13 research outputs found
Atomistic modeling of the dislocation dynamics and evaluation of static yield stress
Static strength characteristics of structural materials are of great importance for the analysis of the materials behaviour under mechanical loadings. Mechanical characteristics of structural materials such as elastic limit, strength limit, ultimate tensile strength, plasticity are, unlike elastic moduli, very sensitive to the presence of impurities and defects of crystal structure. Direct atomistic modeling of the static mechanical strength characteristics of real materials is an extremely difficult task since the typical time scales available for the direct modeling in the frames of classical molecular dynamics do not exceed a hundred of nanoseconds. This means that the direct atomistic modeling of the material deformation can be done for the regimes with rather high strain rates at which the yield stress and other mechanical strength characteristics are controlled by microscopic mechanisms different from those at low (quasi-static) strain rates. In essence, the plastic properties of structural materials are determined by the dynamics of the extended defects of crystal structure (edge and screw dislocations) and by interactions between them and with the other defects in the crystal. In the present work we propose a method that is capable to model the dynamics of edge dislocations in the fcc and hcp materials at dynamic deformations and to estimate the material static yield stress in the states of interest in the frames of the atomistic approach. The method is based on the numerical characterization of the stress relaxation processes in specially generated samples containing solitary edge dislocations
Atomistic modeling of the dislocation dynamics and evaluation of static yield stress
Static strength characteristics of structural materials are of great importance for the analysis of the materials behaviour under mechanical loadings. Mechanical characteristics of structural materials such as elastic limit, strength limit, ultimate tensile strength, plasticity are, unlike elastic moduli, very sensitive to the presence of impurities and defects of crystal structure. Direct atomistic modeling of the static mechanical strength characteristics of real materials is an extremely difficult task since the typical time scales available for the direct modeling in the frames of classical molecular dynamics do not exceed a hundred of nanoseconds. This means that the direct atomistic modeling of the material deformation can be done for the regimes with rather high strain rates at which the yield stress and other mechanical strength characteristics are controlled by microscopic mechanisms different from those at low (quasi-static) strain rates. In essence, the plastic properties of structural materials are determined by the dynamics of the extended defects of crystal structure (edge and screw dislocations) and by interactions between them and with the other defects in the crystal. In the present work we propose a method that is capable to model the dynamics of edge dislocations in the fcc and hcp materials at dynamic deformations and to estimate the material static yield stress in the states of interest in the frames of the atomistic approach. The method is based on the numerical characterization of the stress relaxation processes in specially generated samples containing solitary edge dislocations
ΠΠΠ ΠΠΠΠ’Π« ΠΠ ΠΠΠ«ΠΠΠΠΠ― ΠΠΠΠΠΠ’ΠΠ«Π₯ ΠΠΠΠ ΠΠΠΠ«Π₯ Π’ΠΠ Π ΠΠΠΠ£ΠΠΠ§ΠΠ-ΠΠΠ¨ΠΠ§ΠΠΠ Π’Π ΠΠΠ’Π Π£ ΠΠΠ’ΠΠ
