CN107633115A - The Finite Element Method of multiple spot laser impact forming - Google Patents

The Finite Element Method of multiple spot laser impact forming Download PDF

Info

Publication number
CN107633115A
CN107633115A CN201710721496.5A CN201710721496A CN107633115A CN 107633115 A CN107633115 A CN 107633115A CN 201710721496 A CN201710721496 A CN 201710721496A CN 107633115 A CN107633115 A CN 107633115A
Authority
CN
China
Prior art keywords
impact
lsp
thickness direction
laser
multiple spot
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
CN201710721496.5A
Other languages
Chinese (zh)
Inventor
孙桂芳
朱然
王占栋
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Southeast University
Original Assignee
Southeast University
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Southeast University filed Critical Southeast University
Priority to CN201710721496.5A priority Critical patent/CN107633115A/en
Publication of CN107633115A publication Critical patent/CN107633115A/en
Pending legal-status Critical Current

Links

Landscapes

  • Laser Beam Processing (AREA)

Abstract

The invention discloses a kind of Finite Element Method of multiple spot laser impact forming, comprise the following steps:Multiple spot laser-impact simulation is carried out to the feature unit body with certain size first using Finite Element Simulation Software ABAQUS, obtains the total residual stress distribution σ of thickness direction diverse locationTOT;By theoretical formula σLSPTOT‑σEQ, obtain the residual stress σ as caused by inducing laser-impactLSPThickness direction is distributed;σEQFor equilibrium stress;To residual stress σ caused by laser-impact induction in MatlabLSPThickness direction distributed data is fitted, and obtains σLSPIn the fitting function of thickness direction distribution;Using user's favorite subroutine SIGINI to define primary stress field in ABAQUS, and then the part with actual analysis physical dimension is implicitly analyzed, finally obtain part shape required under specific laser-impact technological parameter effect.The present invention spends less cost to set up the relation between laser impact forming technological parameter and required part shape using the theoretical method being combined with finite element modelling.

