CN107217133B - Laser impact intensified Finite Element Method - Google Patents

Laser impact intensified Finite Element Method Download PDF

Info

Publication number
CN107217133B
CN107217133B CN201710392734.2A CN201710392734A CN107217133B CN 107217133 B CN107217133 B CN 107217133B CN 201710392734 A CN201710392734 A CN 201710392734A CN 107217133 B CN107217133 B CN 107217133B
Authority
CN
China
Prior art keywords
laser
finite element
analysis
carries out
element method
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.)
Active
Application number
CN201710392734.2A
Other languages
Chinese (zh)
Other versions
CN107217133A (en
Inventor
张永康
朱然
杨青天
黄志刚
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.)
Guangdong University of Technology
Original Assignee
Guangdong University of Technology
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 Guangdong University of Technology filed Critical Guangdong University of Technology
Priority to CN201710392734.2A priority Critical patent/CN107217133B/en
Publication of CN107217133A publication Critical patent/CN107217133A/en
Application granted granted Critical
Publication of CN107217133B publication Critical patent/CN107217133B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • CCHEMISTRY; METALLURGY
    • C21METALLURGY OF IRON
    • C21DMODIFYING THE PHYSICAL STRUCTURE OF FERROUS METALS; GENERAL DEVICES FOR HEAT TREATMENT OF FERROUS OR NON-FERROUS METALS OR ALLOYS; MAKING METAL MALLEABLE, e.g. BY DECARBURISATION OR TEMPERING
    • C21D10/00Modifying the physical properties by methods other than heat treatment or deformation
    • C21D10/005Modifying the physical properties by methods other than heat treatment or deformation by laser shock processing
    • CCHEMISTRY; METALLURGY
    • C21METALLURGY OF IRON
    • C21DMODIFYING THE PHYSICAL STRUCTURE OF FERROUS METALS; GENERAL DEVICES FOR HEAT TREATMENT OF FERROUS OR NON-FERROUS METALS OR ALLOYS; MAKING METAL MALLEABLE, e.g. BY DECARBURISATION OR TEMPERING
    • C21D11/00Process control or regulation for heat treatments

Landscapes

  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Thermal Sciences (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Mechanical Engineering (AREA)
  • Materials Engineering (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • Optics & Photonics (AREA)
  • Management, Administration, Business Operations System, And Electronic Commerce (AREA)
  • Laser Beam Processing (AREA)

Abstract

The invention discloses a kind of laser impact intensified Finite Element Methods, including step:It establishes threedimensional model in ABAQUS, material property parameter is set, using Johnson Cook constitutive equations, dynamic explicit analysis step is set and so that in each analysis step inside target that plasticity variation reaches maximum value, while kinetic energy finally levels off to 0;Subprogram editor is carried out to the laser-impact time of more hot spots and position distribution, realizes the application of load;Mesh generation carries out mesh refinement in Laser Shock Processing domain;It creates analysis operation and carries out Explicit solutions, obtain residual stress field and displacement deformation distribution.Laser impact intensified Finite Element Method provided by the invention has the characteristics that rapid, inexpensive, simple and easy to do, calculating is accurate, and future in engineering applications is good.Conveniently the laser impact intensified of more hot spots can be simulated, to provide reliable basis to parameter optimization.

