CN105653822A - Cellular automaton method simulating static recrystallization behavior of GH4169 alloy - Google Patents

Cellular automaton method simulating static recrystallization behavior of GH4169 alloy Download PDF

Info

Publication number
CN105653822A
CN105653822A CN201610060605.9A CN201610060605A CN105653822A CN 105653822 A CN105653822 A CN 105653822A CN 201610060605 A CN201610060605 A CN 201610060605A CN 105653822 A CN105653822 A CN 105653822A
Authority
CN
China
Prior art keywords
cellular
variable
sub
static recrystallization
recrystallization
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.)
Granted
Application number
CN201610060605.9A
Other languages
Chinese (zh)
Other versions
CN105653822B (en
Inventor
蔺永诚
刘延星
陈明松
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.)
Central South University
Original Assignee
Central South 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 Central South University filed Critical Central South University
Priority to CN201610060605.9A priority Critical patent/CN105653822B/en
Publication of CN105653822A publication Critical patent/CN105653822A/en
Application granted granted Critical
Publication of CN105653822B publication Critical patent/CN105653822B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F30/00Computer-aided design [CAD]
    • G06F30/20Design optimisation, verification or simulation

Landscapes

  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Theoretical Computer Science (AREA)
  • Computer Hardware Design (AREA)
  • Evolutionary Computation (AREA)
  • Geometry (AREA)
  • General Engineering & Computer Science (AREA)
  • General Physics & Mathematics (AREA)
  • Management, Administration, Business Operations System, And Electronic Commerce (AREA)
  • Investigating And Analyzing Materials By Characteristic Methods (AREA)

Abstract

The invention discloses a cellular automaton method simulating the static recrystallization behavior of GH4169 alloy. The method includes the following steps that firstly, an initial microstructure is generated; secondly, the static recrystallization behavior is simulated. The cellular automaton method simulating the static recrystallization behavior of GH4169 alloy is a static recrystallization behavior simulating method based on a physical mechanism, the static recrystallization behavior of GH4169 alloy can be accurately simulated, and technological support is provided for reasonably formulating the hot working technology of GH4169 alloy.