Magnetic foreign body in the digestive tract in children may have different ways to stay and outcomes. The authors present clinical examples of location, surgical removal of the magnetic bodies and the described case of complications as a result of multiple magnetic foreign bodies in the gastrointestinal tract. Developed clinical management of patients with suspected presence of magnetic foreign bodies in different sections of the gastrointestinal tract.ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΏΡΠΈΠΌΠ΅ΡΡ Π½Π°Ρ
ΠΎΠΆΠ΄Π΅Π½ΠΈΡ ΠΈ ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠ²Π½ΠΎΠ³ΠΎ ΡΠ΄Π°Π»Π΅Π½ΠΈΡ ΠΌΠ°Π³Π½ΠΈΡΠ½ΡΡ
ΠΎΠ±ΡΠ΅ΠΊΡΠΎΠ², ΠΎΠΏΠΈΡΠ°Π½Ρ ΡΠ»ΡΡΠ°ΠΈ ΡΠ°Π·Π²ΠΈΡΠΈΡ ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½ΠΈΠΉ Π² ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ ΠΌΠ½ΠΎΠΆΠ΅ΡΡΠ²Π΅Π½Π½ΠΎΠ³ΠΎ ΠΏΠΎΠΏΠ°Π΄Π°Π½ΠΈΡ ΠΌΠ°Π³Π½ΠΈΡΠ½ΡΡ
ΠΈΠ½ΠΎΡΠΎΠ΄Π½ΡΡ
ΡΠ΅Π» Π² ΠΆΠ΅Π»ΡΠ΄ΠΎΡΠ½ΠΎ-ΠΊΠΈΡΠ΅ΡΠ½ΡΠΉ ΡΡΠ°ΠΊΡ. ΠΡΡΠ°Π±ΠΎΡΠ°Π½Π° ΡΠ°ΠΊΡΠΈΠΊΠ° Π²Π΅Π΄Π΅Π½ΠΈΡ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ ΠΏΠΎΠ΄ΠΎΠ·ΡΠ΅Π½ΠΈΠ΅ΠΌ Π½Π° Π½Π°Π»ΠΈΡΠΈΠ΅ Ρ Π½ΠΈΡ
ΠΌΠ°Π³Π½ΠΈΡΠ½ΡΡ
ΠΈΠ½ΠΎΡΠΎΠ΄Π½ΡΡ
ΡΠ΅Π» Π² ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΠΎΡΠ΄Π΅Π»Π°Ρ
ΠΆΠ΅Π»ΡΠ΄ΠΎΡΠ½ΠΎ-ΠΊΠΈΡΠ΅ΡΠ½ΠΎΠ³ΠΎ ΡΡΠ°ΠΊΡΠ°
ΠΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΠ»ΡΡΠ°ΠΈ ΠΎΡΡΡΠΎΠ³ΠΎ Π°ΠΏΠΏΠ΅Π½Π΄ΠΈΡΠΈΡΠ° Ρ Π½ΠΎΠ²ΠΎΡΠΎΠΆΠ΄Π΅Π½Π½ΡΡ
Aim. The goal of this study is to describe the clinical observations of acute appendicitis in two newborn infants.
This study was a retrospective analysis performed using data obtained from medical records. Two preterm infants had a gestational age of 33 weeks, a threat of pregnancy termination, rapid childbirth in one case, and a cesarean section in another. At birth, their body weights were low, 2340 and 2420 g, respectively. The condition of the babies was evaluated on the Apgar scale, and both scored 7/8 points. We studied the data of clinical, laboratory, and instrumental study data and surgical intervention protocols.
In the presented newborns, neonatal jaundice, respiratory failure of the III degree, and hypoxic perinatal damage to the central nervous system occurred from birth. On the first childs twelfth day and the second childs ninth day, they experienced a clinically acute inflammatory process in the abdominal cavity, confirmed by inflammation markers (high white blood cell counts and levels of C-reactive protein). According to the sonography of the abdominal organs, the absence of intestinal motility in the right abdominal cavity, the presence of intestinal wall pneumatosis, signs of conglomerate formation from the intestinal loops were revealed. The surgical interventions performed were a laparoscopy and a conversion to laparotomy. In both cases, inflammatory bowel changes corresponded to the course of necrotic enterocolitis, diagnosed with gangrenous-perforated appendicitis and purulent-fibrinous peritonitis. In the section, the mucous appendix was not changed.
Conclusion. The aggravated premorbid background in premature infants predisposes them to necrotic enterocolitis, which can occur in children of this age with isolated perforation of the appendix. The course of necrotic enterocolitis is complicated by the formation of purulent-fibrinous peritonitis due to the destruction of the appendix with minimal changes in its walls.Π¦Π΅Π»Ρ. ΠΠΏΠΈΡΠ°ΡΡ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π½Π°Π±Π»ΡΠ΄Π΅Π½ΠΈΡ ΠΎΡΡΡΠΎΠ³ΠΎ Π°ΠΏΠΏΠ΅Π½Π΄ΠΈΡΠΈΡΠ° Ρ Π΄Π΅ΡΠ΅ΠΉ ΠΏΠ΅ΡΠΈΠΎΠ΄Π° Π½ΠΎΠ²ΠΎΡΠΎΠΆΠ΄Π΅Π½Π½ΠΎΡΡΠΈ.
