Issue 
Manufacturing Rev.
Volume 5, 2018



Article Number  10  
Number of page(s)  18  
DOI  https://doi.org/10.1051/mfreview/2018008  
Published online  27 July 2018 
Review
A review on the modeling and simulations of solidstate diffusional phase transformations in metals and alloys
State Key Laboratory of Solidification Processing, Department of Materials Science and Engineering, Northwestern Polytechnical University,
P. O. Box 542,
Xi'an,
Shaanxi,
710072, PR China
^{*} email: lihongwei@nwpu.edu.cn
Received:
6
March
2018
Accepted:
16
April
2018
Solidstate diffusional phase transformations are vital approaches for controlling of the material microstructure and thus tailoring the properties of metals and alloys. To exploit this mean to a full extent, much effort is paid on the reliable and efficient modeling and simulation of the phase transformations. This work gives an overview of the developments in theoretical research of solidstate diffusional phase transformations and the current status of various numerical simulation techniques such as empirical and analytical models, phase field, cellular automaton methods, Monte Carlo models and molecular dynamics methods. In terms of underlying assumptions, physical relevance, implementation and computational efficiency for the simulation of phase transformations, the advantages and disadvantages of each numerical technique are discussed. Finally, trends or future directions of the quantitative simulation of solidstate diffusional phase transformation are provided.
Key words: Solidstate diffusional phase transformation / numerical simulation / empirical and analytical models / phasefield models / cellular automata / Monte Carlo models / molecular dynamics methods
© X. Liu et al., Published by EDP Sciences 2018
This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
1 Introduction
Mechanical and functional properties of materials such as metals and alloys are largely dependent on their microstructure characteristics which include specific volume fraction of spatially distributed phases with different compositions and/or crystal structures, the size and morphology of grains with different orientations and their spatial distribution [1,2]. Due to solidstate diffusional phase transformation, which involves nucleation, growth and impingement, directly results in the arrangements of constituent phases with different grains size and morphology, it plays an important role in the production of materials with various microstructures [3]. For better control over the material microstructures and thus tailor the properties of metals and alloys, comprehensively understanding and manipulating the process of solidstate diffusional phase transformations are vital and necessary. However, during the phase transformations process, the microstructure evolution is extremely complex and nonlinear in nature because it is affected by heterogeneous grains size of parent phase, asynchronous transformation in different grains at different times, crystallographic anisotropy, thermodynamics, kinetics, and other factors [4]. Therefore, the numerical simulation techniques that can compensate for restrictions of experimental conditions and dynamically reconstruct microstructure evolution are increasingly attractive.
At present, the most advanced numerical simulation methods include empirical and analytical models [5–7], phase field models [8,9], cellular automaton models [10–12], Monte Carlo models [13] and molecular dynamics methods [14]. Empiricallybased model, which is developed on the basis of the classical JohnsonMehlAvramiKolmogorov (JMAK) theory, plays a key role in simulation and prediction of transformations including recrystallization and phase transformation where nucleation, growth and impingement mechanisms operate [15]. Different from empiricallybased model, analytical model is developed on the classical physics and phenomenological theory. In general, empirical and analytical models focus more on providing average information such as the average grain size and phase volume fraction of microstructure evolution in macroscale. By contrast, mesoscopic models including phase field models, cellular automaton and Monte Carlo models can reconstruct the evolution of grain morphology and spatial distribution, solute concentration field in addition to giving macroscopic average information [16]. The phasefield method has become an important and extremely versatile technique for simulating solidification, precipitate growth, coarsening, grain growth, martensitic transformations, dislocation dynamics, crack propagation and so on. However, the large number of difficulttomeasure phenomenological parameters in phasefield equations and the consumption of huge computing resources greatly decrease the universality of phasefield methods in engineering applications [17]. Compared with phasefield method, cellular automaton technique [18] is more feasible to characterize complex topology changes because of simplicity of formulation, excellent scalability for computer code parallelization and high computational efficiency. Nevertheless, accuracy and reliability of the simulation results for cellular automaton method strongly depend on grid partitioning and switching rules of neighboring cells. The Monte Carlo method [19] is similar to cellular automaton method about computational efficiency, but the lack of physical length and time scales makes the algorithm less attractive. In microscale and nanoscale, the molecular dynamics method is the most representative for characterizing microstructure by tracking the motion of atoms [20].
The present review provides a brief summary of the theoretical research of solidstate diffusional phase transformations and the primary numerical simulation techniques. Subsequently, by comparing these simulation techniques with each other, the advantages and disadvantages of each technique are discussed. Finally, the development directions for future investigations will be proposed.
2 State of art in solidstate diffusional phase transformations
Solidstate diffusional phase transformations represent a common phenomenon that when temperature field and other external factors change in many alloys, the diffusion of components in grains and interfaces is activated, and then the migration of interfaces takes place. This process is accompanied by nucleation, growth and impingement of new phase, changes of volume fraction and chemical composition of the individual phases, and microstructure evolution such as lamellar precipitates[21,22]. Since the microstructure determines material properties, it is of great theoretical and realistic importance to realize the accurate description of solidstate diffusional phase transformations and the precise control of the process for tailoring the properties and optimizing the hot working process of metals and alloys.
2.1 Driving force for phase transformation
During the phase transformations, there exist two typically basic processes: one is the diffusion of components in grains and interfaces responsible for the change in chemical composition, the other is the interface migration responsible for a gradual rearrangement of the lattice of the parent phase into the lattice of the product phase [21]. In many studies [23–25], the phase transformations were assumed to evolve under local equilibrium conditions, in which case the kinetics was controlled by solute diffusion. In other words, the rate of interface migration was assumed infinitely fast [26]. The classical description of diffusioncontrolled kinetics is Zener equation [27]. However, the actual lattice transformation from the parent phase into the new phase is not an infinitely fast process. Christian [28] assumed that the diffusion velocity was limitless fast and then introduced the concept of interfacecontrolled kinetics, in that case the interface velocity was proportional to the driving force. At present, the majority of analyses about solidstate diffusional phase transformations are based on one of the diffusioncontrolled and the interfacecontrolled kinetics. However, more and more studies indicate that two control modes are the extreme possibilities for the actual phase transformations [29–31]. Both the diffusivity and interface mobility are not infinite, the phase transformations will be of the mixedmode character [27]. It means that the driving force on phase interface is partially spent for diffusion and partially for interface migration.
In the following sections, the character of the solidstate diffusional transformation will be demonstrated by examples from a partitioning phase transformation of a binary alloy. Consider a binary solution consisting of two components A and B. A forms the lattice and B is the solute. This alloy has two phases that are α (product) phase and β (parent) phase. In the two phases, both the crystal structures and mole fractions of B are different. By taking a Ti–Al alloy as example, the Ti lattice has a bcc structure in βphase and a hcp structure in αphase. More Al atoms can dissolve in αphase than in βphase. The phase transformation will occur when the temperature in system decreases and thus a singlephase region (β) turns into a twophase region (α+β) (Fig. 1). Initially overall concentration of component B is given by X_{0}, X^{α,eq} denotes the concentration of component B in αphase in equilibrium with βphase. X^{β,eq} denotes the concentration of component B in βphase in equilibrium with αphase. X_{β} denotes the concentration of component B in βphase far from the interface and X_{int} denotes the concentration of component B in βphase at the interface. In general, X_{β} is assumed equal to X_{0} without taking into account the soft impingement effect. If diffusion of the solute in the growing phase α is ignored, it can be assumed that the concentration in α phase is X^{α,eq}. If the concentration of component B in parent phase and new phase are equal to X_{0}, near the interface, the kinetics of the transformation is controlled by interface migration. If the concentration of component B in parent phase and new phase are X^{β,eq} and X^{α,eq} near the interface, respectively, the kinetics of the transformation is controlled by diffusion. Actually, the phase transformation is of the mixedmode character, the concentration of component B in βphase at the interface is greater than X^{β,eq} and less than X_{0} (Fig. 2).
Following Hillert [32], the driving force for the phase transformation is equal to the change of Gibbs energy in the system before and after transformation. The change of Gibbs energy for forming per mole of α phase (Fig. 3) is (1)
The Gibbs energy is available for (a) the transinterface diffusion which means the diffusion of solute in interface, (b) the diffusion of solute in parent phase near the interface and the change in lattice . The driving force for transinterface diffusion is proportional to [33].
Svoboda [21] et al. assumed that the interface was negligibly thin relative to the grain size, and the diffusion coefficients of solute in interface were slightly larger than those in parent phase. Therefore, the diffusive fluxes in interface were supposed as practically same as in parent phase near the interface. There is no reason to expect any discontinuity of chemical potential of the solute across the interface. Thus, in the approximation of the sharp interface,
In Figure 3, it can be found that the driving force F_{chem} reaches the maximum as the concentration X_{int} of solute B is equal to X_{0} while the driving force decreases to 0 as X_{int} approaches X^{β,eq}. Hence, it is reasonable to write F_{chem} as a function of (X_{int} − X^{β,eq}). Eriksson [34] evaluated the f(X_{int} − X^{β,eq}) by thermodynamics software e.g., CHEMSAGE, and the function f is linear for a sufficiently large interval of X_{int} and X^{β,eq}. Therefore, a factor was introduced in the function, (4)
Fig. 1 Schematic representation of the partial phase diagram of a binary A–B alloy. 
Fig. 2 Planar interface migration and solution partitioning of a binary A–B alloy with initial concentration for component B [26]. 
Fig. 3 Schematic representation of molar Gibbs energy for the β→α transformation in an A–B alloy in order to derive the driving force acting on interface [32,36]. 
2.2 Nucleation of new phase
It is extremely short in time for nucleation process of the new phase, and the nucleus in nanoscale is tiny. Therefore, to directly observe and analyze the nucleation process is particularly difficult by experiments. Aiming at this problem, in the first half of the 20th century, Gibbs [35], Becker [36], Cahn and Hilliard [37,38] conducted systematic theoretical analysis for nucleation and then developed a series of nucleation theoretical models to derive the nucleation rate, activation energy barrier, size and equilibrium shape of the critical nucleus.
2.2.1 Classical nucleation theory
The classical nucleation theory is based on the assumption that the thermodynamic properties of a nucleus are uniform and the same as the equilibrium bulk counterparts within the nucleus, and that the interface between the nucleus and the parent phase is sharp [39]. In the classical nucleation theory [22], the nucleation rate is dependent on the number of critical nucleus determined by the activation energy barrier of heterogeneous nucleation and the jump frequency of solute atoms across interface which follows Arrhenius equation. Thus, the nucleation rate is [40] (5) where C is the density of nucleation sites of new phase, ω is the frequency factor, is the activation energy barrier of heterogeneous nucleation and Q_{N} is the activation energy of atomic migration across interface. The classical nucleation models include the continuous nucleation models, preexisting nuclei models, Avrami nucleation models and mixed nucleation models.
2.2.1.1 Continuous nucleation
When the undercooling or the overheating is very large, can be neglected and the nucleation rate per unit volume is only determined by the atomic mobility for transport through the interface. The nucleation rate is [41] (6)
where N_{0} is the temperatureindependent nucleation rate, Q_{N} is the activation energy for the jumping of atoms through the interface between the particle of critical size and the matrix. In this mode of nucleation, it is assumed that the nucleation rate is constant at constant temperature and the number of nuclei is zero at the beginning of transformation. The continuous nucleation often operates in the crystallisation of amorphous alloys.