Description

A kind of cellular automation method simulating GH4169 alloy Static Recrystallization behavior
Technical field
The present invention relates to a kind of cellular automation method simulating GH4169 alloy Static Recrystallization behavior, belong to hot-working field of engineering technology.
Background technology
GH4169 alloy has the elevated temperature strength of excellence, resisting fatigue, creep resistant, antioxidation and decay resistance, is widely used in manufacturing the key components and parts of aero-engine: such as the turbine disk, compressor disc, casing etc. Large complicated GH4169 alloyed components generally adopts the multi-stage deep drawing modes such as forging, rolling, extruding to shape. In the forming process of these parts, the Microstructure evolution of alloy is sufficiently complex. Holding stage after hot formed passage interval time and deformation, static recovery, Static Recrystallization or meta-dynamic recrystallization etc. all can occur. This can significantly change the microstructure of alloy, and then affects the quality of forging. In order to obtain the GH4169 alloyed components of high-quality, need a kind of method that can accurately predict alloy Microstructure evolution badly, provide reliable microstructure Prediction means for heat forming technology optimization.
But, owing to GH4169 alloy structure development law in Static Recrystallization process is sufficiently complex, still lack at present and can accurately simulate the method for Microstructure evolution in GH4169 alloy passage interval time. For this difficult problem, the invention provides a kind of cellular automation method that can simulate GH4169 alloy Static Recrystallization behavior. The novelty of the present invention is in that, cellular models introduces the main physical factors affecting recrystallization behavior, drastically increase the precision of prediction of model, it is proposed to method verified by embodiment, result shows that this method can simulate GH4169 alloy Static Recrystallization behavior effectively.
Summary of the invention
It is an object of the invention to provide a kind of cellular automation method simulating GH4169 alloy Static Recrystallization behavior, the method is based on physical mechanism and sets up, it is possible to the forming core of grain structure and rule of growing up in the Static Recrystallization process of the GH4169 that calculates to a nicety.
For reaching above-mentioned purpose, the present invention adopts the technical scheme that: a kind of cellular automation method simulating GH4169 alloy Static Recrystallization behavior, and the method comprises the following steps:
Step 1: generate the step of initial microstructure;
Step 2: the step of simulation Static Recrystallization behavior;
Step 1 includes following sub-step:
(1) selected simulated domain, by discrete for the simulated domain grid for being made up of cellular, sets total simulation step number;
(2) composing initial value to cellular state variable, cellular state variable includes crystal grain numbering variable and grain orientation variable;
(3) in selected simulated domain, N is randomly selectedgIndividual cellular, and give selected NgIndividual cellular composes different crystal grain numbering variablees and grain orientation variable;
(4) all cellulars are carried out one by one calculated below: assuming the state that state transfer is neighbours' cellular of current cellular, the change of computing system energy, if system capacity reduces, then by state that the state transfer of current cellular is neighbours' cellular;
(5) sub-step (4) of step 1 is repeated, until completing total simulation step number;
Step 2 includes following sub-step:
(1) time step �� t and total simulated time t is determinedtotal, compose initial value for cellular state variable; Cellular state variable includes dislocation density variable, recrystallization degree variables, crystal boundary migration distance variable, crystal grain numbering variable and grain orientation variable; Dislocation density initial guess is ��1, recrystallization degree variables initial value is 0, and crystal boundary migration distance initial guess is 0, and crystal grain numbering variable and grain orientation variable are with the result of calculation of step 1 for initial value;
(2) sub-step of Static Recrystallization forming core is simulated;
(3) sub-step of Static Recrystallization grain growth is simulated;
(4) judge whether to reach total simulated time, if not up to, then again performing sub-step (2) and sub-step (3), if having reached total simulated time, stopping simulation;
The sub-step (2) of step 2 comprises the steps:
A. the cellular number N in statistics original grain boundarypg;
B. Static Recrystallization nucleation rate is calculated, computing formula is:
N · = C 1 ( G - G 0 ) C 2 exp ( - Q n / R T )
Wherein, C1��C2And QnFor material parameter, G is deformation energy, G0For the critical energy storage needed for Static Recrystallization forming core, R is ideal gas constant, and T is deformation temperature; Material parameter C1Span be 900-1500, material parameter C2Span be 0-100, material parameter QnSpan be 105-106;
C. the cellular number N of Static Recrystallization forming core is calculatedn, and, A in formulacFor single cell density;
Compose a forming core probability P d. to all cellulars being positioned in original grain boundaryn, and Pn=Nn/Npg, by forming core probability PnThe random number generated with computer contrasts, if forming core probability PnLess than the random number that computer generates, then current cellular is chosen to be Static Recrystallization nucleus, and the dislocation density variable of current cellular is reset to ��0, the recrystallization degree variables of current cellular adds 1, the crystal boundary migration distance variable zero setting of current cellular;
E. the step d of the sub-step (2) of step 2 is repeated, until selecting NnIndividual Static Recrystallization nucleus;
The sub-step (3) of step 2 comprises the steps:
A. crystal boundary migration driving force P, P=�� (�� is calculated1-��0), the �� in formula is dislocation line energy;
B. calculating crystal boundary migration speed V, V=MP, the M in formula is crystal boundary migration rate, and computing formula is
M = δD 0 b exp ( - Q b / R T ) k T b