Description

Laser impact intensified Finite Element Method
Technical field
The present invention relates to reiforcing laser impact technology field, more specifically to a kind of laser impact intensified limited First analogy method.
Background technology
Reiforcing laser impact technology is a kind of novel material surface strengthening means, it is by high power density (GW/ cm2Magnitude), the laser beam of pulse width (ns magnitudes) by transparent restraint layer, act on the suction coated in metal targets surface Receive coating, coating material absorb laser energy gasify rapidly, formed high temperature, high pressure plasma, the plasma is by about The effect of beam layer generates metal surface the shock wave of high intensity.When the dynamic yield that the surge pressure of shock wave is more than material is strong When spending, material surface generates plastic strain, at the end of laser action, due to the reaction of shock zone material, produces inside it The raw residual compressive stress with certain depth, the presence of residual compressive stress cause the closed effect of crackle, tired to effectively reduce The driving force of labor crack propagation extends the service life of part.
Three-dimensional Flattened Gaussian Beams are a kind of laser of the light energy spatial distribution with a uniform plateau region, and impact is strong Change process is brought since complicated mechanism is influenced by a variety of variable factors simultaneously to the optimization of laser impact intensified technological parameter Very big difficulty.Only it relies on experimental data and operating experience using the method repeatedly attempted, needs to take a substantial amount of time and provide Gold.And then Finite Element Method is used to the selection of auxiliary laser shock peening technological parameter, while being answered by analyzing stress Become the variation with displacement to explain strengthening mechanism.Braisted and Brockman are used for the first time in terms of finite element modelling The method of ABAQUS/Explicit+ABAQUS/Implicit has carried out laser impact intensified simulation, and descendant also mostly uses greatly This Finite Element Method, but when for more light spot laser shock strengthenings, this method not only takes but also needs continuous The result of each hot spot Explicit Analysis is brought into implicit analysis, all analyzes and terminates until all hot spots, while for not Same technological parameter (spot radius, overlapping rate, assault route etc.), needs to establish multiple analysis model, therefore there is an urgent need to one kind Laser impact intensified carry out sunykatuib analysis of the improved Finite Element Method to more hot spots.
In conclusion the problems such as laser impact intensified parameter optimization for how efficiently solving more hot spots is difficult, is current Those skilled in the art's urgent problem.
Invention content
In view of this, first of the present invention is designed to provide a kind of laser impact intensified Finite Element Method, The laser impact intensified parameter optimization that the laser impact intensified Finite Element Method can efficiently solve more hot spots is difficult The problem of.
In order to reach above-mentioned first purpose, the present invention provides the following technical solutions:
A kind of laser impact intensified Finite Element Method, including step:
Threedimensional model is established in ABAQUS, material property parameter is set, using Johnson-Cook constitutive equations, setting Dynamic explicit analysis step simultaneously so that plasticity variation reaches maximum value inside target in each analysis step, while kinetic energy finally approaches In 0;
Subprogram editor is carried out to the laser-impact time of more hot spots and position distribution, realizes the application of load;
Mesh generation carries out mesh refinement in Laser Shock Processing domain;
It creates analysis operation and carries out Explicit solutions, obtain residual stress field and displacement deformation distribution.
Preferably, in above-mentioned Finite Element Method, it is thin to carry out grid in Laser Shock Processing domain for the mesh generation Change, specifically includes:
Laser Shock Processing domain carries out mesh refinement using cell type C3D8R, and by the boundary of laser-impact target Region is set as Infinite Element and carries out mesh generation using C3D8;
The establishment analysis operation carries out Explicit solutions, obtains residual stress field and displacement deformation distribution, specific to wrap It includes:
It creates analysis operation and generates INP files, the cell type of Infinite Element is changed to CIN3D8 in INP files, it is raw The INP files of Cheng Xin;Analysis operation is created again, while calling new INP files and subprogram, submits analysis operation and rear place Reason finally obtains residual stress field and displacement deformation distribution.
Preferably, in above-mentioned Finite Element Method, the implementation of this method need to only carry out Explicit Analysis, each Explicit Analysis The time of step is 8 × 10-6s。
Preferably, described that the laser-impact time of more hot spots and position distribution are carried out in above-mentioned Finite Element Method Subprogram editor, specifically includes:
Using Fortran language editing subroutines, laser-impact time and position distribution to more hot spots are into edlin.