2.2.1.2 Saturation by preexisting nuclei
In contrary to the assumptions of continuous nucleation, Cahn supposed that preferential nucleation at grain boundaries, edges or corners caused saturation of the nucleation sites at the beginning of transformation and the further nucleation rate is zero. The saturation of the nucleation sites is depended predominantly on the degree of undercooling or superheating. In this case, the nucleation rate is [42] (7)
where N* is the number of (preexisting) nuclei per unit volume, denotes Dirac functions and φ is the constant heating/cooling rate.
2.2.1.3 Avrami nucleation
According to this nucleation mechanism, the particles of supercritical size (nuclei) are formed from the particles of subcritical size, so the total number of particles of subcritical and supercritical size is constant [43,44]. In this case, the nucleation rate is (8)
where λ is the frequency of becoming the particles of supercritical size (nuclei) from the particles of subcritical size, which follows Arrhenius equation. N^{'} is the number of subcritical particles at t = 0.
2.2.1.4 Mixed nucleation
In practice, the nucleation process may involve a variety of different nucleation mechanisms, which is socalled mixed nucleation phenomenon. It often represents a combination of the preexisting nuclei and continuous nucleation modes. The nucleation rate is equal to some weighted sum of the nucleation rates according to continuous nucleation and preexisting nuclei [41].
2.2.2 Nonclassical nucleation theory of Cahn and Hilliard
In contrast to the classical theory, the nonclassical nucleation theory, which is developed by Cahn and Hilliard [37] firstly, is based on the diffuseinterface description of the interfaces (or gradient thermodynamics). Poduri and Chen [39] extended the nonclassical theory of Cahn and Hilliard to describe the phase transformations involving both compositional and structural changes associated with ordering. Heo and Chen [45] gave a briefly review on the recent advances in modeling and predicting nucleation during solidphase transformations based on the diffuseinterface or nonclassical description of critical nucleus profiles.
2.3 Growth of new phase
The growth of new phase in solidstate diffusional phase transformations is the migration of the phase interface in essence. According to the description from section 2.1, there exist three control modes including the diffusioncontrolled mode, the interfacecontrolled mode and the mixedmode for the migration of interface. Here, the boundary conditions for nonequilibrium interface [46] and the diffusioncontrolled and mixedmode kinetics of the growth for new phase are given as follows.
2.3.1 Interface boundary conditions
At the interface, the flux J_{α/β} of solute B atoms into the parent phase by the migration of interface is (9)
where V (t) is the velocity of the moving interface, V_{m} is the molar volume of element A in parent phase.
In the parent phase near the interface, the diffusive flux J_{diff} of solute B atoms along its gradient is (10)
Here, D is the diffusivity of solute B atoms in parent phase, L is the position of interface and is the solute concentration gradient in parent phase near the interface.
Since the solute B atoms cannot accumulate at the interface, J_{α/β} = J_{diff}. The velocity of moving interface is acquired by (11)
2.3.2 Diffusioncontrolled growth kinetics
For the diffusioncontrolled phase transformation, in equation (10), X_{int}is equal to X^{β,eq}. In order to solve the velocity of moving interface, the solute concentration gradient is prerequisite. Since the interface is moving, is extremely difficult to solve. However, the distance L(t) of interface migration is proportional to , the socalled “constantradius” approximate solution [47,48] and the exact solution of Carslaw and Jaeger [49] were proposed, which was subsequently examined by Aaron [50] et al. In a strict sense, the socalled “constantradius” approximate solution is valid only for very small supersaturation Ω (Ω < 0.1). For larger values of Ω, the exact solution of Carslaw and Jaeger is available [51].
In case of the “constantradius” approximate solution, the distance of interface migration is (12)
and the supersaturation can be write (13)
In general, X_{β} is assumed as equal to X_{0} without taking the soft impingement into account.
In a similar way, the exact solution of Carslaw and Jaeger, in which the supersaturation Ω is replaced by a parameter λ, is expressed as (14)
The parameter λ has a relation with the supersaturation Ω as (15)
Thus, the velocity of moving interface can be written as (16)
2.3.3 Mixedmode growth kinetics
For the mixedmode phase transformation, in equation (10), X^{β,eq} < X_{int} < X_{β}. In general, X_{β} is equal to X_{0} without taking into account the soft impingement. In order to solve the velocity of moving interface, not only the solute concentration gradient , but also the concentration X_{int} as a function of time t should be acquired. To tackle the evolution problem of solute concentration field in parent phase near the interface, Sietsma [26] et al. introduced a Zenerlike approach and Svoboda [21] proposed an analytical technique by developing a finite difference numerical method.
In the Zenerlike approach, Sietsma et al. assumed the concentration gradient was constant and concentration gradient field extended over a distance l into the parent phase. Thus, (17)
When the interface migrates to the position L, the new phase forms with a volume V^{α} and an interfacial area A^{α}. On account of conservation of Batoms at the interface, (18)
According to Christian [52], the interface is proportional to the driving force
V (t) = MF_{chem}.(19)
Here, M is the effective interface mobility with taking the effects of solute drag or transformation strain into account.
By substituting (4) into (18), plugging (16) and (17) into (10), and then combining (18) with (10), the concentration X_{int} will be acquired that (20)
with ΔX_{β} = X^{α,eq} − X_{β}, the parameter Z is given by (21)
According to Svoboda [21], the evolution of the interface is governed by the following system of equations: the bulk diffusion equation (22)
and the initial condition is (23)
By combining (4),(10) with (18), the boundary conditions at the phase interface are obtained as (24)
For the differential equation (21), by considering the boundary initial conditions (Eq. (23)), a nonlinear Volterra integral equation is derived for the mole fraction X_{int}, which is simplified as (25)
By plugging (24) and (4) into (8), the velocity of moving interface is (26)
2.3.4 Impingement of grains in new phase
For the phase transformations that proceed by the formation of nuclei and the growth of these nuclei, it is impossible that a new phase grows into its parent phase without any limit. In other words, the collision process between two growing neighboring grains is inevitable, which results in obstructing growth of the neighboring grains. It is socalled impingement phenomenon. In general, two impingement modes may occur. One is the hard impingement considering only the geometric factor, and the other is the soft impingement involving a compositional change. In the case of soft impingement, when the diffusion fields start to overlap, the phase transformation will slow down [53,54]. However, for the solidstate diffusional phase transformations, soft impingement has been found to prevail, and there usually are wide diffusion layers around the growing nuclei impinging on each other [55,56]. Initially a mean field approximation [27,57] was used to take into account the soft impingement effect in the diffusioncontrolled growth models. However, it is available for mean field approximation in an assumption that a nucleus grows in isolation, which doesn't consider any effect of the neighboring nuclei on the diffusion field. Subsequently, to deal with the overlap of diffusion fileds for the neighbouring grains in more strict ways, many diffusioncontrolled models [58,59] and mixedmodes models [60,61] have been developed to describe the soft impingement effect more accurately.
3 Numerical simulation techniques for solidstate phase transformation
3.1 Empirical and analytical models
In studies of solidstate diffusional phase transformations involving nucleation, growth and impingement, the classical empirical and semiempirical models, such as JohnsonMehlAvrami Kolmogorov (JMAK) approach [52,62] or modified JMAK approach (JMAKlike equations) [63,64] and physical analytical models (for example, ZenerHillert equation, the thermal activation principle of interface of Christian), always play important roles. The years 1937 through 1941 mark an important period in the history of metallurgy. In these years, Johnson and Mehl, Avrami, and Kolmogorov derived expressions for the transformed fraction f as a function of time t in the isothermal transformations [43,65]. The famous JohnsonMehlAvrami Kolmogorov (JMAK) equation is (27)
but the JMAK formula can only be validated when the auxiliary conditions imposed in the original equation are not violated, such as: either pure site saturation at time t = 0 or pure continuous nucleation, large undercooling or overheating for forming high driving force, and randomly dispersed nuclei which grow isotropically [65,66]. In other words, the growth exponent n, the effective activation energy Q and the preexponential factor k_{0} are constant relative to time and temperature. By introducing additivity rule into the original JMAK equation, the application the JMAKlike equation was extended to the nonisothermal transformation. However, the kinetic parameters remain constant [67], which follows so called “isokinetics”. In practice, due to nonrandom distribution of nuclei [68], anisotropic growth [69] and the temperature dependence of the diffusion coefficient and the solute concentration at interface [7], these models which follow so called “isokinetics” are invalid for solidstate diffusional isothermal or nonisothermal phase transformations. Recently, since Cahn [70] first proposed the modified JMAK model with considering nucleation in grain boundary, edge and corner, lots of modified JMAK models by introducing the transient nucleation [71], the spatially correlated nucleation [72], the mixture of nucleation modes, the necessarily associated sizedependent growth [73] or the nonparallel anisotropic growth [74], and the hard or soft impingement, were derived. Shneidman et al. [75] developed a modified JMAK model by considering the effects of transient nucleation, sizedependent growth rate and their correlativity. Tomellini [76] introduced the impingement factor into the JMAK equation to tackle two processes: spatially correlated nucleation with constant nucleation rate and instantaneous cluster growth where cluster overgrowth prevails. By considering variable kinetic parameters (i.e., n (t), Q (t), k_{0} (t) for isothermal case; n (T), Q (T), k_{0} (T) for nonisothermal case) and the mixture of site saturation, continuous nucleation and Avrami nucleation, Liu et al. [77] proposed a general, flexible and modular analytical model, which expounded the influence of the different nucleation and growth modes on the time and temperature dependencies of the transformation rate and the kinetic parameters. For the treatment of the anisotropic effect, up to now, there exist two approaches : one is the phenomenological extension of JMAKlike formulation by adding (one or more) new variables which provide freedom to improve the agreement where anisotropic growth occurs [15], the other is devoting more attention to the derivation of analytical description with physically realistic variables (e.g. the growth rate anisotropy and the orientation) according to the physical essence of anisotropic effect [78]. In order to describe the mutual blocking of growing particles determined by all relevant orders due to the anisotropic effect, Kooi [74,79] developed an analytical model based on Monte Carlo (MC) simulations by incorporating anisotropic growth into the JohnsonMehlAvramiKolmogorov models. With respect to the effect of the thermal history, Song [80] proposed a generalized isokinetics conditions and additivity rule involving the thermal historydependent instantaneous reaction rate by introducing a thermal historyrelated function. So far, a proper analytical approach in the spirit of JMAKlike theory, which can comprehensively consider the different modes of nucleation, growth and impingement, the interactions between nonrandomly dispersed nucleation and anisotropic growth (involving single grain or multiple grains) in solidstate phase transformation, has not yet been developed. In physical analytical models, ZenerHillert [81] equation established the theoretical foundation for the diffusioncontrolled growth kinetic of lamellar phase. Subsequently, Ivantsov [82], Horvay and Cahn [83] derived a more generally applicable equation with taking into account the ellipticparabolic or spherical surface for the tip of new phase. Trivedi [84] introduced the capillary phenomenon and interface dynamics into the equation of Ivantsov. Since the anisotropic effect of strain energy, diffusion and crystallography were not considered, these models were still incompetent to predict solidstate diffusional phase transformations accurately. Over all, much effort still should be paid to study the kinetic models of solidstate diffusional phase transformations with integration of different factors and involving structure evolution.