Wherein, �� D0bAnd QbFor material parameter, �� D0bSpan be 10-11-10-10, QbSpan be 105-106, b is Bai Shi vector, and k is Boltzmann constant;
C. crystal boundary migration distance variables L, L=V �� t are calculated;
If d. crystal boundary migration distance variables L is more than the distance between adjacent two cellulars, then by state that the state transfer of current cellular is recrystallization degree variables neighbours' cellular more than 1.
The novelty of the present invention and have the beneficial effect that (1) incorporates, in Static Recrystallization nucleation rate computing formula, the main physical factors affecting nucleation process, it is possible to describe the nucleation of GH4169 Static Recrystallization exactly; (2) result of calculation of crystal boundary migration rate can reflect the effect of dragging of solute element, meets the development law of alloy crystal boundary migration rate; (3) present invention is the Static Recrystallization analogy method of a kind of physically based deformation mechanism, it is possible to relatively accurately simulation GH4169 alloy Static Recrystallization behavior.
Accompanying drawing explanation
Contrast between crystallite dimension predictive value and the measured value of Fig. 1 this method;
The microstructure predicting result of Fig. 2 this method and the contrast of experimental result;
Detailed description of the invention
Below in conjunction with accompanying drawing, the present invention is described further.
The present invention is a kind of cellular automation method simulating GH4169 alloy Static Recrystallization behavior, and the method comprises the following steps:
Step 1: generate the step of initial microstructure;
Step 2: the step of simulation Static Recrystallization;
Step 1 includes following sub-step:
(1) selected simulated domain 920 �� 920 ��m2, it being divided into 460 �� 460 grids, the length of side of each square cellular is LcIt is 2 ��m, sets total simulation step number as 300;
(2) composing initial value to cellular state variable, cellular state variable includes crystal grain numbering variable and grain orientation variable;
(3) in selected simulated domain, randomly select 178 cellulars, and compose different crystal grain numbering variablees and grain orientation variable to 178 selected cellulars;
(4) all cellulars are carried out one by one calculated below: assuming the state that state transfer is neighbours' cellular of current cellular, the change of computing system energy, if system capacity reduces, then by state that the state transfer of current cellular is neighbours' cellular;
(5) sub-step (4) of step 1 is repeated, until it reaches total simulation step number;
Step 2 includes following sub-step:
(1) time step �� t, �� t=L is determinedc/(M��(��1-��0)), total simulated time ttotalFor 600s, compose initial value to cellular state variable; Cellular state variable includes dislocation density variable, recrystallization degree variables, crystal boundary migration distance variable, crystal grain numbering variable and grain orientation variable; Dislocation density initial guess is ��1, can be obtained by interrupt experiments; Recrystallization degree variables initial value is 0, and crystal boundary migration distance initial guess is 0, and grain orientation variable and grain orientation variable are with the result of calculation of step 1 for initial value;
(2) sub-step of Static Recrystallization forming core is simulated;
(3) sub-step of Static Recrystallization grain growth is simulated;
(4) judge whether to reach total simulated time, if not up to, then again performing sub-step (2) and sub-step (3), if having reached total simulated time, stopping simulation;
The sub-step (2) of step 2 comprises the steps:
A. the cellular number N in statistics original grain boundarypg;
B. Static Recrystallization nucleation rate is calculated, computing formula is:
N · = C 1 ( G - G 0 ) C 2 exp ( - Q n / R T )
Wherein, C1��C2And QnFor material parameter, C1It is 994, C2It is 5.42, QnBe 669286, G it is deformation energy, G0For the critical energy storage needed for Static Recrystallization forming core, R is ideal gas constant, and T is deformation temperature;
C. the cellular number N of Static Recrystallization forming core is calculatedn,, A in formulacFor single cell density;
Compose a forming core probability P d. to all cellulars being positioned in original grain boundaryn, and Pn=Nn/Npg, by forming core probability PnThe random number generated with computer contrasts, if forming core probability PnLess than the random number that computer generates, then current cellular is chosen to be Static Recrystallization nucleus, and the dislocation density variable of current cellular is reset to ��0, ��0Can obtaining according to yield stress reverse, the recrystallization degree variables of current cellular adds 1, the crystal boundary migration distance variable zero setting of current cellular;
E. the step d of the sub-step (2) of step 2 is repeated, until selecting NnIndividual Static Recrystallization nucleus;
The sub-step (3) of step 2 comprises the steps:
A. crystal boundary migration driving force P, P=�� (�� is calculated1-��0), the �� in formula is dislocation line energy;
B. calculating crystal boundary migration speed V, V=MP, the M in formula is crystal boundary migration rate, and computing formula is
M = δD 0 b exp ( - Q b / R T ) k T b
Wherein, �� D0bAnd QbFor material parameter, �� D0bAnd QbValue respectively 6.79 �� 10-11With 2.97 �� 105, b is Bai Shi vector, and k is Boltzmann constant;
C. crystal boundary migration distance variables L, L=V �� t are calculated;
If d. crystal boundary migration distance variables L is more than the distance between adjacent two cellulars, then by state that the state transfer of current cellular is recrystallization degree variables neighbours' cellular more than 1.
Adopting said method, GH4169 Static Recrystallization behavior within the scope of 1253-1313K is simulated, Fig. 1 is that crystallite dimension predicts the outcome the contrast with measurement result, and Fig. 2 is the contrast of microstructure predicting result and experimental result. By the comparing result of Fig. 1 and Fig. 2 it can be seen that the present invention can relatively accurately describe the Static Recrystallization behavior of GH4169 alloy.