Preferably, in above-mentioned Finite Element Method, the laser is three-dimensional Flattened Gaussian Beams, the space at z=0 It is distributed as following formula:
In formula, N, M, W0x, W0yRespectively exponent number and waist width of the Flattened Gaussian Beams in the direction x, y.
Using laser impact intensified Finite Element Method provided by the invention, the laser reinforcing of more hot spots is rushed It hits, only need to carry out Explicit Analysis, the load of different location different moments is realized using subprogram, improves efficiency, simultaneously for Different technological parameters (laser power density, shock peening route, strengthens number, overlapping rate, pulsewidth at spot radius), only needs An analysis model is established, remaining work is completed by subprogram.Therefore this method has rapid, inexpensive, easy to be easy Row calculates accurate feature, and future in engineering applications is good.It can be conveniently to the laser impact intensified carry out mould of more hot spots It is quasi-, to provide reliable basis to parameter optimization.
Description of the drawings
In order to more clearly explain the embodiment of the invention or the technical proposal in the existing technology, to embodiment or will show below There is attached drawing needed in technology description to be briefly described, it should be apparent that, the accompanying drawings in the following description is only this Some embodiments of invention for those of ordinary skill in the art without creative efforts, can be with Obtain other attached drawings according to these attached drawings.
Fig. 1 is the flow diagram of the laser impact intensified Finite Element Method of a specific embodiment of the invention;
Fig. 2 is laser blast wave loading curve.
Specific implementation mode
The embodiment of the invention discloses a kind of Finite Element Methods, excellent in order to the laser impact intensified parameter of more hot spots Change.
Following will be combined with the drawings in the embodiments of the present invention, and technical solution in the embodiment of the present invention carries out clear, complete Site preparation describes, it is clear that described embodiments are only a part of the embodiments of the present invention, instead of all the embodiments.It is based on Embodiment in the present invention, it is obtained by those of ordinary skill in the art without making creative efforts every other Embodiment shall fall within the protection scope of the present invention.
- Fig. 2 is please referred to Fig.1, Fig. 1 is the flow signal for the laser impact intensified Finite Element Method that the present invention is implemented Figure;Fig. 2 is laser blast wave loading curve.
In the diagram, a kind of laser impact intensified Finite Element Method, includes the following steps:
S1:It establishes threedimensional model in ABAQUS, material property parameter is set, using Johnson-Cook constitutive equations, Setting dynamic explicit analysis step simultaneously so that plasticity variation reaches maximum value inside target in each analysis step, while kinetic energy is last Level off to 0;
The time of specific each analysis step can be configured as needed, can be not especially limited herein.
S2:Subprogram editor is carried out to the laser-impact time of more hot spots and position distribution, realizes the application of load;
Namely realize that the application of load, parameter of specific load etc. can be configured as needed by subprogram, in detail Thin refer to the prior art, and details are not described herein again.
S3:Mesh generation carries out mesh refinement in Laser Shock Processing domain;
S4:It creates analysis operation and carries out Explicit solutions, obtain residual stress field and displacement deformation distribution.
This analytic process need to only use Explicit solvers, you can obtain residual stress and displacement deformation distribution.Pass through Subprogram realizes the load of more hot spot different location different moments, brings great convenience to the application of load.
Using laser impact intensified Finite Element Method provided by the invention, the laser reinforcing of more hot spots is rushed It hits, only need to carry out Explicit Analysis, the load of different location different moments is realized using subprogram, improves efficiency, simultaneously for Different technological parameters (laser power density, shock peening route, strengthens number, overlapping rate, pulsewidth at spot radius), only needs An analysis model is established, remaining work is completed by subprogram.Therefore this method has rapid, inexpensive, easy to be easy Row calculates accurate feature, and future in engineering applications is good.It can be conveniently to the laser impact intensified carry out mould of more hot spots It is quasi-, to provide reliable basis to parameter optimization.
Further, it in above-mentioned steps S3, specifically includes:
Laser Shock Processing domain carries out mesh refinement using cell type C3D8R, and by laser-impact target frontier district Domain is set as Infinite Element and carries out mesh generation using C3D8;
Then, analysis operation is created in step S4 and carries out Explicit solutions, obtains residual stress field and displacement deformation distribution, It specifically includes:
It creates analysis operation and generates INP files, the cell type of Infinite Element is changed to CIN3D8 in INP files, it is raw The INP files of Cheng Xin;Analysis operation is created again, while calling new INP files and subprogram, submits analysis operation and rear place Reason finally obtains residual stress field and displacement deformation distribution.
