The United States Government has rights in this invention pursuant to Contract No. W-7405-ENG-48 between the United States Department of Energy and the University of California for the operation of Lawrence Livermore National Laboratory.

BACKGROUND OF THE INVENTION Field of the Invention The present invention relates to laser shock processing, and more specifically, it relates to techniques for contouring metal by laser peening.

Description of Related Art Using high power lasers to improve material properties is one of the most important industrial applications of lasers. Lasers can transmit controllable beams of high-energy radiation for metalworking. Primarily, the laser can generate a high power density that is localized and controllable over a small area. This allows for cost effective and efficient energy utilization, minimizes distortions in surrounding areas, and simplifies material handling. Since the laser pulse involves the application of high power in short time intervals, the process is adaptable to high-speed manufacturing. The fact that the beam can be controlled allows parts having complex shapes to be processed. Also accuracy, consistency, and repeatability are inherent to the system.

Improving the strength of metals by cold working undoubtedly was discovered early in civilization, as ancient man hammered out his weapons and tools. Since the 1950s, shot peening has been used as a means to improve the

fatigue properties of metals. Another method of shock processing involves the use of high explosive materials in contact with the metal surface.

The use of high intensity laser outputs for the generation of mechanical shock waves to treat the surfaces of metals has been well known since the 1970s.

The laser shock process can be used to generate compressive stresses in the metal surfaces, adding strength and resistance to corrosive failure.

Lasers with pulse outputs of 10 to 100 J and pulse durations of 10 to 100 ns are useful for generating inertially confined plasmas on the surfaces of metals. These plasmas create pressures in the range of 10,000 to 100,000 atmospheres and the resulting shock pressure can exceed the elastic limit of the metal and thus compressively stress a surface layer as deep or deeper than 1 mm in the metals. Lasers are now becoming available with average power outputs meaningful for use of the technique at a rate appropriate for industrial production.

In the process of laser shock processing, a metal surface to be treated is painted or otherwise made"black"that is, highly absorbing of the laser light.

The black layer both acts as an absorber of the laser energy and protects the surface of the part from laser ablation and from melting due to the high temperature of the plasma. A thin layer of water, typically 1 to 2 mm, is flowed over this black surface. The water acts to inertially confine or, as it is called, tamp the plasma generated as the laser energy is absorbed in the short time pulse duration, typically 30 ns. Other suitable materials that act as a tamper are also possible. A limitation to the usefulness of the process is the ability to deliver the laser energy to the metal surface in a spatially uniform beam. If not uniform, the highest intensity area of the light can cause a breakdown in the water which blocks delivery of meaningful energy to the painted metal surface. A conventional technique to deliver the laser light to the surface is to use a simple lens to condense the laser output to a power density of roughly 100 J to 200 J per

square centimeter. This condensing technique has the limitation that a true "image"of the laser near-field intensity profile is not obtained at the surface.

Rather a field intensity representing something between the near and far fields is generated. Diffraction of the laser beam as it is focused down onto the surface results in very strong spatial modulation and hot spots.

Any phase aberrations generated within the beam, especially those associated with operation of the laser for high average power, can propagate to generate higher intensity areas within the beam. These high peak intensity regions cause breakdown in the water layer, preventing efficient delivery of the laser energy to the surface to be treated. Another potential cause of breakdown in the tamping material is the generation of non-linear effects such as optical breakdown and stimulated scattering. In a normal generation of a 10 ns to 100 ns pulse within a laser, the output slowly builds over a time period exceeding several pulsewidths. This slow, weak intensity helps to seed the non-linear processes that require buildup times of 10s of nanoseconds. In conventional techniques, the pulse output of the laser is"sliced"by an external means such as a fast rising electro-optical switch or by an exploding foil. These techniques can be expensive and can limit reliability.

A controlled application of compressive stress applied to one side of a metal surface will cause that surface to expand in a predictable manner and can thus curve the metal in a highly controllable fashion. Upon curving, the convex surface is left with a residual compressive stress, which is highly desirable for fatigue and corrosion resistance of the part in operation. The technique of inducing this compressive stress by means of shot peening is well known and in general use. However, shot peening is limited in the depth of intense compressive stress that can be induced without generating significant and undesirable cold working of the surface layer. Due to the required spherical shape of shot used for peening, the process imparts a non-uniform pressure

versus time profile to the metal during each individual impact of the shot.