Description

The Finite Element Method of multiple spot laser impact forming
Technical field
The present invention relates to multiple spot laser impact forming technical field, especially a kind of finite element of multiple spot laser impact forming Analogy method.
Background technology
Laser impact forming is a new laser application field, by quick quick plasticity Accurate Shaping development A kind of brand-new part forming technology come, can also be produced on part top layer while Shape Parts needed for acquisition has Certain thickness residual compressive stress.Laser impact forming is using high power density, the laser of short pulse, passes through specific light Learn element and form corresponding laser facula light beam, the light beam is irradiated on absorbed layer through the water constraint layer of flowing, and absorbed layer is inhaled Receipts laser energy occurs gasification and produces steam, and steam continues to absorb laser energy formation etc. under the restraint condition of restraint layer water Gas ions shock wave, due to the effect of restraint layer, plasma stock wave produces the stress wave propagated to inside parts, works as generation Stress exceed material dynamic yield strength when, part produce macroscopic view plastic deformation.
In order to obtain the laser impact forming part of required shape, it is necessary to be optimized to laser-impact technological parameter, so And in the complexity and shaping due to multiple spot laser impact forming mechanism many variable factors influence so that in optimize technique Very big difficulty in parameter be present.If only relying on experimental data and operating experience to determine technological parameter, will spend substantial amounts of Human and material resources and time, increase manufacturing cost.It is even more so when to the laser impact formings of heavy parts.Pass through fully profit With the forming property of material and the architectural feature of part, with reference to finite element simulation calculation, to excavate new forming process.Cause Finite element modelling is incorporated into multiple spot laser impact forming by this, and laser impact forming technological parameter is optimized.In reality In operation, due to spot size very little, the part stock size of shaping is bigger, hot spot needed for Laser Shock Forming Process Quantity is thousands of, while also needs to be refined in laser-impact area grid, and the amount of calculation of such finite element modelling will be non- Chang Ju great, limited by cost is calculated, there is an urgent need to a kind of new multiple spot laser impact forming finite element modelling side now Method.
The content of the invention
The technical problems to be solved by the invention are, there is provided a kind of finite element modelling side of multiple spot laser impact forming Method, the method being combined using theory with finite element modelling, determined within the less time needed for multiple spot laser impact forming Technological parameter, so as to spend less cost to set up between laser impact forming technological parameter and required part shape Relation.
In order to solve the above technical problems, the present invention provides a kind of Finite Element Method of multiple spot laser impact forming, bag Include following steps:
(1) more dot lasers are carried out to the feature unit body with certain size using Finite Element Simulation Software ABAQUS first Shock simulation, obtain the total residual stress distribution σ of thickness direction diverse locationTOT
(2) by theoretical formula σLSPTOTEQ, obtain the residual stress σ as caused by inducing laser-impactLSPThickness direction Distribution;σEQFor equilibrium stress;
(3) to residual stress σ caused by laser-impact induction in MatlabLSPThickness direction distributed data is fitted, Obtain σLSPIn the fitting function of thickness direction distribution;
(4) primary stress field is defined using user's favorite subroutine SIGINI in ABAQUS, and then to actual analysis The part of physical dimension is implicitly analyzed, and finally obtains part shape required under specific laser-impact technological parameter effect.
Preferably, in step (1), the simulation of multiple spot laser-impact specifically comprises the following steps:
(11) geometrical model and definition material attribute are established;
(12) Explicit Analysis is set to walk;Time of analysis step is it is ensured that kinetic energy finally levels off to 0 in each analysis step;
(13) load and grid division are applied;
(14) analysis operation and post processing are submitted;FEM calculation is completed, obtains the total remnants of thickness direction diverse location Stress distribution σTOT, wherein thickness direction is Z-direction, total residual stress distribution σTOTResidual stress including both direction, The respectively stress σ of X axisTOT,XXWith the stress σ of Y-axisTOT,YY
Preferably, in step (11), the dynamic constitutive of TC4 titanium alloys is described using such as drag;
In formula:A is yield strength, and B and n reflect the strain hardening feature of material, and C reflects strain rate to material property Influence, εpRepresent equivalent plastic strain,Representative refers to strain rate,Represent dynamic strain rate.
Preferably, in step (1), the feature unit body and actual multiple spot laser impact forming part with certain size exist Thickness direction has an identical size, and length and width dimensions are smaller than actual multiple spot laser impact forming part.
Preferably, the residual stress σ as caused by inducing laser-impact in step (2)LSPThickness direction is distributed, wherein thick Degree direction is Z-direction, σLSPThe stress σ of residual stress including both direction, respectively X axisLSP,XXWith the stress of Y-axis σLSP,YY