3.2 Phasefield models
The phasefield approach has emerged as an important and extremely versatile technique for simulating microstructure evolution at the mesoscale level. Initially, the phasefield models were used to simulate dendrite formation in solidification process. Subsequently, with the increasing computer power, the applicability of phasefield models was extended to solidstate transformations, grain growth, dislocation dynamics, crack propagation, electromigration and solidstate sintering and so forth [17].
In the conventional modeling techniques for phase transformation, the regions separating the compositional or structure domains are treated as mathematically sharp interfaces and the multidomain structure is described by the position of the interfacial boundaries(Fig.4(A)). These models are also called sharpinterface models. The local interfacial velocity is determined by part of boundary conditions or the driving force on the interface. Due to these approaches involve explicit tracking of the interface position [17,85], it becomes difficult to simulate complex microstructure in twodimension or threedimension. Therefore, the phasefield modeling, which is able to predict the evolution of arbitrary complex grain morphologies without any presumption on their shape or mutual distribution and explicitly tracking the of the interface position, is very popular. The principal characteristic of phasefield model is the diffuseness of the interface between two phases, so it is sometimes also called diffuse interface models. The view of diffuse interface dates back to van der Waals [86] and Cahn & Hilliard [37]. Chen, Wang, and Khachaturyan [87,88] is first to introduce the diffuseinterface(Fig.4(B)(B)) into solidstate phase transformation modeling. About the historical evolution of diffuseinterface models and the basic concepts of phasefield models, Moelans [17] gave a comprehensive introduction. In phasefield models, the transformation is described by the temporal and spatial evolution of a set of conserved (for concentration field) and nonconserved (involving information on local structure and orientation) field variables which are continuous across the interfacial regions separating the neighboring phases or structures. The evolution of these field variables are governed by the CahnHilliard nonlinear diffusion equation [37,38] and the time dependent GinzburgLandau relaxation equation [89,90].
In solidstate diffusional phase transformation, microstructures have the thermodynamically unstable features. The driving force of the temporal and spatial evolution of the microstructure usually consists of a reduction in the bulkchemical free energy (F_{bulk}), a decrease of the total interfacial energy (F_{int}) between different phases or between the neighboring grains with different orientation in the same phase, the relaxation of the elasticstain energy (F_{elast}) generated by the lattice mismatch and external energies (F_{appl}) due to applied stress, temperature, electrical, and magnetic fields and so on [91]. Thus, the total free energy of a system is (28)
In phasefield models, the total free energy [92] described by a set of conserved (c_{1}, c_{2}, ⋯) and nonconserved (η_{1}, η_{2}, ⋯) field variables can be written as (29)
where f is the local freeenergy density, α_{i} and β_{ij} are the gradient energy coefficients. The evolution of conserved and nonconserved field variables can be obtained by solving the following the CahnHilliard nonlinear diffusion equation [37] and the GinzburgLandau relaxation equation [90], (30) (31)
here, M_{ij} is related to the mobility of atom or interface and L_{pq} is the symmetrical matrix of dynamic structural operator related to the nonconserved field variables. Therefore, in phasefield models, to accurately describe the microstructure evolution in solidstate diffusional phase transformation including nucleation, anisotropy growth, hard or soft impingement needs to establish the appropriate correlation functions of the field variables and the phenomenological parameters for reflecting aforementioned effects.
In recently, many phasefield models, incorporated with nucleation phenomena [93–95], anisotropy effects [96–99] and elasticity/plasticity [100–104] and macroscopic behaviours [105], have been proposed for better quantitatively predicting the microstructure evolution in solidstate diffusional phase transformations. Zhang, Chen and Heo [96] developed a phasefield model combined with the minimax technique to predict the morphology of critical nuclei during solidstate diffusional phase transformation in both two and three dimensions, which took into account the anisotropic interfacial energy as well as the anisotropic longrange elastic interactions. Then, by incorporating with diffuseinterface critical nuclei in phasefield simulations through the explicit nucleation algorithm, the temporal growth kinetics of the introduced nuclei were obtained [95]. Mecozzi et al. [106] have successfully performed two and threedimensional simulations of a grain growth during austenitetoferrite transformation by the multiphasefield (MPF) method, where the interfacial energy and mobility of all interfaces were assumed to be constant. Because the nucleation typically takes place on a much smaller length scale than the further growth of new phase, as above, lots of phasefield models can only be used to study the one of nucleation or growth. To sample frequently enough to observe nucleation would require an impractically large number of integration cycles to be performed in order to observe growth kinetics in real alloys, Simmons et al. [107] introduced a Poisson seeding algorithm into the Phase Field equations instead of the Gaussiandistributed Langevin noise terms for simulating nucleation. Wang [108] used the quantitative phase field method to study the concurrent nucleation and growth in a diffusioncontrolled phase transformation. However, in their works the growth behavior and morphology of simulated grains are isotropic, which is unrealistic in actual phase transformation. Therefore, a series of phasefield models, integrated with the anisotropy growth, have been developed. Yamanaka [109] used a multiphasefield model with considering the dependence of the interfacial energy and mobility on phase and crystal orientation to simulate growth of the ferrite. Wei [97] used the Loginova phasefield model with introducing a highly anisotropic function related to the anisotropy strength of the interfacial energy and interface thickness, and the KimKimSuzuki (KKS) phasefield models [S.G. Kim, W.T. Kim, T. Suzuki Phys. Rev. E, 60 (1999), pp.7186–7197] with a thin interface thickness which could enlarge the simulation domain to a large dimension, to simulate the growth of widmanstatten ferrite from grain boundary allotriomorphic ferrite with perturbed interface during isothermal austeniteferrite transformation. In addition, the effect of elasticity/plasticity resulted from elastic or even plastic deformations should not be neglected. Recently the phase field models, containing the description of elastoviscoplastic material behaviour of the phases combined with diffusion and phase transformation, can be classified into two main groups of theories [110–112]. One is the interpolation models relying on a single set of constitutive equations and interpolation of material parameters, the other is the homogenization models based on the mixture of free energy and dissipation potentials associated with distinct behaviors of the phases. These models have been applied to study the mechanical effect on the diffusioncontrolled growth of the precipitates.
Furthermore, for complex multicomponent systems, the phasefield models coupled with thermodynamic and kinetic databases were developed to put more physics into the expansion of the free energy function in the GinzburgLandau equation. Steinbach [113] discussed details of a direct coupling between the MultiphaseField method and the CALPHAD method and used the CALPHAD −coupled PhaseField model to simulate solidification microstructure formation in Nibase superalloys. Wang et al. [114] presented a MultiphaseField model with inputs from CALPHAD thermodynamic and DICTRA kinetic databases and simulated the growth and dissolution of a precipitates in Ti–Al–V on experimentally relevant length and time scales.
In addition, a number of the phasefield simulations for solidstate phase transformations have been conducted in threedimensions (3D). In the complex phase transformations, due to that the twodimensional (2D) models cannot simulate the basic microstructural features, the threedimensional (3D) simulations which show a realistic representation of the actual microstructure become more atrractive. M.Militzer [115] used the phase field method to simulate the austenitetoferrite phase transformation in steel in threedimensional (3D) space. It was found that the effect of the exact morphology of the initial 3D austenitic microstructure on the kinetics was shown to be small and threedimensional (3D) simulations predict slower transformation rates compared with twodimensional (2D) simulations. Cui [116] developed a threedimensional, nonisothermal phasefield model to systematically investigate the interactions between the temperature, stress, and microstructure fields in shape memory alloys.
As previously mentioned, the phasefield model exhibits the tremendous capability of quantitatively predicting the complex microstructure evolution in solidstate phase transformation. However, for phasefield models [17], there are two major difficulties in achieving more precise quantitative description of the real phase transformation with the coexistence of different nucleation modes, mixed growth mode, anisotropy growth, impingement effect and elasticity/plasticity effect. First, phasefield models contain a great many of phenomenological parameters related to the thermodynamic properties, phase composition, the interfacial structure, the diffusion of solute elements, and the elastic/plastic properties of the coexisting phases. Most of these parameters are difficult to measure. Second, in actual, the width of the interface is several orders smaller than the microstructure features such as grains and precipitates, so massive computer resources will be consumed by resolving the evolution of phasefield variables at the interface and also covering the system with realistic dimensions. Aiming at the problem of excessive computation times and insufficient computer memory, using interface field [117] especially adaptive grids providing a local remeshing at the interface have turned out to be beneficial [118]. For solidstate phase transformation, the Fourierspectral method with semiimplicit time stepping is usually more appropriate than the technique based on adaptive meshing on account of a large number of grains or precipitates involved [119]. However, these computing techniques are either limited by the number of CPU cores or are too intractable to implement in threedimensional simulations. Thus, the GPUbased parallel computing technology is extremely attractive in scientific computation owing to the GPU's massive computation capacity and high memory bandwidth. In the past few years, many researchers have successfully applied the GPU parallel computing algorithm into twodimensional or threedimensional phasefield simulations of dendrite growth [120,121]. To increase the system size towards relevant dimensions, the width of the diffuse interface must be taken artificially large. Much effort has been made in developing phasefield models that allow changing the interface width without affecting interfacial properties or introducing spurious effects [17]. However, a general solution has not yet been found. Therefore, there will still be increasing efforts to develop the more powerful and feasible largescale threedimensional (3D) phasefield model.
Fig. 4 (A) Sharp interface: properties are discontinuous at the interface; (B) Diffuse interface: properties evolve continuously between their equilibrium values in the neighboring grains[17,36]. 
3.3 Cellular automaton models
Cellular automata are synchronous algorithms, first introduced by von Neumann in 1963, and later on in 1986 by Wolfram to a broader scientific public, which describes the discrete spatial and temporal evolution of complex system by applying local (or sometimes midrange) deterministic or probabilistic transformation rules to the cells of a regular (or nonregular, random) grid with local connectivity [122,123]. Since Hesselbarth [123] et al. used the cellular automaton approach for the simulation of recrystallization, in the past several decades, it gradually becomes very promising and popular for simulating the microstructure evolution due to its computation efficiency, flexibility in multiscale bridging, and physical consistency. Cellular automaton method has been successfully performed in two or threedimensional modeling and simulations of dynamic and static recrystallization [124,125], grain coarsening [126], solidification [126], solidstate phase transformation [127], microshear band and shear band propagation [128], cracks propagation [129], etc. It provides a deeper insight into the mechanism and morphological complexity of them without timeconsuming solution of complicated partial differential equations. So far, all these models can be classified into several main groups that referred as the classical cellular automaton, frontal cellular automaton [130], irregular and shapeless cellular automaton [131], and virtual front tracking model based on cellular automaton [132].
