Oscillating welding method

Information

  • Patent Grant
  • 10286490
  • Patent Number
    10,286,490
  • Date Filed
    Friday, February 21, 2014
    10 years ago
  • Date Issued
    Tuesday, May 14, 2019
    5 years ago
Abstract
A method is provided for welding a substrate, in which an energy source and/or a material feed is or are moved in an oscillating motion over the surface of the substrate. The oscillating movement in a vertical and/or horizontal direction during welding results in smaller grains, which prevent the formation of fractures during welding.
Description
CROSS-REFERENCE TO RELATED APPLICATIONS

This application claims priority to PCT Application No. PCT/EP2014/053389, having a filing date of Feb. 21, 2014, based off of DE Application No. 102014200834.4 having a filing date of Jan. 17, 2014, the entire contents of which are hereby incorporated by reference.


FIELD OF TECHNOLOGY

The following relates to a welding method in which the welding beam is moved in oscillation.


BACKGROUND

During the laser deposition welding of nickel-based superalloys having a high proportion of metallic phase γ′, hot cracks can already form during solidification of the melt. By reducing the beam diameter of the laser with a circular intensity distribution, smaller grains are achieved and solidification cracks can be avoided, but this reduces the rate of deposition of the material.


SUMMARY

An aspect relates to a welding method which makes it possible to achieve small grains and high deposition rates.


An oscillating motion in the horizontal direction should cause the solidification front to change constantly so as to produce an oscillating solidification form. As a result of a constantly changing solidification function, the grain growth is interrupted during the solidification of the melt and the microstructure solidifies in fine-grained form. The fine-grained quality of the microstructure causes the welding residual stresses which thus remain to be distributed over the grain boundaries so as to avoid cracks in the weld seam or in the weld metal.


The welding method can be remelting or deposition welding. Both methods produce a melt and a solidification front.





BRIEF DESCRIPTION

Some of the embodiments will be described in detail, with reference to the following figures, wherein like designations denote like members, wherein:



FIG. 1 shows an arrangement for welding; and



FIGS. 2-4 show the sequence of the oscillating motion.





DETAILED DESCRIPTION

The figures and the description represent only exemplary embodiments of the invention.



FIG. 1 shows a device 1 for a welding method, in particular a laser welding method, on the basis of which embodiments of the invention will be explained in a non-limiting manner.


The method is thus not limited to laser welding methods, but is also applicable for electron beam welding methods and other plasma welding methods with corresponding energy sources.


Material 8 is deposited onto a substrate 3, which, in the case of turbine blades or vanes, is a nickel-based or cobalt-based superalloy having a high γ′ proportion and therefore generally an alloy having poor weldability.


A welding bead 6, as part of the deposition weld, has already been generated.


In the case of a remelt method, the welding bead is the remelted region.


At those points where a laser, as an exemplary energy source 13, directs the laser beams 15 (FIG. 2) thereof onto the substrate 3, there is a melt pool 7.


A powder nozzle, as the material feed 14, preferably feeds powder 8, with the powder 8 being melted, in this case by laser radiation 15. The material 8 is fed in the form of powder, but may also be fed as a wire. This laser radiation 15 is in particular pulsed.


The area to be welded is made up of a plurality of welding beads lying next to one another and if appropriate one above another and preferably has, in at least one direction, a length of greater than or equal to 4 mm.



FIGS. 2, 3 and 4 show the for example triangular 44; 31, 34; 43, 49, 55 oscillating motion of the laser radiation 15.


The oscillating motion is preferably affected only in one plane.


The triangular shape 44; 31, 34; 43, 49, 55 is preferably an acute-angled triangle, with a height (in the direction of movement 2) of the triangular shape 44 preferably being at least twice the magnitude of the base 24.


An oscillating motion preferably proceeds as follows:


From a first starting point 21 (FIG. 2), the laser radiation 15 moves counter to the direction of movement 2 at an angle with respect to the direction of movement 2 as far as a first deflection point 22, where the laser radiation 15 is then moved perpendicularly with respect to the direction of movement 2 in a direction 24 as far as a second deflection point 23.


In order that the laser radiation 15 continues to move along as a whole in the direction of movement 2, it then moves obliquely with respect to the direction of movement 2 in the direction of movement 2 in a first oblique direction 30 (FIG. 3) to a second starting point 31, which lies downstream of the first deflection point 22 in the direction of movement 2. The second starting point 31 is level with the first deflection point 22, displaced by a distance 4.


From there, the laser radiation 15 then moves forward again as far as a third deflection point 33. The third deflection point 33 lies downstream of the first starting point 21 in the direction of movement 2. A connecting line between points 21, 33 is parallel to the direction of movement 2. From there, the laser radiation 15 oscillates again at an angle with respect to the direction of movement 2 counter to the direction of movement 2 as far as a fourth deflection point 34.


The fourth deflection point 34 is level with the second starting point 31 in a perpendicular direction with respect to the direction of movement 2 and level with the second deflection point 23 in the direction of movement 2.


In a second perpendicular direction of movement 36 which is perpendicular with respect to the direction of movement 2, the laser radiation 15 moves back to the second starting point 31 of the triangular oscillating motion (FIG. 3).


The further triangular oscillating motion proceeding from FIG. 3 can then be identified in FIG. 4, in which the laser radiation 15 oscillates in a second oblique direction 40 with respect to the direction of movement 2 in the direction of movement 2 to the seventh deflection point 55. The seventh deflection point 55 is level with the point 34. From there, the laser radiation 15 then moves in the direction of the third deflection point 33 to a fifth deflection point 43, which lies downstream of the deflection point 33 as shown in FIG. 3.