Claims (1)

1. the cellular automation method simulating GH4169 alloy Static Recrystallization behavior, it is characterised in that: the method comprises the following steps:
Step 1: generate the step of initial microstructure;
Step 2: the step of simulation Static Recrystallization behavior;
Described step 1 includes following sub-step:
(1) selected simulated domain, by discrete for the simulated domain grid for being made up of cellular, sets total simulation step number;
(2) composing initial value to cellular state variable, described cellular state variable includes crystal grain numbering variable and grain orientation variable;
(3) in selected simulated domain, N is randomly selectedgIndividual cellular, and give selected NgIndividual cellular composes different crystal grain numbering variablees and grain orientation variable;
(4) all cellulars are carried out one by one calculated below: assuming the state that state transfer is neighbours' cellular of current cellular, the change of computing system energy, if system capacity reduces, then by state that the state transfer of current cellular is neighbours' cellular;
(5) sub-step (4) of repeating said steps 1, until completing described total simulation step number;
Described step 2 includes following sub-step:
(1) time step �� t and total simulated time t is determinedtotal, compose initial value for cellular state variable; Described cellular state variable includes dislocation density variable, recrystallization degree variables, crystal boundary migration distance variable, crystal grain numbering variable and grain orientation variable; Institute's dislocation density initial guess is ��1, described recrystallization degree variables initial value is 0, and described crystal boundary migration distance initial guess is 0, and described crystal grain numbering variable and described grain orientation variable are with the result of calculation of described step 1 for initial value;
(2) sub-step of Static Recrystallization forming core is simulated;
(3) sub-step of Static Recrystallization grain growth is simulated;
(4) judge whether to reach described total simulated time, if not up to, then again performing described sub-step (2) and described sub-step (3), if having reached described total simulated time, then stopping simulation;
The described sub-step (2) of described step 2 comprises the steps:
A. the cellular number N in statistics original grain boundarypg;
B. Static Recrystallization nucleation rate is calculatedComputing formula is:
N · = C 1 ( G - G 0 ) C 2 exp ( - Q n / R T )
Wherein, C1��C2And QnFor material parameter, G is deformation energy, G0For the critical energy storage needed for Static Recrystallization forming core, R is ideal gas constant, and T is deformation temperature; Described material parameter C1Span be 900-1500, described material parameter C2Span be 0-100, described material parameter QnSpan be 105-106;
C. the cellular number N of Static Recrystallization forming core is calculatedn, andA in formulacFor single cell density;
Compose a forming core probability P d. to all cellulars being positioned in original grain boundaryn, and Pn=Nn/Npg, by described forming core probability PnThe random number generated with computer compares, if described forming core probability PnLess than the random number that described computer generates, then current cellular is chosen to be Static Recrystallization nucleus, and the dislocation density variable of described current cellular is reset to ��0, recrystallization degree variables add 1 and crystal boundary migration distance variable zero setting;
E. the step d of the sub-step (2) in repeating said steps 2, until selecting NnIndividual Static Recrystallization nucleus;
Sub-step (3) in described step 2 comprises the steps:
A. crystal boundary migration driving force P, P=�� (�� is calculated1-��0), the �� in formula is dislocation line energy;
B. calculating crystal boundary migration speed V, V=MP, the M in formula is crystal boundary migration rate, and computing formula is
M = δD 0 b exp ( - Q b / R T ) k T b
Wherein, �� D0bAnd QbFor material parameter, �� D0bSpan be 10-11-10-10, QbSpan be 105-106, b is Bai Shi vector, and k is Boltzmann constant;
C. described crystal boundary migration distance variables L, L=V �� t are calculated;
If d. crystal boundary migration distance variables L is more than the distance between adjacent two cellulars, then by state that the state transfer of current cellular is recrystallization degree variables neighbours' cellular more than 1.
CN201610060605.9A 2016-01-29 2016-01-29 A kind of cellular automation method of simulation GH4169 alloy Static Recrystallization behaviors Expired - Fee Related CN105653822B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201610060605.9A CN105653822B (en) 2016-01-29 2016-01-29 A kind of cellular automation method of simulation GH4169 alloy Static Recrystallization behaviors