Pressure is initiated at the first contact point of the sphere and then spreads across the impact area as the metals deform and the entire cross-section of the shot contacts the metal. This non-uniform application of pressure results in a local extrusion of the metal, a flow of metal from the center to the outer area of the impact zone. Consequently, more cold work is done on the metal as material extrudes due to the wedge of pressure created by the impact of the shot.

The forming of metals into complex shapes is required for many applications. There are a number of processes that use heat and yielding to stretch and form metal into required shapes. Especially in the aerospace industry, the application of heat and yielding strain can be detrimental to the mechanical properties of the metal and hence undesirable for many metals such as aluminum and titanium. Nonetheless, the aerospace industry needs to form complex shaped parts and achieve the forming with a high degree of precision.

Currently there are problems attaining the desired curvature without yielding in components of greater than half-inch thickness. There is also in general a lack of precise control in the parts forming such that attachment holes and the trimming to exact shape cannot be done until the formed part is brought to the component frame for final installation. Precise forming, with large curvature, especially in thick section materials, would be highly desirable.

The laser peening process as described in the parent application, can be used to shape components by creating residual compressive stress over a given surface area and allowing this stress to create strain resulting in a convex surface curvature. By systematically applying this process to both top and bottom surfaces of a piece of metal, the desired curvature for the entire piece of metal, including complex shapes such as saddle shapes can be achieved.

It would be desirable to provide a technique that achieves a greater curvature than that achieved with laser forming.

SUMMARY OF THE INVENTION It is an object of the present invention to provide a means to achieve an enhanced curvature in a part by pre-loading the component in a local area with a bending moment that results in strain that deflects the part achieving a stress that is near to but below the yielding limit.

The parent application discussed the concept of forming complex shapes in metals by means of laser shot peening. That application teaches that deformation in any desired direction can be enhanced by mechanically inducing a bending moment (although below the yield limit of the metal) in that direction during application of the laser peenforming pulses. This continuation-in-part provides a more detailed description of this enhancement. The advantage of the applied bending moment can be very significant, adding up to 50% improvement with respect to the resulting net deformation and/or curvature. A simple means to induce a bending moment is to employ a fixture consisting of a strongback on the eventual concave side and oriented along the desired arc with grips to attach to the metal on the convex side. The strongback is drilled and threaded in one or more places to accept large bolts that can be screwed through the strongback and to push against a pad in contact with the metal to be formed. Computer controlled hydraulic actuators can be used in place of screws and be more effective in rapidly and exactly applying the desired loading. The pad is contoured to spread the load along the desired arc. Loading is achieved by turning the bolt with a large wrench until achieving a deformation equivalent to the desired percentage of a yielding deformation. With the component thus loaded, laser peening is applied to the convex side along the direction of the deformed arc. As the laser peening is applied to the surface, the induced stress begins to relax the resistance to the applied load. To obtain maximum deformation the bolt is adjusted to keep the loading constant. In the case of the hydraulic load, the computer control maintains a constant load. The laser

peening pattern density and the laser intensity used depends on the material properties and desired residual curvature of the material being contoured. For complex shapes, the fixture and peening process are used along each desired arc of curvature.

BRIEF DESCRIPTION OF THE DRAWINGS Figure 1 shows a forming jig with a bolt-actuated spreader pad.

Figure 2 shows a forming jig with hydraulic control.

DETAILED DESCRIPTION OF THE INVENTION Techniques for laser peening are disclosed in co-pending U. S. Patent No. 6,198, 069, titled"Laser Beam Temporal And Spatial Tailoring For Laser Shock Processing", incorporated herein by reference. Laser technology usable in the present invention is described in U. S. Patent No. 5,285, 310 titled"High Power Regenerative Laser Amplifier,"incorporated herein by reference, and U. S. Patent No. 5,239, 408 titled"High Power, High Beam Quality Regenerative Amplifier," also incorporated herein by reference. Embodiments of laser systems usable in the present invention are described in U. S. Patent No. 5,689, 363 titled"Long Pulse Width, Narrow-Bandwidth Solid State Laser"incorporated herein by reference.

The present invention is a technique used to apply a bending moment load resulting in a deflection to components to achieve approximately 80% yield stress prior to application of a laser peening process. The bending moment is observed to result in a greater curvature than would otherwise be attained in the component after the processing when the bending moment load is removed.