Π Π΅ΡΡΠΎΡΠΏΠ΅ΠΊΡΠΈΠ²Π½ΡΠΉ Π°Π½Π°Π»ΠΈΠ· ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΈΡ
ΠΊΠ°ΡΡ: 2 Π½Π΅Π΄ΠΎΠ½ΠΎΡΠ΅Π½Π½ΡΡ
ΠΌΠ»Π°Π΄Π΅Π½ΡΠ°, Π²ΠΎΠ·ΡΠ°ΡΡ Π³Π΅ΡΡΠ°ΡΠΈΠΈ 33 Π½Π΅Π΄Π΅Π»ΠΈ, ΡΠ³ΡΠΎΠ·Π° ΠΏΡΠ΅ΡΡΠ²Π°Π½ΠΈΡ Π±Π΅ΡΠ΅ΠΌΠ΅Π½Π½ΠΎΡΡΠΈ, ΡΡΡΠ΅ΠΌΠΈΡΠ΅Π»ΡΠ½ΡΠ΅ ΡΠΎΠ΄Ρ Π² ΠΎΠ΄Π½ΠΎΠΌ ΡΠ»ΡΡΠ°Π΅ ΠΈ ΠΊΠ΅ΡΠ°ΡΠ΅Π²ΠΎ ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ Π² Π΄ΡΡΠ³ΠΎΠΌ. ΠΡΠΈ ΡΠΎΠΆΠ΄Π΅Π½ΠΈΠΈ ΠΌΠ°ΡΡΠ° ΡΠ΅Π»Π° Π½ΠΈΠ·ΠΊΠ°Ρ 2340 ΠΈ 2420 Π³ ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²Π΅Π½Π½ΠΎ. Π‘ΠΎΡΡΠΎΡΠ½ΠΈΠ΅ ΠΌΠ°Π»ΡΡΠ΅ΠΉ ΠΎΡΠ΅Π½ΠΈΠ²Π°Π»ΠΎΡΡ ΠΏΠΎ ΡΠΊΠ°Π»Π΅ ΠΠΏΠ³Π°Ρ 7/8 Π±Π°Π»Π»ΠΎΠ² Π² ΠΎΠ±ΠΎΠΈΡ
ΡΠ»ΡΡΠ°ΡΡ
. ΠΠ·ΡΡΠ°Π»ΠΈ Π΄Π°Π½Π½ΡΠ΅ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΡ
, Π»Π°Π±ΠΎΡΠ°ΡΠΎΡΠ½ΡΡ
ΠΈ ΠΈΠ½ΡΡΡΡΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΡΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ, ΠΏΡΠΎΡΠΎΠΊΠΎΠ»Ρ Π²ΡΠΏΠΎΠ»Π½Π΅Π½Π½ΡΡ
ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠ²Π½ΡΡ
Π²ΠΌΠ΅ΡΠ°ΡΠ΅Π»ΡΡΡΠ².