Beneficial effects of the present invention are:Mould is carried out to the feature unit body with smaller physical dimension first in ABAQUS Intend analysis, obtain the residual stress distribution in actual multiple spot laser impact forming part thickness direction, while multiple spot laser-impact mistake Journey numerical simulation need to only carry out Explicit Analysis, apply process for the laser impact intensified load of more hot spots, using Fortran languages The subprogram of speech editor realizes the loading of diverse location at different moments, improves efficiency, greatly reduces calculating cost;Adopt simultaneously Processing is further fitted with the Matlab residual stress data obtained to simulation, residual stress distribution function is obtained, improves The efficiency and accuracy of data analysis;Finally by by different technological parameters, (laser power density, spot radius, impact are strong Change route, strengthen number, overlapping rate, pulsewidth) obtained thickness direction residual stress distribution data as primary stress field, by with Family subprogram SIGINI is defined, to implicitly being analyzed with actual geometry large-scale part, zero of shape needed for acquisition Part, therefore this method has the characteristics of rapid, inexpensive, simple and easy to do, calculating is accurate, has preferable future in engineering applications.
Brief description of the drawings
Fig. 1 is the method flow schematic diagram of the present invention.
Fig. 2 is more laser impact forming loading area schematic diagrames of the present invention.
Fig. 3 is the final part schematic shapes that more laser impact formings of the present invention obtain.
Embodiment
As shown in figure 1, a kind of Finite Element Method of multiple spot laser impact forming, comprises the following steps:
(1) more dot lasers are carried out to the feature unit body with certain size using Finite Element Simulation Software ABAQUS first Shock simulation, obtain the total residual stress distribution σ of thickness direction diverse locationTOT
(2) by theoretical formula σLSPTOTEQ, obtain the residual stress σ as caused by inducing laser-impactLSPThickness direction Distribution;σEQFor equilibrium stress;
(3) to residual stress σ caused by laser-impact induction in MatlabLSPThickness direction distributed data is fitted, Obtain σLSPIn the fitting function of thickness direction distribution;
(4) primary stress field is defined using user's favorite subroutine SIGINI in ABAQUS, and then to actual analysis The part of physical dimension is implicitly analyzed, and finally obtains part shape required under specific laser-impact technological parameter effect.
The Finite Element Method for implementing multiple spot laser impact forming is described in detail below with reference to instantiation:
It is to carry out numerical simulation for multiple spot laser-impact feature unit body first, this process need to only be asked using Explicit Solve device.Multiple spot laser-impact numerical simulation comprises the following steps:
1.1. geometrical model and definition material attribute are established:Laser impact intensified thin-wall part actual size is 150mm* 30mm*3mm, the feature unit body physical dimension of sunykatuib analysis is 25mm*25mm*3mm, density of material 4500kg/m3, Poisson Than 0.34, modulus of elasticity 110GPa.The dynamic constitutive of TC4 titanium alloys is described using Johnson-Cook models, it is public Formula 1 is the expression formula of the model.
In formula:A is yield strength, and B and n reflect the strain hardening feature of material, and C reflects strain rate to material property Influence, εpRepresent equivalent plastic strain,Representative refers to strain rate,Represent dynamic strain rate;
1.2. Explicit Analysis is set to walk:Time of analysis step is it is ensured that kinetic energy finally levels off to 0 in each analysis step;
1.3. apply load and grid division:Loading area is used as shown in Fig. 2 shock wave peak pressure is 3.8GPa Flat top beam, circular light class, spot size 3mm, pulse width are arranged to 10ns, overlapping rate 50%, compiled using Fortran Collect subprogram and carry out more hot spot diverse locations and the application of load at different moments;It is thin that grid is carried out in Laser Shock Processing domain Change, sizing grid is 150 μm x150 μm x75 μm;
1.4. analysis operation and post processing are submitted:FEM calculation is completed, obtains the total remnants of thickness direction diverse location Stress distribution σTOT, wherein thickness direction is Z-direction, total residual stress distribution σTOTResidual stress including both direction, The respectively stress σ of X axisTOT,XXWith the stress σ of Y-axisTOT,YY
By theoretical formula σLSPTOTEQ, obtain the residual stress σ as caused by inducing laser-impactLSPThickness direction point Cloth, wherein thickness direction are Z-direction, σLSPThe stress σ of residual stress including both direction, respectively X axisLSP,XXAnd Y The stress σ of axial directionLSP,YY
To residual stress σ caused by laser-impact induction in MatlabLSPThickness direction distributed data is fitted, and is obtained To different zones σLSPIn the fitting function of thickness direction distribution, it is respectively:
When 0≤X≤50;100≤X≤150;During 0≤Z≤1.68
σLSP,XX=-208.6-376.5*cos (z*2.687)+174.1*sin (z*2.687)
-36.31*cos(2*z*2.687)+99.75*(2*z*2.687)
σLSP,YY=-188.3-361.4*cos (z*2.68)+149.1*sin (z*2.68)
-42.68*cos(2*z*2.68)+92.94*(2*z*2.68)
When 50≤X≤100;During 1.68≤Z≤3
σLSP,XX=-211+196*cos (z*2.627) -372.8*sin (z*2.627)
+27.71*cos(2*z*2.627)+104.6*(2*z*2.627)
σLSP,YY=-189.2+173.5*cos (z*2.634) -355*sin (z*2.634)
+31.82*cos(2*z*2.634)+99.06*(2*z*2.634)
Primary stress field is defined using user's favorite subroutine SIGINI in ABAQUS, and then to actual analysis geometry The part of size is implicitly analyzed, and is finally obtained under specific laser-impact technological parameter effect, required part shape, finally Part shape is as shown in Figure 3.
Although the present invention is illustrated and described with regard to preferred embodiment, it is understood by those skilled in the art that Without departing from scope defined by the claims of the present invention, variations and modifications can be carried out to the present invention.