Preferably, in above-mentioned Finite Element Method, Explicit Analysis, and the time of each Explicit Analysis step need to only be carried out It is 8 × 10-6s.According to specific needs, the time that can also be walked to Explicit Analysis is suitably adjusted.
Specifically, in above-mentioned Finite Element Method, sub- journey is carried out to the laser-impact time of more hot spots and position distribution Sequence editor, specifically includes:
Using Fortran language editing subroutines, laser-impact time and position distribution to more hot spots are into edlin.It adopts Subprogram editor is carried out with Fortran language, is convenient for the calling of subroutine, the machine that other can also be used conventional as needed Device language editing subroutine.
Preferably, in above-mentioned Finite Element Method, the laser is three-dimensional Flattened Gaussian Beams, the space at z=0 It is distributed as following formula:
In formula, N, M, W0x, W0yRespectively exponent number and waist width of the Flattened Gaussian Beams in the direction x, y.As needed Other conventional laser beams may be used.
It is illustrated by taking a preferred embodiment as an example below.
By taking material 2050-T8 aluminium alloys as an example, finite element modelling is carried out, is included the following steps:
Step 1, geometrical model and definition material and section attribute are established in ABAQUS:Geometric dimension is 25mm*25mm* 5mm, density of material 2750kg/m3, Poisson's ratio 0.33, elasticity modulus 72GPa.It is described using Johnson-Cook models The dynamic constitutive of 2050-T8, formula (1) are the expression formula of the model.
In formula:A is yield strength, and B and n have reacted the strain hardening feature of material, and C reflects strain rate to material property Influence, εpEquivalent plastic strain is represented,For static strain rate, value herein is A=510MPa, B=200MPa, n =0.45, C=0.02,Dynamic explicit analysis step is set it is ensured that in each analysis step plasticity inside target Variation reaches maximum value, while kinetic energy, finally close to 0, the time of each analysis step is set as 8 × 10-6s;
Apply load:Laser power density is 3.5GW/cm2, using circular light class, spot diameter 1.5mm, pulse width It is set as 10ns, spatial distribution of the three-dimensional Flattened Gaussian Beams at z=0 is formula 2, and laser blast wave loading curve is Fig. 2, Using Fortran language editing subroutines, laser-impact time and position distribution to more hot spots are into edlin;
In formula, N, M, W0x, W0yRespectively exponent number and waist width of the Flattened Gaussian Beams in the direction x, y.
Step 3, mesh generation:Mesh refinement is carried out in Laser Shock Processing domain, uses cell type for C3D8R;It will Laser-impact target borderline region is set as Infinite Element, and first using cell type C3D8, unit size size is for the part 150μm*150μm*50μm;
Step 4, it creates analysis operation and generates INP files, be changed to the cell type of Infinite Element part in INP files CIN3D8 generates new INP files;Analysis operation is created again, while calling new INP files and Fortran language editors Subprogram, submit analysis operation and post-processing, finally obtain residual stress field and displacement deformation distribution.
The aluminium alloy plate laser impact intensified to three-dimensional Flattened Gaussian Beams is simulated using finite element software ABAQUS Analysis, this analytic process need to only use Explicit solvers, you can obtain residual stress and displacement deformation distribution.The present invention is logical Crossing Fortran language editing subroutines realizes the load of more hot spot different location different moments, is brought to the application of load Great convenience, while in optimization shock peening technological parameter (laser power density, spot radius, shock peening route, reinforcing time Number, overlapping rate, pulsewidth) on bring great convenience, study process above parameter on laser shock peening influence when only need An analysis model is established, remaining is operated in subprogram and completes, and improves modeling efficiency.This finite element model simultaneously Infinite Element is used as reflecting boundary, prevents from generating stress wave reflection on boundary, reenters model, so as to cause knot Fruit is incorrect, and the use of Infinite Element, which can also be reduced, calculates the time.The analogy method is high, at low cost with modeling efficiency, counts It calculates feature true, that the time is short accurately, there is certain future in engineering applications.
Each embodiment is described by the way of progressive in this specification, the highlights of each of the examples are with other The difference of embodiment, just to refer each other for identical similar portion between each embodiment.
The foregoing description of the disclosed embodiments enables those skilled in the art to implement or use the present invention. Various modifications to these embodiments will be apparent to those skilled in the art, as defined herein General Principle can be realized in other embodiments without departing from the spirit or scope of the present invention.Therefore, of the invention It is not intended to be limited to the embodiments shown herein, and is to fit to and the principles and novel features disclosed herein phase one The widest range caused.

