Beam Shaping Optics for Stable Laser Welding Depth of Field

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Solution Overview

Problem

In laser-based material processing, particularly in welding, the keyhole mode is unstable due to keyhole collapse and pore/crack formation, while the conduction mode has limited penetration and large heat-affected zones, leading to distortion. Additionally, Gaussian beams provide uniform intensity but have a small depth of field, making them difficult to control and resulting in high manufacturing costs.

Innovation Solution

A beam shaping system is introduced that uses a diffractive element, such as an axicon, to transform a multimode flat-top laser beam into a Gaussian intensity distribution within the beam waist, increasing the depth of field and energy by recreating the Gaussian region adjacent to or within the waist, thereby improving the stability and quality of the weld.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Volume of moving object

If keyhole mode is used to increase weld penetration, then penetration depth is improved, but stability deteriorates due to keyhole collapse and pore/crack formation

Engineering Contradiction:
Improveweld penetration depthVSAvoidwelding process stability
Core Design Contradiction:
Volume of moving objectVSReliability

Solution Approach 1:

The patent changes the beam intensity distribution parameter from Gaussian to flat-top profile. This parameter change allows the system to operate in a stable conduction mode while achieving sufficient penetration, eliminating keyhole collapse issues. The flat-top profile distributes energy more uniformly across the beam cross-section, preventing localized overheating and keyhole instability.

Inventive Principle:
Principle #35Parameter changes

2Reliability

If conduction mode is used to improve stability, then welding stability is improved, but penetration depth deteriorates due to low power density

Engineering Contradiction:
Improvewelding process stabilityVSAvoidweld penetration depth
Core Design Contradiction:
ReliabilityVSVolume of moving object

Solution Approach 1:

The patent modifies the beam intensity distribution parameter to flat-top profile, which redistributes power density uniformly across the beam cross-section. This allows conduction mode operation to achieve adequate penetration depth while maintaining stability, as the uniform energy distribution prevents localized vaporization and enables controlled melting throughout the weld zone.

Inventive Principle:
Principle #35Parameter changes

Solution Approach 2:

The patent transitions from point-focused energy delivery (Gaussian beam) to area-distributed energy delivery (flat-top beam). This dimensional change in energy distribution allows the entire beam cross-section to contribute effectively to weld penetration, achieving deep penetration in conduction mode without relying on a concentrated keyhole.

Inventive Principle:
Principle #17Another dimension (Dimensionality change)

3Volume of moving object

If conduction mode is used to achieve desired weld penetration, then penetration depth is improved, but heat-affected zone size increases causing distortion

Engineering Contradiction:
Improveweld penetration depthVSAvoidheat-affected zone size
Core Design Contradiction:
Volume of moving objectVSArea of stationary object

Solution Approach 1:

The flat-top beam profile changes the thermal distribution parameter, creating a more uniform temperature field in the weld zone. This uniform heating reduces thermal gradients and minimizes the heat-affected zone extent, thereby reducing distortion while achieving adequate penetration depth through efficient energy utilization across the entire beam cross-section.

Inventive Principle:
Principle #35Parameter changes

4Illumination intensity

If Gaussian beam is used to provide uniform intensity distribution, then intensity uniformity is improved, but depth of field deteriorates making control difficult

Engineering Contradiction:
Improveintensity distribution uniformityVSAvoiddepth of field
Core Design Contradiction:
Illumination intensityVSLength of stationary object

Solution Approach 1:

The patent inverts the conventional approach by using a flat-top beam profile instead of Gaussian. This inversion of the intensity distribution profile fundamentally changes the beam propagation characteristics, creating a longer depth of field while maintaining useful intensity distribution for welding applications.

Inventive Principle:
Principle #13The other way round (Inversion)

Applied Scientific Principles

This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.

Function Achieved in This Case

This configuration enhances the depth of field and energy distribution, reducing the impact of robotic errors and workpiece uniformity issues, leading to improved weld quality and reduced damage to non-uniform workpieces, while maintaining high manufacturing precision.

Implementation Method 1

A beam shaping system is introduced that uses a diffractive element, such as an axicon, to transform a multimode flat-top laser beam into a Gaussian intensity distribution within the beam waist

Methodology Applied
Scientific EffectDiffraction: Diffraction

Data Source

PatentUS20230364706A1Beam shaping system in the process of laser welding
Publication Date: 2023.11.16 IPG PHOTONICS CORP
  • US20230364706A1 patent drawing
  • US20230364706A1 patent drawing
  • US20230364706A1 patent drawing

AI summary

A beam-shaper for transforming a MM beam with the flattop intensity distribution profile includes an end block which is fused to a downstream end of a fiber outputting the MM beam along a path within a laser head. The beam-shaper further has a collimator mounted to the laser head downstream from the end block. The collimated MM beam is then focused on the working zone with a beam waist characterized by a Gaussian intensity profile. The Gaussian region may be provided in the vicinity of the beam waist by positioning the collimator so that the Gaussian region of the MM flattop beam is located inside the end block and in the focal plane of the collimator. Alternatively, the Gaussian region may be provided within the waist by using a diffractive optical element which transforms the flattop distribution profile into a donut-shaped profile.