In the classical cellular automata, take the twodimensional model as an example, the entities of the automaton are the types of the neighboring cells (Fig. 5), the state variables of cells in space evolving with time and cell status update rules without any restrictions [133]. A cellular automata simulation for complex microstructure evolution proceeds by discrete simulation steps (namely discrete time steps) consisting of the computation of the new states (t_{0} + Δt) of the all cells based on their current states (t_{0}), which can be presented as the following function with Moor configuration in twodimension, (32)
where is the value of the state variable of the cell (i, j) at the time t_{0}, and the function f specifies the set of transformation rules which determine the updated state of a cell based on the cell's previous state and the states of all cells in the local neighborhood of that cell. Besides, some conditions at the outer boundaries of the grid such as periodic, reflexive or fixed grid are applied in order to study the infinite target domain by simulating a finite representative region.
The most of cellular automata models, which can be found in literature, are twodimensional(2D). 2D cellular automata models are simpler and faster in calculation in account of having less elements, connections and complicated algorithms. However, microstructure evolution is pointedly threedimensional phenomena, the results obtained by 2D cellular automata models cannot always be directly transferred to a real 3D process [130]. Therefore, 3D cellular automata models attracted a growing number of researches[134,135]. Due to more cells in simulated domain and more neighbours for each cell relative to 2D models, the 3D models require significantly more memory and time for the calculation, which increases the difficulty in accurately predicting real microstructure evolution.
During the implementation of the classical automaton models, some problems and aspects needing to be improved have been encountered. One of the most significant is the inherent and artificial anisotropy introduced in the computations by the mesh of squared cells, which causes that the preferential growth directions of all the simulated grains are aligned with the mesh axis or at 45 degree and thus leads to the growth kinetics without physical significance. For the problem, Stefanescu et al. [127] developed a cellular automaton model coupled with virtual interface tracking scheme (Fig. 6). In this model, the procedure of constructing virtual sharp interface for capturing new interface cells in a time step is as follows. First, for all interface cells, the length L_{ϕ} dependent on the local growth angle φ is assumed equal to f_{s} = 1 (new phase fraction f_{s}) and measured from the interface cell center along the normal direction of the local interface, which can be written as (Fig. 6(A)) (33)
here cells size is Δx. The position of the new interface at time t+Δt can be gauged from the interface cell center along the normal direction of the local interface at a distance proportional to the f_{s} in one cell. And the entire virtual sharp interface at time t+Δt will be described by connecting the position of new interfaces in all interface cells. Second, the parent phase cells, found inside the area surrounded by the entire virtual sharp interface, are considered captured and will become new interface cells (Fig. 6(B)). Subsequently, after capturing the new interface cells and then updating the state variables, the procedure is repeated again in the next time step.
Another problem is that interface energy and mobility relies on its curvature which is dependent on the orientation of the interface surface, meanwhile, the method of using the symmetrical grid to discretize the surface in such a way that only a very limited number of orientations are represented cannot resolve curvature [131]. For this problem, Janssens et al. [136] first presented the random grid or irregular cellular automaton based on Voronoi cells to solve this problem by local variation of the cell lattice geometry (Fig.7 (A)). Afterwards the shapeless or point cellular automata were developed from the random grid or irregular cellular automaton by Janssens. In this model, shapeless cell shapes are not computed explicitly and only a point position is used, which makes much more flexible in definition of neighborhood (Fig.7(B)).
In addition, no cell state is actually changed until the end of the solution step when the states of all cells are updated simultaneously in the classical cellular automata, which directly influences the calculation time. Much effort has been focused on developing modified cellular automaton models allowing for significant acceleration of the calculation especially in the threedimensional tasks. In order to only consider the small area near the front of moving interface for growing grains from the calculations in the current step, Svyetlichnyy [137,138] presented the FCA (frontal cellular automata) algorithm. FCA consists of a complex of the millions of cells with the same multistates automaton (Fig. 8). The series of automaton states includes the initial matrix state q_{0}, the frontal cell q_{1}, the boundary cell q_{2}, the cell inside the grain q_{3}, the transient state q_{4} accompanied with calculation of the time delay, nucleation state q_{5}, the cell in the edge of the grain q_{6}, and the cell in the corner of the grain q_{7}. Besides, some conditions used by transition rules respectively are the nucleation condition I_{0}, the time delay condition I_{1} which controls grain growth or mobility of interface, the conditions I_{2} and I_{3} which determine nucleus location (on grain boundary, inside the grain, in the edge or corner of the grain), and state change condition I_{4} which refers as that neighboring cells transits from the states q_{2}, q_{3}, q_{6}, q_{7} into the transient state q_{4} for all neighbors of all frontal cells. For the phase transformation, in FCA, the initial states of the cell before transformation can be arbitrary (q_{1} − q_{7}), and then the conditions (I_{1} − I_{7}) are responsible for the transformation. The boundary conditions such as periodic displacement conditions and full open conditions are usually used. Relative to the classical cellular automata, the most advantage of FCA is found out allowing for recognition of the changes in cells state without studying their neighborhood.
In the formulation of cellular automaton models for solidstate diffusional phase transformation, each cell represents a volume of real material characterized by certain attributes with a distinct phase or grain, solute concentration and an orientation indictor. There are several state variables with describing certain attributes used on each cell in phase transformation such as the phase state variables, the solute atom concentration variables, the orientation variables, the velocity and displacement variables of the moving interface, and volume fraction variables. The cellular automaton will be in progress by synchronously updating these state variables for all lattice cells in each time step, and thus spatial and temporal microstructure evolution is described. In recently, many cellular automaton models for solidstate diffusional phase transformation have been developed to focus on simulating the austeniteferrite phase transformations in Fe–C alloy in which interstitial solute carbon atoms have high diffusion coefficient[139–141]. However, as regard to substitution solid solution like FeMn or Ti–Al–Mo alloy, the attractive force occurs from the solute atoms on the moving interface, which is socalled solute drag without existing in interstitial solid solution. According to Cahn [138], the solute atoms have different drag effects in three regimes of the interface velocity. Therefore, the effects of solute drag for solidstate phase transformation in substitution solid solution cannot be neglected. Furthermore, in most of these models, the growth behavior and morphology of simulated grains were assumed to be isotropic [141,142], which was not correspondent with practice. Besides, because the nucleation typically takes place on a much smaller length scale than the further growth of new phase, as with the phasefield models, the cellular automata is not able to simulate the process of different nucleation modes and mixed growth mode occurring in sequence. And last but definitely not least, above mentioned models, the phase transformation is supposed to happen with only the diffusioncontrolled or the interfacecontrolled kinetics in the isothermal condition without considering the effect of the thermal history. A cellular automaton model [143] coupled with Svoboda's analytic solution of diffusional phase transformation was established to divide the diffusion, mixed or interfacecontrolled transformation in isothermal and nonisothermal processes. However, due to the critical conditions could not be obtained as a result of the difficulttomeasure constant factor in the driving force model, and due to only taking into account the cooling ratedependent transformation temperature, the cellular automaton model was not enough to simulate the actual nonisothermal transformation. All in all, much effort should be focused on improving the cellular automata models for better modeling and simulation of the solidstate phase transformation in the future.
Fig. 5 Neighboring type in cellular automata: (A) von Neumann configuration; (B) Moor configuration. 
Fig. 6 Illustration of (A) determining the position of sharp virtual interface, and (B) capturing rules for new interface cells [127,134]. 
Fig. 7 Illustration of (A) cells distribution in a twodimensional irregular cellular automata based on the Voronoi cells, and (B) a shapeless cell on a curved interface and its spherical neighborhood [121]. 
Fig. 8 Illustration of FCA (frontal cellular automata). 
3.4 Monte Carlo models
MC models were developed from Ising and Potts models of ferromagnetic systems used in statistical physics [144]. Initially they were used to simulate grain growth by Anderson et al. [145], after that they have been widely used to model the microstructure evolution in materials such as the recrystallization and the phase transformation. In Monte Carlo models [146], space is discreted into a set of lattice points onto which a continuum microstructure is mapped at a length scale above that of atoms and below that of grains, similarly to the probabilistic cellular automaton models. The grain boundaries are defined as existing between lattice sites of neighbouring grains. The energy of the system is represented by a Hamiltonian which sums the interfacial energy of the system. The Monte Carlo models simulate curvaturedriven grain boundary motion by the random movement of kinks (2D) or ledges (3D) along the grain boundaries controlled by the transition rules. Due to the calculations of grain boundary curvature and energy are ambiguous and the transition rules governing the change of voxel state are often not physically justified, the physical meaning of units of length, time and energy in Monte Carlo models is often unspecified [147]. Nonetheless, the numerical implementation is straightforward and decent computational efficiency can be achieved in the Monte Carlo models, especially since the algorithm is very suitable for parallelization, the Monte Carlo models are still frequently used to model the complex microstructure evolution in materials.
3.5 Molecular dynamics methods
Molecular dynamics simulation serves as an essential technique for the investigation of fundamental atomic behaviors in metals and alloys, which was developed by Alder and Wainwright in the late 1950s [148]. It has facilitated scientific discovery of interactions among particles or atoms since molecular dynamics method allows us to examine the varying atomic configurations at finite temperatures by incorporating statistical mechanics [149]. The molecular dynamics methods simulate microstructure evolutions from the atomistic point of view by solving the particle trajectories derived from the interatomic forces. Numerical integration of atomic motion is carried out on the interatomic forces, which results in the particle velocity. The velocity of the particles follows the Maxwell–Boltzmann distribution, which is temperature dependent. Then, the particle position is obtained by further integrating the velocity. Molecular dynamics methods have evolved as the powerful tool to investigate the mechanisms of physical phenomena such as nucleation, and nucleus growth which are difficult to observe experimentally [14], [150].
4 The comparison of different numerical simulation techniques
As above, the theoretical researches of solidstate diffusional phase transformations and the primary numerical modeling techniques are discussed. All these phase transformation models characterized by complex mathematical formulations present various predictive capabilities. In the following, the advantages and disadvantages of each modeling technique will be discussed in terms of the underlying assumptions, physical relevance, implementation and computational efficiency for the simulation of the solidstate diffusional phase transformations.
Historically, the classical empirical and semiempirical models represented by JohnsonMehlAvramiKolmogorov (JMAK) approach were commonly used for simulations of phase transformations. The JMAK formula are valid only in conditions of either pure site saturation at initial moment or pure continuous nucleation, large undercooling or overheating for forming high driving force, and randomly dispersed nuclei which grow isotropically. In these models, all attention is focused on the kinetics while the microstructural aspects are essentially ignored, and thus its only provide average information such as the average grain size and phase volume fraction of microstructure evolution on macroscale. Afterwards, several upgrades of the model with integration of the mixed nucleation modes, anisotropic growth, and the hard or soft impingement effects were proposed. Much effort has been paid on developing the models involving structure evolution, and the approach is still commonly used. Compared with the JMAK approach, the phase field models and the cellular automaton models can reconstruct the evolution of grain morphology and spatial distribution, solute concentration field in addition to giving macroscopic average information.
The phasefield modeling is a mechanisticbased microstructure modeling method, in which phenomenological character and the equations for the evolution of the phase field variables are derived based on general thermodynamics and kinetics principles. It can predict the evolution of arbitrary complex microstructure without any presumption on their shape or mutual distribution and explicitly tracking the of the interface position, meanwhile, provide an insight into controlling mechanisms in solidstate diffusional phase transformations [151,152]. Because a large number of grains or precipitates are involved in solidstate diffusional phase transformation, the Fourierspectral method with semiimplicit time stepping and uniform mesh is usually more appropriate than the technique based on adaptive meshing in phasefield models [17]. However, the phasefield models contain a large number of phenomenological parameters related to the thermodynamic properties, the phase composition, the interfacial structure, the diffusion of solute elements, and the elastic/plastic properties of the coexisting phases, meanwhile, most of these parameters are difficult to measure. Besides, the phase field simulations are more computationally intensive than the JMAK approach and the cellular automata.