Π£ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Π½ΡΡ
Π½ΠΎΠ²ΠΎΡΠΎΠΆΠ΄Π΅Π½Π½ΡΡ
Ρ ΡΠΎΠΆΠ΄Π΅Π½ΠΈΡ ΠΏΡΠΎΡΠ΅ΠΊΠ°Π»Π° Π½Π΅ΠΎΠ½Π°ΡΠ°Π»ΡΠ½Π°Ρ ΠΆΠ΅Π»ΡΡΡ
Π°, Π΄ΡΡ
Π°ΡΠ΅Π»ΡΠ½Π°Ρ Π½Π΅Π΄ΠΎΡΡΠ°ΡΠΎΡΠ½ΠΎΡΡΡ III ΡΡΠ΅ΠΏΠ΅Π½ΠΈ, Π³ΠΈΠΏΠΎΠΊΡΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΠΏΠ΅ΡΠΈΠ½Π°ΡΠ°Π»ΡΠ½ΠΎΠ΅ ΠΏΠΎΡΠ°ΠΆΠ΅Π½ΠΈΠ΅ ΡΠ΅Π½ΡΡΠ°Π»ΡΠ½ΠΎΠΉ Π½Π΅ΡΠ²Π½ΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ. ΠΠ° 12-Π΅ ΡΡΡΠΊΠΈ Ρ ΠΏΠ΅ΡΠ²ΠΎΠ³ΠΎ ΠΈ 9-Π΅ ΡΡΡΠΊΠΈ Ρ Π²ΡΠΎΡΠΎΠ³ΠΎ ΡΠ΅Π±Π΅Π½ΠΊΠ° Π²ΠΎΠ·Π½ΠΈΠΊΠ»Π° ΠΊΠ»ΠΈΠ½ΠΈΠΊΠ° ΠΎΡΡΡΠΎΠ³ΠΎ Π²ΠΎΡΠΏΠ°Π»ΠΈΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ ΠΏΡΠΎΡΠ΅ΡΡΠ° Π² Π±ΡΡΡΠ½ΠΎΠΉ ΠΏΠΎΠ»ΠΎΡΡΠΈ, ΠΏΠΎΠ΄ΡΠ²Π΅ΡΠΆΠ΄Π΅Π½Π½Π°Ρ ΠΌΠ°ΡΠΊΠ΅ΡΠ°ΠΌΠΈ Π²ΠΎΡΠΏΠ°Π»Π΅Π½ΠΈΡ (Π²ΡΡΠΎΠΊΠΈΠ΅ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»ΠΈ Π»Π΅ΠΉΠΊΠΎΡΠΈΡΠΎΠ² ΠΈ ΡΡΠΎΠ²Π½Π΅ΠΉ Π‘-ΡΠ΅Π°ΠΊΡΠΈΠ²Π½ΠΎΠ³ΠΎ Π±Π΅Π»ΠΊΠ°). ΠΠΎ Π΄Π°Π½Π½ΡΠΌ ΡΠΎΠ½ΠΎΠ³ΡΠ°ΡΠΈΠΈ ΠΎΡΠ³Π°Π½ΠΎΠ² Π±ΡΡΡΠ½ΠΎΠΉ ΠΏΠΎΠ»ΠΎΡΡΠΈ Π²ΡΡΠ²Π»Π΅Π½ΠΎ ΠΎΡΡΡΡΡΡΠ²ΠΈΠ΅ ΠΏΠ΅ΡΠΈΡΡΠ°Π»ΡΡΠΈΠΊΠΈ ΠΊΠΈΡΠ΅ΡΠ½ΠΈΠΊΠ° Π² ΠΏΡΠ°Π²ΡΡ
ΠΎΡΠ΄Π΅Π»Π°Ρ
Π±ΡΡΡΠ½ΠΎΠΉ ΠΏΠΎΠ»ΠΎΡΡΠΈ, Π½Π°Π»ΠΈΡΠΈΠ΅ ΠΏΠ½Π΅Π²ΠΌΠ°ΡΠΎΠ·Π° ΠΊΠΈΡΠ΅ΡΠ½ΠΎΠΉ ΡΡΠ΅Π½ΠΊΠΈ, ΠΏΡΠΈΠ·Π½Π°ΠΊΠΈ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΊΠΎΠ½Π³Π»ΠΎΠΌΠ΅ΡΠ°ΡΠ° ΠΈΠ· ΠΏΠ΅ΡΠ΅Π»Ρ ΠΊΠΈΡΠ΅ΡΠ½ΠΈΠΊΠ°. ΠΠΏΠ΅ΡΠ°ΡΠΈΠ²Π½ΠΎΠ΅ Π²ΠΌΠ΅ΡΠ°ΡΠ΅Π»ΡΡΡΠ²ΠΎ: Π»Π°ΠΏΠ°ΡΠΎΡΠΊΠΎΠΏΠΈΡ, ΠΊΠΎΠ½Π²Π΅ΡΡΠΈΡ Π½Π° Π»Π°ΠΏΠ°ΡΠΎΡΠΎΠΌΠΈΡ. Π ΠΎΠ±ΠΎΠΈΡ
ΡΠ»ΡΡΠ°ΡΡ
Π²ΠΎΡΠΏΠ°Π»ΠΈΡΠ΅Π»ΡΠ½ΡΠ΅ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΊΠΈΡΠ΅ΡΠ½ΠΈΠΊΠ° ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΠΎΠ²Π°Π»ΠΈ ΡΠ΅ΡΠ΅Π½ΠΈΡ Π½Π΅ΠΊΡΠΎΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠ½ΡΠ΅ΡΠΎΠΊΠΎΠ»ΠΈΡΠ°, Π΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΡΠΎΠ²Π°Π½ Π³Π°Π½Π³ΡΠ΅Π½ΠΎΠ·Π½ΠΎ-ΠΏΠ΅ΡΡΠΎΡΠ°ΡΠΈΠ²Π½ΡΠΉ Π°ΠΏΠΏΠ΅Π½Π΄ΠΈΡΠΈΡ ΠΈ Π³Π½ΠΎΠΉΠ½ΠΎ-ΡΠΈΠ±ΡΠΈΠ½ΠΎΠ·Π½ΡΠΉ ΠΏΠ΅ΡΠΈΡΠΎΠ½ΠΈΡ. ΠΠ° ΡΠ°Π·ΡΠ΅Π·Π΅ ΡΠ»ΠΈΠ·ΠΈΡΡΠ°Ρ Π°ΠΏΠΏΠ΅Π½Π΄ΠΈΠΊΡΠ° Π½Π΅ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½Π°.
ΠΠ°ΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅. ΠΡΡΠ³ΠΎΡΠ΅Π½Π½ΡΠΉ ΠΏΡΠ΅ΠΌΠΎΡΠ±ΠΈΠ΄Π½ΡΠΉ ΡΠΎΠ½ Ρ Π½Π΅Π΄ΠΎΠ½ΠΎΡΠ΅Π½Π½ΡΡ
Π½ΠΎΠ²ΠΎΡΠΎΠΆΠ΄Π΅Π½Π½ΡΡ
ΠΏΡΠ΅Π΄ΡΠ°ΡΠΏΠΎΠ»Π°Π³Π°Π΅Ρ Π²ΠΎΠ·Π½ΠΈΠΊΠ½ΠΎΠ²Π΅Π½ΠΈΡ Π½Π΅ΠΊΡΠΎΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠ½ΡΠ΅ΡΠΎΠΊΠΎΠ»ΠΈΡΠ°, ΠΊΠΎΡΠΎΡΡΠΉ Ρ Π΄Π΅ΡΠ΅ΠΉ Π΄Π°Π½Π½ΠΎΠ³ΠΎ Π²ΠΎΠ·ΡΠ°ΡΡΠ° ΠΌΠΎΠΆΠ΅Ρ ΠΏΡΠΎΡΠ΅ΠΊΠ°ΡΡ Ρ ΠΈΠ·ΠΎΠ»ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ ΠΏΠ΅ΡΡΠΎΡΠ°ΡΠΈΠ΅ΠΉ ΡΠ΅ΡΠ²Π΅ΠΎΠ±ΡΠ°Π·Π½ΠΎΠ³ΠΎ ΠΎΡΡΠΎΡΡΠΊΠ°. Π’Π΅ΡΠ΅Π½ΠΈΠ΅ Π½Π΅ΠΊΡΠΎΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠ½ΡΠ΅ΡΠΎΠΊΠΎΠ»ΠΈΡΠ° ΠΎΡΠ»ΠΎΠΆΠ½ΡΠ΅ΡΡΡ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π³Π½ΠΎΠΉΠ½ΠΎ-ΡΠΈΠ±ΡΠΈΠ½ΠΎΠ·Π½ΠΎΠ³ΠΎ ΠΏΠ΅ΡΠΈΡΠΎΠ½ΠΈΡΠ° Π·Π° ΡΡΠ΅Ρ Π΄Π΅ΡΡΡΡΠΊΡΠΈΠΈ Π°ΠΏΠΏΠ΅Π½Π΄ΠΈΠΊΡΠ° ΠΏΡΠΈ ΠΌΠΈΠ½ΠΈΠΌΠ°Π»ΡΠ½ΡΡ
ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡΡ
Π² Π΅Π³ΠΎ ΡΡΠ΅Π½ΠΊΠ°Ρ
MD modeling of screw dislocation influence upon initiation and mechanism of BCC-HCP polymorphous transition in iron
The present work is devoted to classical molecular dynamics investigation into microscopic mechanisms of the bcc-hcp transition in iron. The interatomic potential of EAM type used in the calculations was tested for the capability to reproduce ab initio data on energy evolution along the bcc-hcp transformation path (Burgers deformation + shuο¬e) and then used in the large-scale MD simulations. The large-scale simulations included constant volume deformation along the Burgers path to study the origin and nature of the plasticity, hydrostatic volume compression of defect free samples above the bcc to hcp transition threshold to observe the formation of new phase embryos, and the volume compression of samples containing screw dislocations to study the effect of the dislocations on the probability of the new phase critical embryo formation. The volume compression demonstrated high level of metastability. The transition starts at pressure much higher than the equilibrium one. Dislocations strongly affect the probability of the critical embryo formation and significantly reduce the onset pressure of transition. The dislocations affect also the resulting structure of the samples upon the transition. The formation of layered structure is typical for the samples containing the dislocations. The results of the simulations were compared with the in-situ experimental data on the mechanism of the bcc-hcp transition in iron
MD modeling of screw dislocation influence upon initiation and mechanism of BCC-HCP polymorphous transition in iron
The present work is devoted to classical molecular dynamics investigation into microscopic mechanisms of the bcc-hcp transition in iron. The interatomic potential of EAM type used in the calculations was tested for the capability to reproduce ab initio data on energy evolution along the bcc-hcp transformation path (Burgers deformation + shuο¬e) and then used in the large-scale MD simulations. The large-scale simulations included constant volume deformation along the Burgers path to study the origin and nature of the plasticity, hydrostatic volume compression of defect