Claims (5)

1. a kind of laser impact intensified Finite Element Method, which is characterized in that including step:
Threedimensional model is established in ABAQUS, material property parameter is set, using Johnson-Cook constitutive equations, setting dynamic Explicit Analysis walks and so that in each analysis walks inside target that plasticity variation reaches maximum value, while kinetic energy finally levels off to 0;
Subprogram editor is carried out to the laser-impact time of more hot spots and position distribution, realizes the application of load;
Mesh generation carries out mesh refinement in Laser Shock Processing domain;
It creates analysis operation and carries out Explicit solutions, obtain residual stress field and displacement deformation distribution.
2. Finite Element Method according to claim 1, which is characterized in that the mesh generation is strong in laser-impact Change region and carry out mesh refinement, specifically includes:
Laser Shock Processing domain carries out mesh refinement using cell type C3D8R, and by the borderline region of laser-impact target It is set as Infinite Element and mesh generation is carried out using C3D8;
It creates analysis operation and carries out Explicit solutions, obtain residual stress field and displacement deformation distribution, specifically include:
It creates analysis operation and generates INP files, the cell type of Infinite Element is changed to CIN3D8 in INP files, generate new INP files;Analysis operation is created again, while calling new INP files and subprogram, submits analysis operation and post-processing, Finally obtain residual stress field and displacement deformation distribution.
3. Finite Element Method according to claim 1, which is characterized in that the implementation of this method only need to explicitly be divided The time of analysis, each Explicit Analysis step is 8 × 10-6s。
4. Finite Element Method according to claim 1, which is characterized in that the laser-impact time to more hot spots Subprogram editor is carried out with position distribution, is specifically included:
Using Fortran language editing subroutines, laser-impact time and position distribution to more hot spots are into edlin.
5. according to claim 1-4 any one of them Finite Element Methods, which is characterized in that the laser is three-dimensional flat-top Gaussian beam, the spatial distribution at z=0 are following formula:
In formula, N, M, W0x, W0yRespectively exponent number and waist width of the Flattened Gaussian Beams in the direction x, y.
CN201710392734.2A 2017-05-27 2017-05-27 Laser impact intensified Finite Element Method Active CN107217133B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201710392734.2A CN107217133B (en) 2017-05-27 2017-05-27 Laser impact intensified Finite Element Method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201710392734.2A CN107217133B (en) 2017-05-27 2017-05-27 Laser impact intensified Finite Element Method

Publications (2)

Publication Number Publication Date
CN107217133A CN107217133A (en) 2017-09-29
CN107217133B true CN107217133B (en) 2018-10-19

Family

ID=59947059

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201710392734.2A Active CN107217133B (en) 2017-05-27 2017-05-27 Laser impact intensified Finite Element Method

Country Status (1)

Country Link
CN (1) CN107217133B (en)

Families Citing this family (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107794362B (en) * 2017-09-30 2020-02-07 广东工业大学 Online real-time variable pulse width blade laser shock strengthening deformation control method
CN107937705B (en) * 2017-11-28 2019-11-08 广东工业大学 A kind of method and system of metal-surface strengthening
CN110361121B (en) * 2018-04-09 2020-12-25 中国科学院沈阳自动化研究所 Accurate prediction method for laser shock peening induced residual stress field
CN108531714B (en) * 2018-07-04 2019-05-10 北京航空航天大学 A kind of multi-Precision optimization method that mortise structure is laser impact intensified
CN109777942B (en) * 2019-01-31 2020-06-02 中国石油大学(华东) Welding stress and deformation regulation and control method for local postweld heat treatment of ultra-large pressure container
CN110162834A (en) * 2019-04-11 2019-08-23 广东镭奔激光科技有限公司 The analogy method and reinforcing quality control apparatus of laser-impact data based on acquisition
JP2023506346A (en) 2019-12-13 2023-02-16 カーステン マニュファクチュアリング コーポレーション Golf club head with textured striking face and method of making same
CN111985131B (en) * 2020-08-10 2022-10-04 北京航空航天大学 Turbine mortise laser shock peening numerical simulation method considering curved surface shape
CN111931408B (en) * 2020-08-13 2023-02-10 广东工业大学 Finite element simulation method for laser spalling process
CN113913604B (en) * 2021-08-10 2023-05-23 中国航发常州兰翔机械有限责任公司 Helicopter director lug curved surface water coating control method and system