Relative to the classical empirical models and the phasefield models, the cellular automata models are more easily implemented without solving complex partial differential equations and its can be used to capture many aspects of the microstructure physics in solidstate diffusional phase transformation. Since the discrete nature of the algorithms is well suited for parallelization, the cellular automaton methods possess the high computational efficiency. However, a precise calculation of the mean curvature which is necessary for grain boundary migration by capillarity remains difficult [98]. Moreover, due to the sharp interface in the cellular automaton models, compared with the phasefield models with the diffuseinterface, the cellular automaton approach is less than accurate to predict solidstate diffusional phase transformation. Besides, limitations of the cellular automata also lie in the dependence on the underlying solution grid and the types of the neighboring cells. In addition, for solidstate diffusional phase transformations, the time step in the cellular automata simulation is virtual or defined as e.g., the ratio between the cell size and maximum interface velocity, or a scaled ratio between the average cell size and the average interface velocity, which is deficient in physical meanings [153].
The Monte Carlo model as usually is very similar to the probabilistic cellular automata model in terms of implementing. Both models describe the discrete spatial and temporal evolution of complex system by applying local transformation rules to the grids with local connectivity. The differences between them lie in the transition rule and the method of updating the state of each cell [154]. In the Monte Carlo models the transition rule is determined by the reduction in local free energy, whereas the cellular automata model is more flexibility to adjust the transition rule for matching kinetics of a particular experimental system. Therefore, the Monte Carlo simulations lack physical length and time scales, and the results are difficult to match to experiment. In the Monte Carlo models sites are chosen at random for updating, whereas in the cellular automata models all sites update simultaneously. Thus, the cellular automata models are generally more efficient than the Monte Carlo models.
The phasefield models, the cellular automata models and the Monte Carlo models in mesoscale allow the simulation of a relatively large representative volume element that can be composed of thousand to million grains. However, the effects and physical mechanisms are predefined and preimplemented in these models, it is impossible for them to resolve the mechanisms of phenomena acting at the atomic scale. In this case, the molecular dynamics simulations are utilized to describe atomic interactions to make up for the disadvantage of mesoscopic models. Compared to these mesoscopic models, the representative volume element that can be simulated by the molecular dynamics models in a reasonable time is very limited, which occasionally results in insufficient statistical representativeness and undesired effects of the size of the simulated volume [155]. With increasing computational power, large scale atomistic simulations can be conducted with several million or even billion atom systems, e.g. into studying phase transformation kinetics [156], deformation and fracture in metallic systems [157].
5 The future prospects
Although various numerical simulation techniques as above have been successfully used to describe the solidstate diffusional phase transformations, there will also be increasing efforts in the accuracy and efficiency of models. The new trends or future directions for the simulation of solidstate diffusional phase transformation will be expected.
5.1 Integrating the nucleation phenomena (mixedmodes, nuclear morphology)
Nucleation of the new phase typically takes place on the much smaller length scale than the subsequent growth of nucleus and it is generally extremely short in time for nucleation process. Moreover, in practice, the distribution of nucleus is not random and there are various nucleation phenomena. It have been found that the nucleation was either related to time like transient nucleation and continuous nucleation, or correlated with space like nucleation in grain boundary, edge and corner at parent phase. In addition, the morphology of the critical nucleus is very complicated by additional contact angle conditions for nucleation occurring at the planar defects. The existing models on mesoscopic scale can only describe a single nucleation mode with ignoring the morphology of nucleus, and thus it is not feasible to consider both the nucleation and the growth at the same time for these models. However, many models represented by the molecular dynamics on microscopic scale and nanoscopic scale are benefited to accurately capture the grain boundary energy and interfacial energy and predict the geometry of the nucleus by tracking motion of atoms. Therefore, future efforts are expected to be focused on coupling between mesoscopic simulation and microscopic or nanoscopic calculations for complex nucleation phenomena in solidstate diffusional phase transformation.
5.2 Incorporating with the anisotropic effect
In general, the fundamental process underlying the microstructure evolution in solidstate diffusional phase transformations is the migration of interface or growth of new phase in a broader sense. The kinetics and morphology of grains growth in new phase are determined by the properties of interfaces such as the anisotropic interfacial energy and mobility. Anisotropy of the interfacial energy and mobility reflects the atomistic crystallographic structure of interfaces, meanwhile, the lowenergy interfaces structures leads to the faceted interface as well. At present, many findings allow to make a rough estimate successfully for the anisotropic grain boundary energy in case of the same lattice structure and composition. However, with respect to the interfacial energy, the effects of lattices structure and chemical composition also remain largely unexplored and the anisotropy of interfacial mobility is difficult to measure, which make it impossible to accurately predict anisotropic growth of grains in new phase.
5.3 Introducing the hard or soft impingement effect
In general, for the phase transformation consisting of nucleation and growth, the collision process between neighboring grains is inevitable. When the impingement occurs, with decreasing of the distance between the edges of neighboring grains, the diffusion fields start to overlap, at the same time, the concentration gradient becomes more flat, the growth rate is predicted to decrease locally and thus the phase transformation slows down. In that case, the growth law cannot be considered as given a priori before collision process since it is a function of the local environment of each grain. However, at present, due to the lack of knowledge on the exact nature of diffusion layers for the hard and soft impingement, the collision process between grains described in the existing models is now less effective than the genuine impingement process.
5.4 Considering the thermal history
In the past few decades, various analytical models have been successfully developed to predict the nonisothermal transformations process with the use of the additivity concept in the isokinetic condition. The conventional additivity rule is only valid in the assumption that nonisothermal transformations process is described as the summation of a series of short period isothermal transformation process, which implies that the instantaneous reaction rate only depends on the current state of every short period isothermal transformation process. However, in practice, the diffusion field around new phase during nonisothermal transformation has an intrinsic memory of the thermal history as a result of the temperature dependence of the diffusion coefficient and the local equalized solute concentration at the interphase boundary, which leads to a temperature pathdependent instantaneous growth rate. Therefore, most of analytical models introduced the conventional additivity rule usually overestimate or underestimate the measured extent of precipitation reactions. At present, for more accurately predicting solidstate diffusional phase transformations, there has been increasing efforts to be spent on creating the thermal historyrelated function, and developing a generalized additivity rule which involves the thermal historydetermined instantaneous reaction rate.
5.5 Coupling with macroscopic deformation
Solidstate diffusional phase transformations are always not immune to the effect of the elastic deformation and plastic deformation such as the stored energy, the dynamic and static recrystallization, the globularization and the deformation heating and so on during the metal forming process. When the solidstate phase transformation takes place after the elasticplastic deformation, in other words, the deformation is applied in singlephase region at high temperature or in twophase region with isothermal conditions and then the cooling treatment is performed at given rate. The stored energy is the main factor for contributing to the driving force of the phase transformation. However, if the solidstate phase transformation process operates simultaneously with deformation, not only the stored energy, the dynamic and static recrystallization, the globularization and the deformation heating have significant influences on the kinetics and crystallography (orientation relationship, morphology) of phase transformation, but also in turn the changes of the volume fractions of constituent phases and grains morphology on the mesoscale affect the deformation resistance on the macroscale. Up till now, due to lack of knowledge on the exact mechanism of the interaction of phase transformation and deformation, few investigations are performed on modeling the phase transformation coupled with macroscopic deformation.
5.6 Improving computational efficiency and accuracy for quantitative simulation
Numerical simulation can provide the important insights into the role of special material or process parameters on the volume, shape and spatial distribution of new phase, orientation relationships between new phase and parent phase, or kinetics in solidstate diffusional phase transformation. However, the more versatile and feasible technique for quantitative predicting the microstructure evolution is required both the high computational efficiency and the accuracy for the numerical solution. As is known to all, the more accurate solution of details of the microstructure evolution requires the finer mesh. In contrast, the coarser mesh is more benefit to the high efficient calculation. For the phasefield models, a finite volume or finite element discretization based on adaptive meshing which provides a local remeshing at the interfaces, or artificially enlarging the width of the diffuse interface is often applied to improving the accuracy of simulation quantitatively and the computational efficiency. However, the problem of excessive computation times and insufficient computer memory is still not solved with the use of these methods. For the cellular automaton models, it is more easily implemented without the excessive computation times and solving complex partial differential equations. However, once coupled with the finite element simulation on macroscale which provides the macroscopic information for the cellular automaton models, huge amounts of computational resources will be consumed by the numerical solution of the coupled system. Although a series of powerful parallel algorithms are developed to improving the computational efficiency, it is still difficult for the cellular automaton methods to simulate the microstructure evolution with a more fine mesh for accurate solution of details as a result of unreasonable computation time and inadequate computer memory.
6 Conclusions
The modeling and simulation of the solidstate diffusional transformations in metals are reviewed and the results may be summarized as follows:

The traditional diffusioncontrolled and interfacecontrolled modes fail to correctly describe the growth kinetics of new phase over the entire course of the transformation. The mixedmode model which can consider both the effects and the varying relative importance of two extreme kinetics modes provides an appropriate approach to describe the character of actual phase transformation accurately.

The nucleation, the growth of new phase with diffusion and mixedmode character, and the impingement effects of the growing neighboring grains are described briefly.

Aiming at the precision prediction of the nucleation, the growth and the impingement in the transformation, the developments of the empirical and analytical models, the phasefield models, the cellular automaton models, the Monte Carlo models and the molecular dynamics methods are summarized in detailed. Five numerical techniques provide good tools for the simulation of complex microstructure evolution.

By comparing with these models, it is found that: the empirical and analytical models only provide average information on macroscale; the mechanisticbased phase field simulation can predict the evolution of arbitrary complex microstructure without any presumption on their shape or mutual distribution and explicitly tracking the of the interface position while it is more computationally intensive; the cellular automata models are more easily implemented and possess the high computational efficiency while its lack physical meanings on the time scale and the growth kinetics of grains; the Monte Carlo model as usually is very similar to the cellular automata model; the molecular dynamics simulations are utilized to describe atomic interactions to make up for the disadvantage of mesoscopic models while the representative volume element that can be simulated is very limited.

Increasing efforts will be expected, to focus on exploring more advanced numerical simulation techniques coupled with atomistic calculations and macroscopic simulation, for predicting many important or nonnegligible phenomena such as the mixture of different nucleation modes, the anisotropic growth caused by the anisotropic interfacial energy or mobility, the hard and soft impingement, and the effect of the thermal history and the elastic or plastic deformation.
Acknowledgments
The authors would like to gratefully acknowledge the project supported by the National Natural Science Foundation of China (51675433), and the Research Fund of the State Key Laboratory of Solidification Processing (NWPU), China (Grant No.149QZ2016) and the 111 Project (B08040).