Claims (5)

1. a kind of Finite Element Method of multiple spot laser impact forming, it is characterised in that comprise the following steps:
(1) multiple spot laser-impact is carried out to the feature unit body with certain size using Finite Element Simulation Software ABAQUS first Simulation, obtain the total residual stress distribution σ of thickness direction diverse locationTOT
(2) by theoretical formula σLSPTOTEQ, obtain the residual stress σ as caused by inducing laser-impactLSPThickness direction is distributed; σEQFor equilibrium stress;
(3) to residual stress σ caused by laser-impact induction in MatlabLSPThickness direction distributed data is fitted, and is obtained σLSPIn the fitting function of thickness direction distribution;
(4) primary stress field is defined using user's favorite subroutine SIGINI in ABAQUS, and then to actual analysis geometry The part of size is implicitly analyzed, and finally obtains part shape required under specific laser-impact technological parameter effect.
2. the Finite Element Method of multiple spot laser impact forming as claimed in claim 1, it is characterised in that in step (1), The simulation of multiple spot laser-impact specifically comprises the following steps:
(11) geometrical model and definition material attribute are established;
(12) Explicit Analysis is set to walk;Time of analysis step is it is ensured that kinetic energy finally levels off to 0 in each analysis step;
(13) load and grid division are applied;
(14) analysis operation and post processing are submitted;FEM calculation is completed, obtains the total residual stress of thickness direction diverse location It is distributed σTOT, wherein thickness direction is Z-direction, total residual stress distribution σTOTResidual stress including both direction, respectively For the stress σ of X axisTOT,XXWith the stress σ of Y-axisTOT,YY
3. the Finite Element Method of multiple spot laser impact forming as claimed in claim 2, it is characterised in that step (11) In, the dynamic constitutives of TC4 titanium alloys is described using such as drag;
<mrow> <mi>&amp;sigma;</mi> <mo>=</mo> <mrow> <mo>(</mo> <mi>A</mi> <mo>+</mo> <msubsup> <mi>B&amp;epsiv;</mi> <mi>p</mi> <mi>n</mi> </msubsup> <mo>)</mo> </mrow> <mo>&amp;lsqb;</mo> <mn>1</mn> <mo>+</mo> <mi>C</mi> <mi>L</mi> <mi>n</mi> <mrow> <mo>(</mo> <mfrac> <mover> <mi>&amp;epsiv;</mi> <mo>&amp;CenterDot;</mo> </mover> <mover> <msub> <mi>&amp;epsiv;</mi> <mn>0</mn> </msub> <mo>&amp;CenterDot;</mo> </mover> </mfrac> <mo>)</mo> </mrow> <mo>&amp;rsqb;</mo> <mo>-</mo> <mo>-</mo> <mo>-</mo> <mrow> <mo>(</mo> <mn>1</mn> <mo>)</mo> </mrow> </mrow>
In formula:A is yield strength, and B and n reflect the strain hardening feature of material, and C reflects shadow of the strain rate to material property Ring, εpRepresent equivalent plastic strain,Representative refers to strain rate,Represent dynamic strain rate.
4. the Finite Element Method of multiple spot laser impact forming as claimed in claim 1, it is characterised in that in step (1), Feature unit body with certain size and actual multiple spot laser impact forming part are in thickness direction with identical size, length and width Size is smaller than actual multiple spot laser impact forming part.
5. the Finite Element Method of multiple spot laser impact forming as claimed in claim 1, it is characterised in that in step (2) The residual stress σ as caused by inducing laser-impactLSPThickness direction is distributed, and wherein thickness direction is Z-direction, σLSPIncluding two The stress σ of the residual stress in individual direction, respectively X axisLSP,XXWith the stress σ of Y-axisLSP,YY
CN201710721496.5A 2017-08-22 2017-08-22 The Finite Element Method of multiple spot laser impact forming Pending CN107633115A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201710721496.5A CN107633115A (en) 2017-08-22 2017-08-22 The Finite Element Method of multiple spot laser impact forming