This bending moment is applied by means of a fixture, called a forming jig and consisting of a strongback placed on the eventual concave side and oriented along the desired arc with grips to attach to the metal on the convex side. In one embodiment, the strongback is drilled and threaded in one or more places to accept large bolts that can be screwed through the strongback and load against a

pad placed in contact with the metal to be formed. The pad is contoured to spread the load along the desired arc. Loading is achieved by turning in the bolt with appropriate torque until achieving a deformation equivalent to approximately 80% of a yielding deformation. With the component thus loaded, laser peening is applied to the convex side along the direction of the deformed arc. As peening is applied and the metal begins to take shape, the bolt load is adjusted to keep the load near the 80% yield.

The laser peening pattern density and intensity and fluence used depends on the material properties and desired residual curvature of the material being contoured. For complex shapes, the fixture and peening process are used along each desired arc of curvature. The applied bending moment uniformly loads the component as opposed to being applied as a simple point source load. Uniform loading is achieved by employing spreader pad"at or near the desired curvature and deployed under the end of the bolt that is in contact with the metal. Uniform loading can further be achieved by employing multiple bolts with spreader pads deployed over the arc to be formed. The pre- forming can be done using a single forming jig that is moved from arc section to section or by using multiple jigs that pre-deflect the overall curvature to be achieved. Because of the large loading encountered between the bolt and the spreader pad, it is important to use materials that allow the bolt to freely turn without creating torque onto the spreader pad and result in marring of the component surface. Suitable materials for the bolt would be a 1. 5" diameter #5 cadmium plated steel bolt and the spreader pad would be a Teflon plastic pad with 1. 4" depth by 1. 6" diameter locator depression for contact with the bolt.

Use of the forming jig results in greater curvature for a given application of laser peening and thus allows for formation of sharper radii of curvature components than would otherwise be possible. Adjusting the bolt loading adds to this effect.

Figure 1 shows a forming jig with a bolt-controlled spreader pad. The jig 10 is comprised of a strongback 12 that has grips 14 and a threaded hole 16 for a bolt 18. A spreader pad 20 is in contact with the distal end of the bolt 18. As the bolt 18 is turned clockwise, the spreader pad is forced to move in the same direction of movement as the bolt 18. In operation, a component 22 to be shaped is inserted into the forming jig 10 between the spreader pad 20 and the grips 12.

As the bolt is screwed into the strongback, the component 22 to be shaped is forced by the spreader pad against the grips 12. Force is applied by the spreader pad 20 against the component until the component 22 achieves a desired <BR> <BR> curvature. Laser peening, as described, e. g. , in the parent application, is applied to the convex side 24 of the component 22. As discussed in the parent application, the step of generating laser induced compressive stress may include covering the workpiece with a layer of material that absorbs laser light. In some <BR> <BR> cases, the material may be a plastic, e. g. , a polyvinyl acetate plastic or a polyvinyl chloride plastic. Another material found useful as the laser light absorbing material is a metal foil with an adhesive backing. After this initial stage of laser peening has been applied to the convex side, further laser peening may be applied to the concave side 26 if desired.

Figure 2 shows a forming jig with a hydraulically-controlled spreader pad. The jig 110 is comprised of a strongback 112 that has grips 114 and a through hole 116 for a hydraulic piston 118. A spreader pad 120 is in contact with the distal end of the hydraulic piston 118. As the hydraulic piston 118 is actuated, the spreader pad is forced to move in the same direction of movement as the hydraulic piston 118. In operation, the hydraulic piston 118 is positioned to a minimum position such that the spreader pad is also at a minimum position.

A component 122 to be shaped is inserted into the forming jig 110 between the spreader pad 120 and the grips 114. As the hydraulic piston is actuated, the component 122 to be shaped is forced by the spreader pad against the grips 114.

Force is applied by the spreader pad 120 against the component until the component 122 achieves a desired curvature. Laser peening is applied to the convex side 124 of the component 122. Further laser peening may be applied to the concave side 126 if desired. Peening on the concave side will selectively flatten the curvature in the area peened.

The foregoing description of the invention has been presented for purposes of illustration and description and is not intended to be exhaustive or to limit the invention to the precise form disclosed. Many modifications and variations are possible in light of the above teaching. The embodiments were chosen and described to best explain the principles of the invention and its practical application to thereby enable others skilled in the art to best use the invention in various embodiments and with various modifications suited to the particular use contemplated. The scope of the invention is to be defined by the following claims.