present invention, can be used for shaping objects of brittle or high-strength materials. Besides, this method can be employed for shaping objects when access to them is difficult, e.g. under vacuum or under hazardous conditions [high tension, harmful radiation, etc.].