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201710721496.5A CN107633115A (en) 2017-08-22 2017-08-22 The Finite Element Method of multiple spot laser impact forming

Publications (1)

Publication Number Publication Date
CN107633115A true CN107633115A (en) 2018-01-26

Family

ID=61100583

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201710721496.5A Pending CN107633115A (en) 2017-08-22 2017-08-22 The Finite Element Method of multiple spot laser impact forming

Country Status (1)

Country Link
CN (1) CN107633115A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111310375A (en) * 2020-02-14 2020-06-19 广东工业大学 Machining method for optimizing shock wave pressure of laser double-sided simultaneous opposite impact titanium alloy blade
CN111931408A (en) * 2020-08-13 2020-11-13 广东工业大学 Finite element simulation method for laser spalling process
CN113221394A (en) * 2021-02-08 2021-08-06 西北工业大学 Simulation method for laser shot-peening forming of integral wall panel of airplane
CN114492113A (en) * 2022-01-05 2022-05-13 南京航空航天大学 Impact damage numerical simulation optimization method based on laser mapping entity grid

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5988982A (en) * 1997-09-09 1999-11-23 Lsp Technologies, Inc. Altering vibration frequencies of workpieces, such as gas turbine engine blades
CN101275177A (en) * 2007-11-30 2008-10-01 江苏大学 Anti-fatigue controlled laser shot peening method and device therefor
CN103143593A (en) * 2011-12-07 2013-06-12 江苏大学 Laser shock wave metal plate reshaping method and device
CN104866652A (en) * 2015-04-29 2015-08-26 西北工业大学 Finite element simulation method for shot-peening strengthening deformation based on ABAQUS

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5988982A (en) * 1997-09-09 1999-11-23 Lsp Technologies, Inc. Altering vibration frequencies of workpieces, such as gas turbine engine blades
CN101275177A (en) * 2007-11-30 2008-10-01 江苏大学 Anti-fatigue controlled laser shot peening method and device therefor
CN103143593A (en) * 2011-12-07 2013-06-12 江苏大学 Laser shock wave metal plate reshaping method and device
CN104866652A (en) * 2015-04-29 2015-08-26 西北工业大学 Finite element simulation method for shot-peening strengthening deformation based on ABAQUS

Non-Patent Citations (9)

* Cited by examiner, † Cited by third party
Title
A T DEWALD .ETAL: "Eigenstrain-based model for prediction of laser peeningresidual stresses in arb. Part 1 model description.pdf", 《THE JOURNAL OF STRAIN ANALYSIS FOR ENGINEERING DESIGN》 *
P. PAGLIARO .ETAL: "Measuring Multiple Residual-Stress Components using the Contour Method and Multiple Cuts", 《EXPERIMENTAL MECHANICS》 *
WILLIAM BRAISTED .ECT: "Finite element simulation of laser shock peening", 《INTERNATIONAL JOURNAL OF FATIGUE 21》 *
余天宇 等: "平顶光束激光冲击2024铝合金诱导残余应力场的模拟与实验", 《中国激光》 *
叶鸿伟: "激光喷丸强化诱导的三维残余应力场分析及其评价", 《中国优秀硕士学位论文全文数据库 信息科技辑》 *
戴毅斌 等: "多点激光微冲击成形的数值模拟研究", 《红外与激光工程》 *
朱然 等: "三维平顶光束激光冲击2024铝合金的残余应力场数值模拟", 《中国激光》 *
杨永红 等 著: "《现代飞机机翼壁板数字化喷丸成形技术》", 31 August 2012, 西北工业大学出版社 *
杨涛 等 著: "《末敏末修灵巧弹药技术与效能分析》", 31 October 2016, 国防工业出版社 *