References
 Y.J. Lan et al., Mesoscale simulation of deformed austenite decomposition into ferrite by coupling a cellular automaton method with a crystal plasticity finite element model, Acta Materialia 53 (2005) 991–1003 [CrossRef] [Google Scholar]
 H. Yang et al., Review on cellular automata simulations of microstructure evolution during metal forming process: Grain coarsening, recrystallization and phase transformation, Sci. China Technol. Sci. 54 (2011) 2107–2118 [CrossRef] [Google Scholar]
 Y.H. Jiang et al., Solidstate phase transformation kinetics in the nearequilibrium regime, J. Mater. Sci. 50 (2015) 662–677 [CrossRef] [Google Scholar]
 K.J. Song et al., Cellular automatonbased study of factors that affect dynamic solid phase transformation kinetics, Appl. Math. Model. 39 (2015) 5058–5072 [CrossRef] [Google Scholar]
 H. Li et al., Nonisothermal phasetransformation kinetics model for evaluating the austenization of 55 CrMo steel based on Johnson–Mehl–Avrami equation, Materials & Design 92 (2016) 731–741 [CrossRef] [Google Scholar]
 Y.H. Jiang, F. Liu, S.J. Song, Extension of analytical model of solidstate phase transformation, Trans. Nonferrous Metals Soc. China 22 (2012) 1176–1181 [CrossRef] [Google Scholar]
 M. Meng et al., On the modeling of diffusioncontrolled growth of primary alpha in heat treatment of twophase Tialloys, J. Alloys & Compounds 691 (2016) 67–80 [CrossRef] [Google Scholar]
 R. Shi et al., Microstructure and transformation texture evolution during α, precipitation in polycrystalline α/β, titanium alloys − A simulation study, Acta Materialia 94 (2015) 224–243 [CrossRef] [Google Scholar]
 S. Cui et al., Interface stress evolution of martensitic transformation in MnCu alloys: a phasefield study, Materials & Design 109 (2016) 88–97 [CrossRef] [Google Scholar]
 Y. Deng, S. Xiu, Research on microstructure evolution of austenitization in grinding hardening by cellular automata simulation and experiment, Int. J. Adv. Manuf. Technol. 93 (2017) 2599–2612 [CrossRef] [Google Scholar]
 C. Halder, L. Madej, M. Pietrzyk, Discrete microscale cellular automata model for modelling phase transformation during heating of dual phase steels, Archives Civil & Mech. Eng. 14 (2014) 96–103 [CrossRef] [Google Scholar]
 D.S. Svyetlichnyy, Threedimensional frontal cellular automata model of microstructure evolution phase transformation module, ISIJ Int. 54 (2014) 1386–1395 [CrossRef] [Google Scholar]
 B.J. Kooi, Monte Carlo simulations of phase transformations caused by nucleation and subsequent anisotropic growth: extension of the JohnsonMehlAvramiKolmogorov theory, Phys. Rev. B 70 (2004) 155–163 [Google Scholar]
 H. Song, J.J. Hoyt, A molecular dynamics study of heterogeneous nucleation at grain boundaries during solidstate phase transformations, Comput. Mater. Sci. 117 (2016) 151–163 [CrossRef] [Google Scholar]
 G.Z. Quan, J. Pan, Z.H. Zhang, Phase transformation and recrystallization kinetics in spacetime domain during isothermal compressions for Ti6Al4V analyzed by multifield and multiscale coupling FEM, Materials & Design 94 (2016) 523–535 [CrossRef] [Google Scholar]
 N.M. Xiao et al., Progress in mesoscopic modeling of microstructure evolution in steels, Sci. China Technol. Sci. 55 (2012) 341–356 [CrossRef] [Google Scholar]
 N. Moelans, B. Blanpain, P. Wollants, An introduction to phasefield modeling of microstructure evolution, CalphadComput. Coupling Phase Diagrams & Thermochemistry 32 (2008) 268–294 [CrossRef] [Google Scholar]
 M.A. Miodownik, A review of microstructural computer models used to simulate grain growth and recrystallisation in aluminium alloys, J. Light Metals 2 (2002) 125–135 [CrossRef] [Google Scholar]
 H. Hallberg, Approaches to modeling of recrystallization, Metals 1 (2011) 16–48 [CrossRef] [Google Scholar]
 J.M. Haile, Molecular dynamics simulation: elementary methods, Comput. Phys. 7 (1993) 625 [CrossRef] [Google Scholar]
 J. Svoboda et al., Kinetics of interfaces during diffusional transformations, Acta Materialia 49 (2001) 1249–1259 [CrossRef] [Google Scholar]
 A.K. Jena, M.C. Chaturvedi, Phase transformation in materials, Prentice Hall, 1992 [Google Scholar]
 W.A. Soffa, D.E. Laughlin, Diffusional phase transformations in the solid state. Phys. Metall. (2014) 0851–1020 [CrossRef] [Google Scholar]
 E. Kozeschnik, Modeling solidstate diffusion − Computational Materials Engineering − 5. Comput. Mater. Eng., 2007 151–177 [CrossRef] [Google Scholar]
 H.I. Aaronson, M. Enomoto, J.K. Lee, Mechanisms of diffusional phase transformations in metals and alloys, 2010 [CrossRef] [Google Scholar]
 J. Sietsma, S.V.D. Zwaag, A concise model for mixedmode phase transformations in the solid state, Acta Materialia 52 (2004) 4143–4152 [CrossRef] [Google Scholar]
 C. Zener, Theory of growth of spherical precipitates from solid solution, J. Appl. Phys. 20 (1949) 950–953 [CrossRef] [Google Scholar]
 J.W. Christian, The theory of transformations in metals and alloys, Newnes, 2002 [Google Scholar]
 J. Sietsma et al., Evolution of the mixedmode character of solidstate phase transformations in metals involving solute partitioning, Zeitschrift Für Metallkunde 97 (2006) 356–361 [CrossRef] [Google Scholar]
 E.D. Schmidt, E.B. Damm, S.A. Sridhar, Study of diffusion and interfacecontrolled migration of the austenite/ferrite front during austenitization of a casehardenable alloy steel, Metall. & Mater. Trans. A 38 (2007) 698–715 [CrossRef] [Google Scholar]
 H. Chen, B. Appolaire, S.V.D. Zwaag, Application of cyclic partial phase transformations for identifying kinetic transitions during solidstate phase transformations: experiments and modeling, Acta Materialia 59 (2011) 6751–6760 [CrossRef] [Google Scholar]
 M. Hillert, Solute drag, solute trapping and diffusional dissipation of Gibbs energy 1, Acta Materialia 47 (1999) 4481–4505 [CrossRef] [Google Scholar]
 G.P. Krielaart, J. Sietsma, S.V.D. Zwaag, Ferrite formation in Fe–C alloys during austenite decomposition under nonequilibrium interface conditions, Mater. Sci. & Eng. A 237 (1997) 216–223 [CrossRef] [Google Scholar]
 A. Salwén, A new model for diffusional growth, Metallurgical Transactions A 24 (1993) 1507–1516 [CrossRef] [Google Scholar]
 G. Eriksson, K. Hack, ChemSage—a computer program for the calculation of complex chemical equilibria, Metall. Trans. B 21 (1990) 1013–1023 [CrossRef] [Google Scholar]
 J.W. Gibbs, On the equilibrium of heterogeneous substances, Trans Connecticut Acad, 1967 [Google Scholar]
 R. Becker, W. Döring, Kinetische Behandlung der Keimbildung in übersättigten Dämpfen, Annalen Der Physik 416 (1935) 719–752 [NASA ADS] [CrossRef] [Google Scholar]
 J.W. Cahn, J.E. Hilliard, Free energy of a nonuniform system. I. Interfacial free energy, J. Chem. Phys. 28 (1958) 258–267 [CrossRef] [Google Scholar]
 J.W. Cahn, J.E. Hilliard, Free energy of a nonuniform system, III. Nucleation in a twocomponent incompressible fluid. The Selected Works of John W. Cahn, 2013, pp. 39–50 [CrossRef] [Google Scholar]
 R. Poduri, L.Q. Chen, Nonclassical nucleation theory of ordered intermetallic precipitates—application to the Al–Li alloy, Acta Materialia 44 (1996) 4253–4259 [CrossRef] [Google Scholar]
 D.A. Porter, K.E. Easterling, Phase transformations in metal and alloys, 2nd edition. Chapman & Hall, 1992 [CrossRef] [Google Scholar]
 F. Liu, F. Sommer, E.J. Mittemeijer, An analytical model for isothermal and isochronal transformation kinetics, J. Mater. Sci. 39 (2004) 1621–1634 [CrossRef] [Google Scholar]
 F. Liu et al., Analysis of solid state phase transformation kinetics: models and recipes, Metall. Rev. 52 (2013) 193–212 [CrossRef] [Google Scholar]
 M. Avrami, Kinetics of phase change. II Transformationtime relations for random distribution of nuclei, J. Chem. Phy. 8 (1940) 212–224 [NASA ADS] [CrossRef] [Google Scholar]
 M. Avrami, Granulation, phase change, and microstructure kinetics of phase change. III, J. Chem. Phys. 9 (1941) 177–184 [NASA ADS] [CrossRef] [Google Scholar]
 Y. Liu et al., Isothermal austenite–ferrite transformation of Fe–0.04 at.% C alloy: dilatometric measurement and kinetic analysis, Acta Materialia 56 (2008) 3833–3842 [CrossRef] [Google Scholar]
 G. Meyrick, G.W. Powell, Phase transformations in metals and alloys, Annu. Rev. Mater. Sci. 74 (2003) 299–301 [Google Scholar]
 T.W. Heo, L.Q. Chen, Phasefield modeling of nucleation in solidstate phase transformations, JOM 66 (2014) 1520–1528 [CrossRef] [Google Scholar]
 Y.V. Leeuwen, Moving interfaces in lowcarbon steel − a phase transformation model, Appl. Sci. 29 (2000) 223–230 [Google Scholar]
 R.D. Doherty, Diffusive phase transformations in the solid state − Physical Metallurgy (Fourth Edition) − Chapter 15[J]. Phys. Metall. (1996) 1363–1505 [CrossRef] [Google Scholar]
 Ø. Grong, H.R. Shercliff, Microstructural modelling in metals processing, Progr. Mater. Sci. 47 (2002) 163–282 [CrossRef] [Google Scholar]
 H.S. Carslaw, J.C. Jaeger, Conduction of heat in solids/by H. S. Carslaw and J. C. Jaeger[J], 1959 [Google Scholar]
 H.B. Aaron, D. Fainstein, G.R. Kotler, Diffusionlimited phase transformations: a comparison and critical evaluation of the mathematical approximations, J. Appl. Phys. 41 (1970) 4404–4410 [CrossRef] [Google Scholar]
 S.L. Semiatin et al., Microstructure evolution during alphabeta heat treatment of Ti6Al4V, Metall. & Mater. Trans. A 34 (2003) 2377–2386 [CrossRef] [Google Scholar]
 M. Avrami, Kinetics of phase change. I general theory, J. Chem. Phys. 7 (1939) 1103–1112 [NASA ADS] [CrossRef] [Google Scholar]
 K. Fan et al., Analysis of soft impingement in nonisothermal precipitation, J. Mater. Res. 24 (2009) 3664–3673 [CrossRef] [Google Scholar]
 C. Wert, C. Zener, Interference of growing spherical precipitate particles, J. Appl. Phys. 21 (1950) 5–8 [CrossRef] [Google Scholar]
 K. Fan et al., Modeling of isothermal solidstate precipitation using an analytical treatment of soft impingement, Acta Materialia 56 (2008) 4309–4318 [CrossRef] [Google Scholar]