free samples above the bcc to hcp transition threshold to observe the formation of new phase embryos, and the volume compression of samples containing screw dislocations to study the effect of the dislocations on the probability of the new phase critical embryo formation. The volume compression demonstrated high level of metastability. The transition starts at pressure much higher than the equilibrium one. Dislocations strongly affect the probability of the critical embryo formation and significantly reduce the onset pressure of transition. The dislocations affect also the resulting structure of the samples upon the transition. The formation of layered structure is typical for the samples containing the dislocations. The results of the simulations were compared with the in-situ experimental data on the mechanism of the bcc-hcp transition in iron
Structure and tribological behavior of submicrocrystalline titanium modified with nitrogen ions
MD modeling of screw dislocation influence upon initiation and mechanism of BCC-HCP polymorphous transition in iron
The present work is devoted to classical molecular dynamics investigation into microscopic mechanisms of the bcc-hcp transition in iron. The interatomic potential of EAM type used in the calculations was tested for the capability to reproduce ab initio data on energy evolution along the bcc-hcp transformation path (Burgers deformation + shuο¬e) and then used in the large-scale MD simulations. The large-scale simulations included constant volume deformation along the Burgers path to study the origin and nature of the plasticity, hydrostatic volume compression of defect free samples above the bcc to hcp transition threshold to observe the formation of new phase embryos, and the volume compression of samples containing screw dislocations to study the effect of the dislocations on the probability of the new phase critical embryo formation. The volume compression demonstrated high level of metastability. The transition starts at pressure much higher than the equilibrium one. Dislocations strongly affect the probability of the critical embryo formation and significantly reduce the onset pressure of transition. The dislocations affect also the resulting structure of the samples upon the transition. The formation of layered structure is typical for the samples containing the dislocations. The results of the simulations were compared with the in-situ experimental data on the mechanism of the bcc-hcp transition in iron