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201610060605.9A CN105653822B (en) 2016-01-29 2016-01-29 A kind of cellular automation method of simulation GH4169 alloy Static Recrystallization behaviors

Publications (2)

Publication Number Publication Date
CN105653822A true CN105653822A (en) 2016-06-08
CN105653822B CN105653822B (en) 2018-11-09

Family

ID=56488100

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201610060605.9A Expired - Fee Related CN105653822B (en) 2016-01-29 2016-01-29 A kind of cellular automation method of simulation GH4169 alloy Static Recrystallization behaviors

Country Status (1)

Country Link
CN (1) CN105653822B (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106053754A (en) * 2016-07-06 2016-10-26 中南大学 Method for predicting dynamic recrystallization fractions of high-alloy materials under time-varying working conditions
CN106944607A (en) * 2017-04-25 2017-07-14 哈尔滨理工大学 A kind of inoculant alloy grain structure Numerical Predicting Method
CN110706758A (en) * 2019-09-12 2020-01-17 上海交通大学 Multistage cellular automata method for simulating dynamic recrystallization
CN110929416A (en) * 2019-12-06 2020-03-27 大连大学 Method for simulating Ni-Mn-In alloy structure evolution process based on cellular automaton
CN113808678A (en) * 2021-09-28 2021-12-17 东莞理工学院 Cellular automata method for simulating growth behavior of GH4169 alloy crystal grains

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104928605A (en) * 2015-07-20 2015-09-23 中南大学 Method for predicting nickel base alloy high temperature flow stress and dynamic recrystallization behavior

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104928605A (en) * 2015-07-20 2015-09-23 中南大学 Method for predicting nickel base alloy high temperature flow stress and dynamic recrystallization behavior

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
YAN-XING LIU, Y.C.LIN, HONG-BIN LI, DONG-XUWEN, XIAO-MIN CHEN, M: "《Study of dynamic recrystallization in a Ni-based superalloy by experiments and cellular automaton model》", 《MATERIALS SCIENCE & ENGINEERING A》 *
郭娟,王艳敏,李卫,吴迪,赵宪明: "《静态再结晶过程的元胞自动机模拟Ⅰ——微观组织演化和动力学研究》", 《大型铸锻件》 *