 S.E. Offerman et al., Solidstate phase transformations involving solute partitioning: modeling and measuring on the level of individual grains, Acta Materialia 52 (2004) 4757–4766 [CrossRef] [Google Scholar]
 D. Crespo et al., Microstructural evaluation of primary crystallization with diffusioncontrolled grain growth, Phys. Rev. B Condens. Matter 55 (1997) 3435–3444 [CrossRef] [Google Scholar]
 C. Hao, S.V.D. Zwaag, Modeling of soft impingement effect during solidstate partitioning phase transformations in binary alloys, J. Mater. Sci. 46 (2011) 1328–1336 [CrossRef] [Google Scholar]
 M. Tomellini, Soft impingement in diffusioncontrolled growth of binary alloys: moving boundary effect in onedimensional system, J. Mater. Sci. 48 (2013) 5653–5663 [CrossRef] [Google Scholar]
 H. Chen, V.D.Z. Sybrand, A mixedmode model considering soft impingement effects for solidstate partitioning phase transformations, Solid State Phenom. 172–174 (2011) 561–566 [CrossRef] [Google Scholar]
 R.E. Lyon, An integral method of nonisothermal kinetic analysis, Thermochimica Acta 297 (1997) 117–124 [CrossRef] [Google Scholar]
 J. Málek, Crystallization kinetics by thermal analysis, J. Therm. Anal & Calorim. 56 (1999) 763–769 [CrossRef] [Google Scholar]
 W.A. Johnson, Reaction kinetics in process of nucleation and growth, Trans. AIME 135 (1939) 416–458 [Google Scholar]
 S.J. Song et al., Kinetics of solidstate transformation subjected to anisotropic effect: model and application, Acta Materialia 59 (2011) 3276–3286 [CrossRef] [Google Scholar]
 F. Liu et al., Analytical description for solidstate phase transformation kinetics: extended works from a modular model, a review, J. Mater. Sci. & Technol. 32 (2016) 97–120 [CrossRef] [Google Scholar]
 V.V. Sessa, M. Fanfoni, M. Tomellini, Validity of Avrami's kinetics for random and nonrandom distributions of germs, Phys. Rev. B Condens. Matter 54 (1996) 836–841 [CrossRef] [Google Scholar]
 G. Tegze et al., Diffusioncontrolled anisotropic growth of stable and metastable crystal polymorphs in the phasefield crystal model, Phys. Rev. Lett. 103 (2009) 035702 [CrossRef] [PubMed] [Google Scholar]
 J.W. Cahn, The kinetics of grain boundary nucleated reactions, Acta Metallurgica 4 (1956) 449–459 [CrossRef] [Google Scholar]
 K.F. Kelton, A.L. Greer, C.V. Thompson, Transient nucleation in condensed systems, J. Chem. Phys. 79 (1983) 6261–6276 [CrossRef] [Google Scholar]
 M. Tomellini, M. Fanfoni, M. Volpe, Spatially correlated nuclei: how the JohnsonMehlAvramiKolmogorov formula is modified in the case of simultaneous nucleation, Phys. Rev. B 62 (2000) 11300 [CrossRef] [Google Scholar]
 P.R. Rios, E. Villa, Simultaneous and sequential transformations, Acta Materialia 59 (2011) 1632–1643 [CrossRef] [Google Scholar]
 B.J. Kooi, Monte Carlo simulations of phase transformations caused by nucleation and subsequent anisotropic growth: extension of the JohnsonMehlAvramiKolmogorov theory, Physical Review B 70 (2004) 155–163 [Google Scholar]
 V.A. Shneidman, M.C. Weinberg, The effects of transient nucleation and sizedependent growth rate on phase transformation kinetics, J. NonCrystalline Solids 160 (1993) 89–98 [CrossRef] [Google Scholar]
 A. Bhattacharya, C.S. Upadhyay, S. Sangal, A quantitative phasefield simulation of softimpingement in austenite to ferrite transformation with mixedmode, Metall. & Mater. Trans. A (2017) 1–14 [Google Scholar]
 M. Tomellini, Impingement factor in the case of phase transformations governed by spatially correlated nucleation, Phys. Rev. B 78 (2008) 1436–1446 [CrossRef] [Google Scholar]
 M.C. Weinberg, D.P.B. Iii, Avrami exponents for transformations producing anisotropic particles, J. NonCrystalline Solids 202 (1996) 290–296 [CrossRef] [Google Scholar]
 B.J. Kooi. Extension of the Johnson–Mehl–Avrami–Kolmogorov theory incorporating anisotropic growth studied by Monte Carlo simulations, Phys. Rev. B 73 (2006) 054103 [CrossRef] [Google Scholar]
 A.T.W. Kempen, F. Sommer, E.J. Mittemeijer, The kinetics of the austeniteferrite phase transformation of FeMn: differential thermal analysis during cooling, Acta Materialia 50 (2002) 3545–3555 [CrossRef] [Google Scholar]
 S.J. Song, F. Liu, Y.H. Jiang, Generalized additivity rule and isokinetics in diffusioncontrolled growth, J. Mater. Sci. 49 (2014) 2624–2629 [CrossRef] [Google Scholar]
 M. Hillert, Role of interfacial energy during solidstate phase transformations, Jernkontorets Annaler 141 (1957) 757–789 [Google Scholar]
 G.P. Ivantsov, The temperature field around a spherical, cylindrical, or pointed crystal growing in a cooling solution, Dokl. Akad. Nauk SSSR 58 (1947) 567–569 [Google Scholar]
 G. Horvay, J.W. Cahn, Dendritic and spheroidal growth, Acta Metallurgica 9 (1961) 695–705 [CrossRef] [Google Scholar]
 R. Trivedi, The role of interfacial free energy and interface kinetics during the growth of precipitate plates and needles, Metall. Mater. Trans. B 1 (1970) 921–927 [Google Scholar]
 L.Q. Chen, W. Yang, Computer simulation of the domain dynamics of a quenched system with a large number of nonconserved order parameters: the graingrowth kinetics, Phys. Rev. B Condens. Matter 50 (1994) 15752 [CrossRef] [Google Scholar]
 L.Q. Chen, A.G. Khachaturyan, Dynamics of simultaneous ordering and phase separation and effect of longrange Coulomb interactions, Phys. Rev. Lett. 70 (1993) 1477 [CrossRef] [Google Scholar]
 J.D.V.D. Waals, The thermodynamic theory of capillarity under the hypothesis of a continuous variation of density, J. Stat. Phys. 20 (1979) 200–244 [CrossRef] [Google Scholar]
 V.L. Ginzburg, L.D. Landau, On the theory of superconductivity, J. Exp. Theor. Phys. 20 (1950) 35 [Google Scholar]
 V.L. Ginzburg, L.D. Landau, Phenomenological theory, J. Exp. Theor. Phys. 20 (1950) 1064 [Google Scholar]
 L.Q. Chen, Phasefield models for microstructure evolution, Annu. Rev. Mater. Res. 32 (2002) 113–140 [CrossRef] [Google Scholar]
 L.Q. Chen, Y. Wang, The continuum field approach to modeling microstructural evolution, JOM 48 (1996) 13–18 [CrossRef] [Google Scholar]
 L. Zhang, L.Q. Chen, Q. Du, Simultaneous prediction of morphologies of a critical nucleus and an equilibrium precipitate in solids, Commun. Comput. Phys. 7 (2010) 674–682 [Google Scholar]
 T.W. Heo et al., Incorporating diffuseinterface nuclei in phasefield simulations, Scripta Materialia 63 (2010) 8–11 [CrossRef] [Google Scholar]
 W. Yan et al., Phasefield modeling of Widmanstätten ferrite formation during isothermal transformation in low carbon steels, Comput. Mater. Sci. 81 (2014) 503–509 [CrossRef] [Google Scholar]
 T.W. Heo, L.Q. Chen, Phasefield modeling of nucleation in solidstate phase transformations, JOM 66 (2014) 1520–1528 [CrossRef] [Google Scholar]
 Y. Jin et al., 2D finite element modeling of misorientation dependent anisotropic grain growth in polycrystalline materials: level set versus multiphasefield method, Comput. Mater. Sci. 104 (2015) 108–123 [CrossRef] [Google Scholar]
 E. Miyoshi, T. Takaki, Extended higherorder multiphasefield model for threedimensional anisotropicgraingrowth simulations, Comput. Mater. Sci. 120 (2016) 77–83 [CrossRef] [Google Scholar]
 A.G. Khachaturyan, Theory of structural transformations in solids, Courier Corporation, 2013 [Google Scholar]
 F. Peter, P. Oliver, L.L. Joel, Modelling of phase separation in alloys with coherent elastic misfit, J. Stat. Phys. 95 (1999) 1429–1503 [CrossRef] [MathSciNet] [Google Scholar]
 L. Q. Chen, S. Hu, Phasefield method applied to straindominated microstructure evolution during solidstate phase transformations. Continuum scale simulation of engineering materials: fundamentalsmicrostructuresprocess applications, 2004, pp. 271–296 [Google Scholar]
 B. Appolaire et al., Noncoherent interfaces in diffuse interface models, Philos. Magazine 90 (2010) 461–483 [CrossRef] [Google Scholar]
 K. Ammar et al., Combining phase field approach and homogenization methods for modelling phase transformation in elastoplastic media, European J. Comput. Mech. 18 (2009) 485–523 [CrossRef] [Google Scholar]
 K. Ammar et al., Modelling inheritance of plastic deformation during migration of phase boundaries using a phase field method, Meccanica 49 (2014) 2699–2717 [CrossRef] [Google Scholar]
 V. De Rancourt et al., Homogenization of viscoplastic constitutive laws within a phase field approach, J. Mech. & Phys. Solids 88 (2016) 291–319 [CrossRef] [Google Scholar]
 J.P. Simmons et al., Microstructural development involving nucleation and growth phenomena simulated with the phase field method, Mater Sci. & Eng. A 365 (2004) 136–143 [CrossRef] [Google Scholar]
 G. Wang, D.C. Zeng, Z.W. Liu, Phase field study of concurrent nucleation and growth in a diffusioncontrolled solidstate phase transformation, Adv. Mater. Res. 490–495 (2012) 1140–1144 [CrossRef] [Google Scholar]
 A. Yamanaka, T. Takaki, Y. Tomita, Multiphasefield modeling of diffusive solid phase transition in carbon steel during continuous cooling transformation, J. Crys. Growth 310 (2008) 1337–1342 [CrossRef] [Google Scholar]
 M. Militzer et al., Threedimensional phase field modelling of the austenitetoferrite transformation, Acta Materialia 54 (2006) 3961–3972 [CrossRef] [Google Scholar]
 Q. Chen et al., Quantitative phase field modeling of diffusioncontrolled precipitate growth and dissolution in Ti–Al–V , Scripta Materialia 50 (2004) 471–476 [CrossRef] [Google Scholar]
 N. OforiOpoku, N. Provatas, A quantitative multiphase field model of polycrystalline alloy solidification, Acta Materialia 58 (2010) 2155–2164 [CrossRef] [Google Scholar]
 I. Steinbach et al., CALPHAD and phasefield modeling: a successful liaison, J. Phase Equilibria & Diffusion 28 (2007) 101–106 [CrossRef] [Google Scholar]
 M. Militzer et al., Threedimensional phase field modelling of the austenitetoferrite transformation, Acta Materialia 54 (2006) 3961–3972 [CrossRef] [Google Scholar]