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111310375A (en) * 2020-02-14 2020-06-19 广东工业大学 Machining method for optimizing shock wave pressure of laser double-sided simultaneous opposite impact titanium alloy blade
CN111310375B (en) * 2020-02-14 2023-05-16 广东工业大学 Processing method for optimizing laser double-sided simultaneous opposite impact titanium alloy blade shock wave pressure
CN111931408A (en) * 2020-08-13 2020-11-13 广东工业大学 Finite element simulation method for laser spalling process
CN113221394A (en) * 2021-02-08 2021-08-06 西北工业大学 Simulation method for laser shot-peening forming of integral wall panel of airplane
CN113221394B (en) * 2021-02-08 2023-03-17 西北工业大学 Simulation method for laser shot blasting forming of integral wall panel of airplane
CN114492113A (en) * 2022-01-05 2022-05-13 南京航空航天大学 Impact damage numerical simulation optimization method based on laser mapping entity grid
WO2023131035A1 (en) * 2022-01-05 2023-07-13 南京航空航天大学 Impact damage numerical simulation optimization method based on laser mapping of entity grid
CN114492113B (en) * 2022-01-05 2024-06-11 南京航空航天大学 Impact damage numerical simulation optimization method based on laser mapping solid grids

Similar Documents

Publication Publication Date Title
CN107633115A (en) The Finite Element Method of multiple spot laser impact forming
Cui et al. Large-scale sheet deformation process by electromagnetic incremental forming combined with stretch forming
CN104978456B (en) A kind of universal valve design optimization method
Psyk et al. Electromagnetic forming—a review
Qiu et al. Electromagnetic force distribution and deformation homogeneity of electromagnetic tube expansion with a new concave coil structure
Venters et al. Ducted wind turbine optimization
CN103246772A (en) ABAQUS-based finite element simulation method of correcting welding deformation through ultrasonic shot-peening
CN107217133A (en) Laser impact intensified Finite Element Method
Liu et al. Progress on design and related R&D activities for the water-cooled breeder blanket for CFETR
Yuan et al. Spectral element applications in complex nuclear reactor geometries: Tet-to-hex meshing
Kear et al. Computational aerodynamic optimisation of vertical axis wind turbine blades
CN106339541A (en) Method for analyzing fatigue strength of welding seam of tower drum door frame in large-scale wind generating set
Lin et al. Transient heat conduction analysis using the NURBS-enhanced scaled boundary finite element method and modified precise integration method
Luo et al. High-Reynolds number viscous flow computations using an unstructured-grid method
Wang et al. Laser shock micro-bulk forming: Numerical simulation and experimental research
CN107180131A (en) Method for determining the laser impact intensified thin-wall part Deformation Curvature radius of multiple spot
Lee et al. A preform design approach for uniform strain distribution in forging processes based on convolutional neural network
Zhang et al. Optimization of porthole extrusion dies with the developed algorithm based on finite volume method
CN104615812B (en) A kind of hypersonic return capsule profile Aerodynamic Heating numerical grid generation method
CN103279629A (en) Energy utilization rate numerical calculation method of laser deep melting point welding
CN113065272A (en) Method for rapidly realizing numerical simulation of welding deformation
CN103279630B (en) Laser dark fusing point weldering keyhole dynamic compaction (DC) method for numerical simulation
Huang et al. Wall vortex induced by the collapse of a near-wall cavitation bubble: Influence of the water surface
Wang et al. Study on the rotary forming process of a rim-thickened disc-like part using a local heating method
Lin et al. A particle finite element method based partitioned paradigm for the axial-flow-induced vibration analysis of NHR200-II fuel rod

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
RJ01 Rejection of invention patent application after publication

Application publication date: 20180126

RJ01 Rejection of invention patent application after publication