# The Effect of Interatomic Potentials on the Nature of Nanohole Propagation in Single-Crystal Nickel: A Molecular Dynamics Simulation Study

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## Abstract

**:**

## 1. Introduction

## 2. Simulation Conditions

#### 2.1. Initial Conditions

^{−1}was applied to the Y direction of single-crystal Ni. In the simulation, the simulation timestep was 0.001 ps. To analyze the nanohole propagation behaviors of single-crystal Ni, we visualized the atomic configurations and stress distributions of Ni atoms using the Open Visualization Tool (OVITO) [39].

#### 2.2. Potential between Atoms

## 3. Simulation Results and Discussion

#### 3.1. Stress–Strain Behavior

#### 3.2. Nanohole Propagation Behavior

_{yy}= 32.2 GPa). As the $\mathsf{\epsilon}$ value increased, the no. 1 nanohole gradually grew and coalesced with the main nanohole. At the same time, the no. 2 nanopore formed at the right-bottom corner of the main nanohole due to the stress concentration (ε = 10.2%, σ

_{yy}= 31 GPa; see Figure 4(c1)). Then, the no. 2 nanopore gradually grew and coalesced with the main nanohole, and the left region of the main nanohole also produced two nanopores (no. 3 and no. 4 nanopores). As shown in Figure 4d, the plastic deformation occurred in the upper local area of the right nanopore. When ε = 10.7%, the new no. 3 and no. 4nanopores continued to grow, and the misorientation between the tensile direction and the nanohole growth direction was 45°, indicating that the crack mainly propagated along the (110) plane of single-crystal Ni (see Figure 4g). Meanwhile, the stress concentration was present in the region of the front of the right-bottom corner of the propagated nanohole (Figure 4g; σ

_{yy}= 34 GPa), which gave rise to the new no. 5 nanopore initiation (Figure 4h). As ε = 15.9%, the nanohole propagated across the whole single-crystal Ni (Figure 4i). When the $\mathsf{\epsilon}$ value was below 10.4%, the nanohole was propagated using a fast brittle propagation model that included the process of formation and the coalescence of nanopores at the front of the nanohole with almost no emission of dislocations from the nanohole. With the strain increasing from 10.4% to 10.9%,however, the process of nanohole propagation was accompanied by the emission and slip of dislocations.

_{yy}= 26 GPa at the right-side local region of the nanohole (Figure 7(d1,d2)). Further increased strain led to the formation of a new nanopore to release the stress concentration level (Figure 7(e1,e2)). Finally, through the process of dislocation slip and the formation and coalescence of the nanopore, the tensile model was completely fractured.

#### 3.3. Relationship between Crack Length and Tensile Strain

#### 3.4. Discussion

## 4. Conclusions

- (1)
- The MEAM potential is best suited to describe the brittle propagation behavior of nanoholes in single-crystal Ni.
- (2)
- The EAM/FS potential is effective in characterizing the plastic growth behavior of nanoholes in single-crystal Ni.

^{−1}). The microstructure evolution and nanohole propagation process in the single-crystal Ni can be different as the simulation conditions change. In the future, we will systematically consider the effects of temperature, strain rate, crack shape, and potential function on crack propagation in single-crystal Ni.

## Supplementary Materials

## Author Contributions

## Funding

## Data Availability Statement

## Acknowledgments

## Conflicts of Interest

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**Figure 1.**The MD model of FCC single-crystal Ni with a central cylindrical nanohole: (

**a**) the size and orientation of simulated region and (

**b**) single-crystal Ni with cylindrical nanohole.

**Figure 2.**The stress–strain behavior of single-crystal Ni under the (

**a**) MEAM potential, (

**b**) EAM/FS potential, and (

**c**) EAM potential. The failure location is marked by the solid arrow.

**Figure 3.**The elastic strain ${\mathsf{\epsilon}}_{\mathrm{e}}$, total strain ${\mathsf{\epsilon}}_{\mathrm{t}}$ and accumulated plastic strain ${\mathsf{\epsilon}}_{\mathrm{p}}$ of single-crystal Ni under different styles of interatomic potentials.

**Figure 4.**The contour plots of the atomic tensile stress field and nanohole growth states at different tensile strains (MEAM potential).

**Figure 5.**The contour plots of the atomic tensile stress field and crack growth states at different tensile strains (EAM/FS potential).

**Figure 7.**The contour plots of the atomic tensile field and crack growth states at different tensile strains (EAM potential).

**Figure 8.**The crack length–strain curve of single-crystal Ni at different styles of potentials. The symbol ‘×’ denotes the fracture point of the tensile model.

MEAM | EAM/FS | EAM | ||
---|---|---|---|---|

Surface energy (erg/cm^{2}) | (100) plane | 1943 | 1444 | 1580 |

(110) plane | 2057 | 1548 | 1730 | |

(111) plane | 1606 | 1153 | 1450 | |

Stacking fault energy (erg/cm^{2}) | 125 | 33 | -- |

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**MDPI and ACS Style**

Qin, X.; Liang, Y.; Gu, J.; Peng, G. The Effect of Interatomic Potentials on the Nature of Nanohole Propagation in Single-Crystal Nickel: A Molecular Dynamics Simulation Study. *Crystals* **2023**, *13*, 585.
https://doi.org/10.3390/cryst13040585

**AMA Style**

Qin X, Liang Y, Gu J, Peng G. The Effect of Interatomic Potentials on the Nature of Nanohole Propagation in Single-Crystal Nickel: A Molecular Dynamics Simulation Study. *Crystals*. 2023; 13(4):585.
https://doi.org/10.3390/cryst13040585

**Chicago/Turabian Style**

Qin, Xinmao, Yilong Liang, Jiabao Gu, and Guigui Peng. 2023. "The Effect of Interatomic Potentials on the Nature of Nanohole Propagation in Single-Crystal Nickel: A Molecular Dynamics Simulation Study" *Crystals* 13, no. 4: 585.
https://doi.org/10.3390/cryst13040585