 S. Cui, J. Wan, X. Zuo et al., Threedimensional, nonisothermal phasefield modeling of thermally and stressinduced martensitic transformations in shape memory alloys, Int. J. Solids & Struc. 109 (2017) 1–11 [CrossRef] [Google Scholar]
 I. Steinbach, F. Pezzolla, A generalized field method for multiphase transformations using interface fields, Physica D: Nonlinear Phenomena 134 (1999) 385–393 [CrossRef] [MathSciNet] [Google Scholar]
 S.B. Biner, Programming phase field modeling, Springer, 2017 T. Takaki et al., Twodimensional phase field simulations of dendrite competitive growth during the directional solidification of a binary alloy bicrystal, Acta Materialia 81 (2014) 272–283 [CrossRef] [Google Scholar]
 T. Takaki et al., Twodimensional phasefield simulations of dendrite competitive growth during the directional solidification of a binary alloy bicrystal, Acta Materialia 81 (2014) 272–283 [CrossRef] [Google Scholar]
 C. Yang, Q. Xu, B. Liu, GPUaccelerated threedimensional phasefield simulation of dendrite growth in a nickelbased superalloy, Comput. Mater. Sci. 136 (2017) 133–143 [CrossRef] [Google Scholar]
 Rolling of advanced high strength steels: theory, simulation and practice, CRC Press, 2017 [Google Scholar]
 K.G.F. Janssens. An introductory review of cellular automata modeling of moving grain boundaries in polycrystalline materials, Math. & Comput. Simul. 80 (2010) 1361–1381 [CrossRef] [Google Scholar]
 H.W. Hesselbarth, L. Kaps, F. Haessner, Two dimensional simulation of the recrystallization kinetics in the case of inhomogeneous stored energy. Mater. sci. Forum, (1993) 317–322 [CrossRef] [Google Scholar]
 P.J. Hurley, F.J. Humphreys, Modelling the recrystallization of singlephase aluminium, Acta Materialia 51 (2003) 3779–3793 [CrossRef] [Google Scholar]
 Y.C. Lin et al., Study of static recrystallization behavior in hot deformed Nibased superalloy using cellular automaton model, Materials & Design 99 (2016) 107–114 [CrossRef] [Google Scholar]
 K.J. Song et al., Numerical simulation of β to α phase transformation in heat affected zone during welding of TA15 alloy, Comput. Mater. Sci. 72 (2013) 93–100 [CrossRef] [Google Scholar]
 C. Wu, Y. He, H.W. Li, Modeling of static coarsening of twophase titanium alloy in the α+β twophase region at different temperature by a cellular automata method. Chin. Sci. Bull. 58 (2013) 3023–3032 [CrossRef] [Google Scholar]
 M.F. Zhu, D.M. Stefanescu, Virtual front tracking model for the quantitative modeling of dendritic growth in solidification of alloys, Acta Materialia 55 (2007) 1741–1755 [CrossRef] [Google Scholar]
 L. Madej, P.D. Hodgson, M. Pietrzyk, Multiscale rheological model for discontinuous phenomena in materials under deformation conditions, Comput. Mater. Sci. 38 (2007) 685–691 [CrossRef] [Google Scholar]
 J.L. He, M.T. Li, Cellular automata to simulate crack propagation of quasibrittle materials, Appl. Mech. & Mater. 90–93 (2011) 748–751 [Google Scholar]
 D.S. Svyetlichnyy, Modelling of the microstructure: from classical cellular automata approach to the frontal one, Comput. Mater. Sci. 50 (2011) 92–97 [CrossRef] [Google Scholar]
 K.G.F. Janssens, I rregular cellular automata modeling of grain growth. Continuum scale simulation of engineering materials: fundamentals − microstructures − process applications, 2005, pp. 297–308 [Google Scholar]
 K.J. Song et al., Virtual front tracking cellular automaton modeling of isothermal β to α phase transformation with crystallography preferred orientation of TA15 alloy, Model. & Simul.Mater. Sci. & Eng. 22 (2014) 5006 [Google Scholar]
 D. Raabe et al., Continuum scale simulation of engineering materials: fundamentals − microstructures − process applications, Front. Psychol. 6 (2014) 885 [Google Scholar]
 L. BeltranSanchez, D.M. Stefanescu, Growth of solutal dendrites: a cellular automaton model and its quantitative capabilities, Metall. & Mater. Trans. A 34 (2003) 367–382 [CrossRef] [Google Scholar]
 K.G.F. Janssens, E.A. Holm, S.M. Foiles, Introducing solute drag in irregular cellular automata modeling of grain growth, Mater. Sci. Forum 467–470 (2004) 1045–1050 [CrossRef] [Google Scholar]
 D.S. Svyetlichnyy, Reorganization of cellular space during the modeling of the microstructure evolution by frontal cellular automata, Comput. Mater. Sci. 60 (2012) 153–162 [CrossRef] [Google Scholar]
 D.S. Svyetlichnyy, Modeling of grain refinement by cellular automata, Comput. Mater. Sci. 77 (2013) 408–416 [CrossRef] [Google Scholar]
 J.W. Cahn, The impuritydrag effect in grain boundary motion, Acta Metallurgica 10 (1962) 789–798 [CrossRef] [Google Scholar]
 B. Su, Z. Han, B. Liu, Cellular automaton modeling of austenite nucleation and growth in hypoeutectoid steel during heating process, ISIJ Int. 53 (2013) 527–534 [CrossRef] [Google Scholar]
 R. Golab et al., Sensivity analysis of the cellular automata model for austeniteferrite phase transformation in steels, Appl. Math. 4 (2013) 1531–1536 [CrossRef] [Google Scholar]
 C. Zheng, D. Raabe, D. Li, Prediction of postdynamic austenitetoferrite transformation and reverse transformation in a lowcarbon steel by cellular automaton modeling, Acta Materialia 60 (2012) 4768–4779 [CrossRef] [Google Scholar]
 C. Zheng, D. Raabe, Interaction between recrystallization and phase transformation during intercritical annealing in a coldrolled dualphase steel: a cellular automaton model, Acta Materialia 61 (2013) 5504–5517 [CrossRef] [Google Scholar]
 K.J. Song et al., Cellular automaton modeling of diffusion, mixed and interface controlled phase transformation, J. Phase Equilibria & Diffusion 36 (2015) 136–148 [CrossRef] [Google Scholar]
 F.Y. Wu, The Potts model, Rev. Modern Phys. 54 (1982) 235–268 [CrossRef] [Google Scholar]
 M.P. Anderson et al., Computer simulation of grain growth I. Kinetics, Acta Metallurgica 32 (1984) 783–791 [CrossRef] [Google Scholar]
 A.D. Rollett, Overview of modeling and simulation of recrystallization, Prog. Mater. Sci. 42 (1997) 79–99 [CrossRef] [Google Scholar]
 J.K. Mason, Grain boundary energy and curvature in Monte Carlo and cellular automata simulations of grain boundary motion, Acta Materialia 94 (2015) 162–171 [CrossRef] [Google Scholar]
 B.J. Alder, T.E. Wainwright, Studies in molecular dynamics. I. General method, J. Chem. Phys. 31 (1959) 459–466 [CrossRef] [MathSciNet] [Google Scholar]
 C.P. Chui et al., Molecular dynamics simulation of iron — a review, Spin 05 (2015) [Google Scholar]
 S. Okita et al., Molecular dynamics simulations investigating consecutive nucleation, solidification and grain growth in a twelvemillionatom Fesystem, J. Cryst. Growth 474 (2017) 140–145 [CrossRef] [Google Scholar]
 D.U. Furrer, Application of phasefield modeling to industrial materials and manufacturing processes, Current Opin. Solid State Mater. Sci. 15 (2011) 134–140 [CrossRef] [Google Scholar]
 M. Mamivand, M.A. Zaeem, H.E. Kadiri, A review on phase field modeling of martensitic phase transformation, Comput. Mater. Sci. 77 (2013) 304–311 [CrossRef] [Google Scholar]
 H. Li, X. Sun, H. Yang, A threedimensional cellular automatacrystal plasticity finite element model for predicting the multiscale interaction among heterogeneous deformation, DRX microstructural evolution and mechanical responses in titanium alloys, Int. J. Plasti. 87 (2016) 154–180 [CrossRef] [Google Scholar]
 M.A. Miodownik, A review of microstructural computer models used to simulate grain growth and recrystallisation in aluminium alloys, J. Light Metals 2 (2002) 125–135 [CrossRef] [Google Scholar]
 P.W. Hoffrogge, L.A. BarralesMora, Grainresolved kinetics and rotation during grain growth of nanocrystalline aluminium by molecular dynamics, Comput. Mater. Sci. 128 (2017) 207–222 [CrossRef] [Google Scholar]
 S. Tateyama, Y. Shibuta, T. Suzuki, A molecular dynamics study of the fccbcc phase transformation kinetics of iron, Scripta Materialia 59 (2008) 971–974 [CrossRef] [Google Scholar]
 S. Chakraborty, J. Zhang, S. Ghosh, Accelerated molecular dynamics simulations for characterizing plastic deformation in crystalline materials with cracks, Comput. Mater. Sci. 121 (2016) 23–34 [CrossRef] [Google Scholar]
Cite this article as: Xueyan Liu, Hongwei Li, Mei Zhan, A review on the modeling and simulations of solidstate diffusional phase transformations in metals and alloys, Manufacturing Rev. 5, 10 (2018)
All Figures
Fig. 1 Schematic representation of the partial phase diagram of a binary A–B alloy. 

In the text 
Fig. 2 Planar interface migration and solution partitioning of a binary A–B alloy with initial concentration for component B [26]. 

In the text 
Fig. 3 Schematic representation of molar Gibbs energy for the β→α transformation in an A–B alloy in order to derive the driving force acting on interface [32,36]. 

In the text 
Fig. 4 (A) Sharp interface: properties are discontinuous at the interface; (B) Diffuse interface: properties evolve continuously between their equilibrium values in the neighboring grains[17,36]. 

In the text 
Fig. 5 Neighboring type in cellular automata: (A) von Neumann configuration; (B) Moor configuration. 

In the text 
Fig. 6 Illustration of (A) determining the position of sharp virtual interface, and (B) capturing rules for new interface cells [127,134]. 

In the text 
Fig. 7 Illustration of (A) cells distribution in a twodimensional irregular cellular automata based on the Voronoi cells, and (B) a shapeless cell on a curved interface and its spherical neighborhood [121]. 

In the text 
Fig. 8 Illustration of FCA (frontal cellular automata). 

In the text 
Current usage metrics show cumulative count of Article Views (fulltext article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.
Data correspond to usage on the plateform after 2015. The current usage metrics is available 4896 hours after online publication and is updated daily on week days.
Initial download of the metrics may take a while.