for first order phase transitions under certain strong assumptions • Random nucleation events with constant rates of nucleation and growth in an infinite domain • n is referred to as the Avrami exponent • Found from the slope of log(-log(1-Y)) vs log(t) • n = d + 0 (site saturation) n = d + 1 (continuous nucleation)
evolution of Φ given by Allen-Cahn Equation: • Initial Condition: • Driving force for solidification: https://pages.nist.gov/pfhub/benchmarks/benchmark8.ipynb/ 𝜖2 = 1,𝜔 = 1, 𝑀 = 1 • Double Well • Interpolation Function • Definition of Constants
• Shared Goals: • Plot the 2d representation of phi • Plot the volume fraction of the solid • Plot the total free energy • Plot the Avrami Plot Wu et al. Phase Field Benchmark Problems for Nucleation, CMS 2021 Part Domain Size r* r0 Seeds Part 2 500 x 500 1.0 2.2 25 Part 3 1000 x 1000 2.0 2.2 100 • Part 2 - Site Saturation • All seeds placed at t = 0 • Seeds are randomly located • Expected Avrami constant: n = 2 • Part 3 – Continuous Nucleation • Seeds are randomly placed in location and time • Expected Avrami constant: n = 3
Neumann BCs for parts 2 & 3 • PF Hub Website does not mention BCs in parts 2 & 3 • EDIT: Periodic BCs fit the assumptions of Avrami theory better • Infinite domain, spatiotemporal homogeneity of nucleation and growth • Simulations have been performed showing how BCs affect the Avrami constant • With this change part 2 yields ~2.0 Avrami constant (as expected)
& 3 in CMS paper and PF Hub website • r 0 /r* affects the rate of growth and Avrami Constant • Changing r0 /r* to 2.2 in part 3 yields ~3.0 values for Avrami constant • Edit: Change r* in part 3 to r* = 1.0 Part Initial Radius (r0 ) Critical Radius (r*) r0 / r* Part 2 2.2 1.0 2.2 Part 3 2.2 2.0 1.1
paper finding the Avrami constant uses a method of linear fitting in a range of log(t) • Part 3: 1.5 < log(t) < 2.5 • New approach: • Linear fit in range of log(-log(1-Y)) • -2 < log(-log(1-Y) < 0 • Corresponds to 0.02 < Y < 0.9 • In cases of late first seed nucleation in pt. 3, 1st approach yields no value of slope • 2nd approach yields a consistent fitting range in part 2 and part 3 Wu et al. Phase Field Benchmark Problems for Nucleation, CMS 2021
involve stochasticity • Large numbers of simulations provides greater statistical accuracy • Changed the number of simulations suggested for parts 2 and 3 • 5 simulations each to 10 simulations each • Different random positions of seeds and times • N = 5 obtains 1.97 ≤ n ≤ 2.03 77% of the time for pt. 2 • N = 10 obtains 1.97 ≤ n ≤ 2.03 96% of the time for pt. 2
Boundary condition → Periodic in parts 2 and 3 • r* → 1.0 in part 3 •r0 /r* ratio and transient growth • Post-processing using limits in the log(-log(1-Y)) axis • Use of statistics • Completed edits can be viewed at: https://pages.nist.gov/pfhub/benchmarks/benchmark8.ipynb/ • More in: Mancias, José, et al. "On the Effect of Nucleation Undercooling on Phase Transformation Kinetics." Integrating Materials and Manufacturing Innovation 11.4 (2022) • Corresponding Github Repo: https://github.com/joseam2/PF_Nucleation_Benchmark_Julia