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103246772A (en) * 2013-05-11 2013-08-14 天津大学 ABAQUS-based finite element simulation method of correcting welding deformation through ultrasonic shot-peening
CN105117547A (en) * 2015-08-25 2015-12-02 大连理工大学 Simulation method for residual stress prediction of micro-milling nickel-based superalloy
CN105224758A (en) * 2015-10-13 2016-01-06 河海大学 A kind of for design-calculated Ballast track high-speed railway modeling Analysis method
CN105224750A (en) * 2015-10-10 2016-01-06 北京工业大学 A kind of new spatial based on response surface can open up single reed structure optimization method in hinge

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20080078479A1 (en) * 2006-09-29 2008-04-03 Massachusetts Institute Of Technology Determining constitutive models for fracture prediction in ductile materials undergoing plastic deformation

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103246772A (en) * 2013-05-11 2013-08-14 天津大学 ABAQUS-based finite element simulation method of correcting welding deformation through ultrasonic shot-peening
CN105117547A (en) * 2015-08-25 2015-12-02 大连理工大学 Simulation method for residual stress prediction of micro-milling nickel-based superalloy
CN105224750A (en) * 2015-10-10 2016-01-06 北京工业大学 A kind of new spatial based on response surface can open up single reed structure optimization method in hinge
CN105224758A (en) * 2015-10-13 2016-01-06 河海大学 A kind of for design-calculated Ballast track high-speed railway modeling Analysis method

Also Published As

Publication number Publication date
CN107217133A (en) 2017-09-29

Similar Documents

Publication Publication Date Title
CN107217133B (en) Laser impact intensified Finite Element Method
Arif Numerical prediction of plastic deformation and residual stresses induced by laser shock processing
CN103246772A (en) ABAQUS-based finite element simulation method of correcting welding deformation through ultrasonic shot-peening
CN109063248B (en) Gas-liquid-solid coupling calculation method for laser shock peening
CN107180131A (en) Method for determining the laser impact intensified thin-wall part Deformation Curvature radius of multiple spot
Zhang et al. Numerical and experimental investigations of laser shock forming aluminum alloy sheet with mold
CN111310375A (en) Machining method for optimizing shock wave pressure of laser double-sided simultaneous opposite impact titanium alloy blade
Riazuelo et al. Coherence properties of a smoothed laser beam in a hot plasma
CN107633115A (en) The Finite Element Method of multiple spot laser impact forming
CN109359337B (en) Simulation method for variable light spot and powder particle size coupling effect
Tikhonchuk et al. Physics of laser-plasma interaction for shock ignition of fusion reactions
CN103712724B (en) A kind of characterizing method based on relative laser-impact intensity
Cela et al. Numerical simulations of Rayleigh-Taylor instability in elastic solids
Mironov et al. Effect of the laser pulse temporal shape on the hole boring efficiency
Hu et al. Study on residual stress of laser shock processing based on numerical simulation and orthogonal experimental design
Hua et al. Laser shock forming of aluminum sheet: Finite element analysis and experimental study
Zhang et al. Numerical investigation of surface textural dimples of titanium alloy subjected to laser shock processing
Togashi et al. Numerical simulation of H 2/air detonation using unstructured mesh
CN209416639U (en) Laser pumping formula firer's shock simulation device
CN110361121A (en) A kind of accurate prediction technique in laser impact intensified induction residual stress field
Danduk et al. Modeling and strategies for laser shock processing
Singh et al. Modeling and optimization of a laser shock peening process
Ohnishi et al. Numerical Simulation of Laser‐Driven In‐Tube Accelerator Operation
Dai et al. Surface dynamic deformation of LY2 aluminum alloy subjected to a laser shock wave planishing technique with different kinds of contacting foils
WEI et al. Mitigation of Tensile Residual Stress Induced During Welding with Laser Shock Processing.

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
GR01 Patent grant
GR01 Patent grant