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106053754A (en) * 2016-07-06 2016-10-26 中南大学 Method for predicting dynamic recrystallization fractions of high-alloy materials under time-varying working conditions
CN106053754B (en) * 2016-07-06 2017-11-14 中南大学 A kind of method that high-alloying MATERIALS ' DYNAMIC recrystallizes fraction under variable working condition during prediction
CN106944607A (en) * 2017-04-25 2017-07-14 哈尔滨理工大学 A kind of inoculant alloy grain structure Numerical Predicting Method
CN110706758A (en) * 2019-09-12 2020-01-17 上海交通大学 Multistage cellular automata method for simulating dynamic recrystallization
CN110706758B (en) * 2019-09-12 2022-02-11 上海交通大学 Multistage cellular automata method for simulating dynamic recrystallization
CN110929416A (en) * 2019-12-06 2020-03-27 大连大学 Method for simulating Ni-Mn-In alloy structure evolution process based on cellular automaton
CN113808678A (en) * 2021-09-28 2021-12-17 东莞理工学院 Cellular automata method for simulating growth behavior of GH4169 alloy crystal grains
CN113808678B (en) * 2021-09-28 2024-05-07 东莞理工学院 Cellular automaton method for simulating growth behavior of GH4169 alloy crystal grains

Also Published As

Publication number Publication date
CN105653822B (en) 2018-11-09

Similar Documents

Publication Publication Date Title
CN105653822A (en) Cellular automaton method simulating static recrystallization behavior of GH4169 alloy
Reyes et al. Grain size modeling of a Ni-base superalloy using cellular automata algorithm
CN104928605A (en) Method for predicting nickel base alloy high temperature flow stress and dynamic recrystallization behavior
US11574095B2 (en) Simulation system for semiconductor process and simulation method thereof
CN102339344B (en) Back analysis identification method for parameters of dynamic re-crystallizing model
CN111069328A (en) Isothermal extrusion process parameter optimization method based on particle swarm optimization
Cao et al. Cellular automaton simulation of dynamic recrystallization behavior in V-10Cr-5Ti alloy under hot deformation conditions
Ramakokovhu et al. Significance of residual stresses in fatigue life prediction of micro gas turbine blades
CN112288139A (en) Air conditioner energy consumption prediction method and system based on chaotic time sequence and storage medium
CN107229771B (en) Method for carrying out simulation measurement on spring pressing force of nuclear fuel plate
Hasan et al. ANN modeling of nickel base super alloys for time dependent deformation
CN115130239A (en) Mechanical property prediction method for metal additive manufacturing based on multi-scale modeling
Sulzer et al. Critical assessment 31: on the modelling of tertiary creep in single-crystal superalloys
Guan-feng et al. Constitutive model of 25CrMo4 steel based on IPSO-SVR and its application in finite element simulation
Wen et al. Deep learning-based modeling of the strain rate-dependent thermomechanical processing response for a novel HIPed P/M nickel-based superalloy
Gan et al. Atomic insights into the effects of Al element on the nanoindentation behavior of single-crystal FeNiCoCr-based multicomponent alloys
Longuet et al. Advanced modeling tools for processing and lifing of aeroengine components
CN104951633B (en) A kind of method for predicting nickel-base alloy processing hardening and dynamic recovery behavior
CN111210877B (en) Method and device for deducing physical parameters
Azarbarmas et al. A new cellular automaton method coupled with a rate-dependent (CARD) model for predicting dynamic recrystallization behavior
CN107061032A (en) The Forecasting Methodology and forecasting system of a kind of engine operating state
Zaletelj et al. Numerical methods for TMF cycle modeling
CN114864017A (en) Prediction calculation method and system for global grain size of aluminum alloy casting
Taverniers et al. Physics-based statistical learning approach to mesoscopic model selection
Yu et al. Cellular automata method for simulating microstructure evolution

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20181109

Termination date: 20200129