From the fifth deflection point 43, the laser radiation 15 moves obliquely with respect to the direction of movement 2 counter to the direction of movement 2 in a third rearward motion 46 as far as a sixth deflection point 49. From the sixth deflection point 49, the laser radiation 15 oscillates perpendicularly with respect to the direction of movement 2 to the seventh deflection point 55.


Effectively, a triangular shape is always displaced in the direction of movement 2 for the course of the laser radiation 15, such that the triangular shapes overlap.


This represents only one procedure for the preferably triangular oscillation.


On account of embodiments of the invention, this procedure achieves improved material properties.


Although the present embodiments of has been disclosed in the form of preferred embodiments and variations thereon, it will be understood that numerous additional modifications and variations could be made thereto without departing from the scope of the invention.


For the sake of clarity, it is to be understood that the use of ‘a’ or ‘an’ throughout this application does not exclude a plurality, and ‘comprising’ does not exclude other steps or elements.

Claims
  • 1. A method for welding a substrate, comprising the following step: providing an energy source and a material feed;moving at least one of the energy source and the material feed in an oscillating motion with respect to a surface of the substrate, wherein the oscillating motion occurs at least once at least partially in a triangular shape with respect to the surface; andemitting energy and material with respect to the surface of a substrate, during the oscillating motion, thereby producing a weld on the surface of the substrate.
  • 2. The method as claimed in claim 1, in which remelt welding takes place.
  • 3. The method as claimed in claim 1, in which deposition welding takes place.
  • 4. The method as claimed in claim 1, in which the energy source is moved in an oscillating motion at least once in a triangular shape with respect to the surface.
  • 5. The method as claimed in claim 1, in which the energy source and the material feed are moved in an oscillating motion at least once at least partially in a triangular shape with respect to the surface.
  • 6. The method as claimed in claim 1, in which the energy source and the material feed are moved in an oscillating motion at least once in a triangular shape with respect to the surface.
  • 7. The method as claimed in claim 1, in which laser radiation is used as the energy source.
  • 8. The method as claimed in claim 1, in which powder is fed via the material feed.
  • 9. The method as claimed in claim 1, in which nickel-based or cobalt-based superalloys are used as the substrate.
  • 10. The method as claimed in claim 1, in which use is made of a welding nozzle, which has the material feed wherein the material feed is a powder feed, and generation and supply of the energy wherein the energy is laser radiation.
  • 11. The method as claimed in claim 1, in which the oscillating deflection is up to 2 mm.
  • 12. The method as claimed in claim 1, in which the welded area is ≥4 mm in at least one orientation.
  • 13. The method as claimed in claim 1, in which the energy source and/or material feed are moved repeatedly perpendicularly, with respect to the direction of movement.
  • 14. The method as claimed in claim 1, in which the oscillating motion is effected only two-dimensionally.
Priority Claims (1)
Number Date Country Kind
10 2014 200 834 Jan 2014 DE national
PCT Information
Filing Document Filing Date Country Kind
PCT/EP2014/053389 2/21/2014 WO 00
Publishing Document Publishing Date Country Kind
WO2015/106833 7/23/2015 WO A
US Referenced Citations (16)
Number Name Date Kind
4562332 Walter Dec 1985 A
4814575 Petitbon Mar 1989 A
4832981 Yamazaki May 1989 A
4832982 Mori et al. May 1989 A
6054192 Otsuka et al. Apr 2000 A
20060255019 Martukanitz Nov 2006 A1
20110073636 Arjakine et al. Mar 2011 A1
20110089150 Arjakine Apr 2011 A1
20110248001 Kawanaka Oct 2011 A1
20120267347 Arjakine Oct 2012 A1
20130216836 Grebe Aug 2013 A1
20130232749 Bruck Sep 2013 A1
20140197139 Burbaum Jul 2014 A1
20140291304 Mudd, II Oct 2014 A1
20150298258 Arjakine Oct 2015 A1
20160288263 Arjakine Oct 2016 A1
Foreign Referenced Citations (13)
Number Date Country
101052495 Oct 2007 CN
102112266 Jun 2011 CN
10217200 Oct 2003 DE
0856393 Aug 1998 EP
2311597 Apr 2011 EP
2005-088078 Apr 2005 JP
2007-296580 Nov 2007 JP
2008194730 Aug 2008 JP
20050023271 Mar 2005 KR
2006116722 Nov 2006 WO
WO2006116722 Nov 2006 WO
2009143909 Dec 2009 WO
WO2009143909 Dec 2009 WO
Non-Patent Literature Citations (8)
Entry
Machine translation of Japan Patent document No. 2005-088,078, Mar. 2018.
Machine translation of Japan Patent document No. 2007-296,580, Mar. 2018.
Korean Office Action for Korean Application No. 10-2016-7018857, dated Jan. 3, 2018.
English Translation of Chinese Office Action for CN Application No. 201480073421.5, dated Jan. 17, 2017.
Application No. PCT/EP2014/053389, International Search Report dated Nov. 20, 2014.
Application No. DE 10217200 Al, Search Report dated Jan. 17, 2014.
International Search Report PCT/EP2014/053389; Filing Date: Feb. 21, 2014; 2 pgs.
Non-English European Exam Report for Application No. 14 707 705.1 dated Nov. 8, 2018.
Related Publications (1)
Number Date Country
20160318124 A1 Nov 2016 US