7 research outputs found
Π’Π΅ΡΠΌΠΎΠΊΠΈΠ½Π΅ΡΠΈΡΠ΅ΡΠΊΠ°Ρ ΠΠΠ‘ ΠΏΡΠΈ ΠΎΠ±ΡΠ°ΡΠ½ΠΎΠΌ ΡΠ°Π·ΠΎΠ²ΠΎΠΌ ΠΏΠ΅ΡΠ΅Ρ ΠΎΠ΄Π΅ Π² Π½ΠΈΠΊΠ΅Π»ΠΈΠ΄Π΅ ΡΠΈΡΠ°Π½Π° ΠΊΠ°ΠΊ ΡΠΏΠΎΡΠΎΠ± Π·Π°ΠΏΠΈΡΠΈ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠΈ
The external factors that inο¬uence on the thermokinetic EMF value in the Ti β 50 at.% Ni samples were determined. A method for setting thermokinetic EMF in certain sections of the TiNi wire was developed. The thermokinetic EMF value was measured directly using a digital millivoltmeter MNIPI V7-72. The sections of the Ti β 50 at.% Ni wire samples were subjected to tensile tests on a tensile machine IP 5158-5. On the basis of calorimetric studies, the kinetics of martensitic transformations was investigated. It was found that the direct phase transition affects the thermokinetic EMF value of the Ti β 50 at.% Ni during thermal cycling. Thermal cycling in the temperature range of the complete martensitic transformation causes the thermokinetic EMF value reduction by 0.16 mV by the 15th temperature cycle. The degradation of the thermokinetic EMF value by 0.04 mV took place during thermal cycling in the temperature range of the incomplete martensitic transformation by the 70th thermal cycle. The thermokinetic EMF value was restored to 0.22 mV with increasing temperature to 240 Β°Π‘, as in the case of annealing at temperatures of 400Γ·800 Β°Π‘. The thermokinetic EMF value is associated with a change in physical and mechanical properties of the alloy during thermal cycling. It is characterized by a change in stages of the phase transition and a shift of the characteristic temperatures. On the basis of the obtained experimental data, a method was proposed for a purposeful setting of extended TiNi wire sections with the thermokinetic EMF value from 0 to 0.6 mV, using different methods of inο¬uence on its value (thermal cycling, deformation, temperature change in heating zone). The proposed technical solution can be used as a method for information recording.Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½Ρ Π·Π°ΠΊΠΎΠ½ΠΎΠΌΠ΅ΡΠ½ΠΎΡΡΠΈ Π²Π»ΠΈΡΠ½ΠΈΡ Π²Π½Π΅ΡΠ½ΠΈΡ
ΡΠ°ΠΊΡΠΎΡΠΎΠ² Π½Π° ΡΠ΅ΡΠΌΠΎΠΊΠΈΠ½Π΅ΡΠΈΡΠ΅ΡΠΊΡΡ ΠΠΠ‘ Π² ΠΎΠ±ΡΠ°Π·ΡΠ°Ρ
Ti β 50 Π°Ρ.% Ni, Π° ΡΠ°ΠΊΠΆΠ΅ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠ°Π½ ΡΠΏΠΎΡΠΎΠ± Π·Π°Π΄Π°Π½ΠΈΡ ΡΠ΅ΡΠΌΠΎΠΊΠΈΠ½Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΠΠ‘ Π½Π° ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½Π½ΡΡ
ΡΡΠ°ΡΡΠΊΠ°Ρ
TiNi-ΠΏΡΠΎΠ²ΠΎΠ»ΠΎΠΊΠΈ. Π’Π΅ΡΠΌΠΎΠΊΠΈΠ½Π΅ΡΠΈΡΠ΅ΡΠΊΡΡ ΠΠΠ‘ ΠΈΠ·ΠΌΠ΅ΡΡΠ»ΠΈ ΠΏΡΡΠΌΡΠΌ ΡΠΏΠΎΡΠΎΠ±ΠΎΠΌ Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΡΠΈΡΡΠΎΠ²ΠΎΠ³ΠΎ ΠΌΠΈΠ»Π»ΠΈΠ²ΠΎΠ»ΡΡΠΌΠ΅ΡΡΠ° ΠΠΠΠΠ Π7-72. ΠΠ΅ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΡΡΠ°ΡΡΠΊΠΎΠ² ΠΏΡΠΎΠ²ΠΎΠ»ΠΎΡΠ½ΡΡ
ΠΎΠ±ΡΠ°Π·ΡΠΎΠ² Ti β 50 Π°Ρ.% Ni ΠΎΡΡΡΠ΅ΡΡΠ²Π»ΡΠ»ΠΈ Π½Π° ΠΈΡΠΏΡΡΠ°ΡΠ΅Π»ΡΠ½ΠΎΠΉ ΠΌΠ°ΡΠΈΠ½Π΅ ΠΠ 5158-5. ΠΠ° ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΠΈ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ² ΠΊΠ°Π»ΠΎΡΠΈΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π»ΠΈ ΠΊΠΈΠ½Π΅ΡΠΈΠΊΡ ΠΌΠ°ΡΡΠ΅Π½ΡΠΈΡΠ½ΡΡ
ΠΏΡΠ΅Π²ΡΠ°ΡΠ΅Π½ΠΈΠΉ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ Π½Π° Π²Π΅Π»ΠΈΡΠΈΠ½Ρ ΡΠ΅ΡΠΌΠΎΠΊΠΈΠ½Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΠΠ‘ Ti β 50 Π°Ρ.% Ni ΠΏΡΠΈ ΡΠ΅ΡΠΌΠΎΡΠΈΠΊΠ»ΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ Π²Π»ΠΈΡΠ΅Ρ ΡΡΠ΅ΠΏΠ΅Π½Ρ ΠΏΡΡΠΌΠΎΠ³ΠΎ ΡΠ°Π·ΠΎΠ²ΠΎΠ³ΠΎ ΠΏΠ΅ΡΠ΅Ρ
ΠΎΠ΄Π°. Π’Π΅ΡΠΌΠΎΡΠΈΠΊΠ»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ Π² ΠΈΠ½ΡΠ΅ΡΠ²Π°Π»Π΅ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡ ΠΏΠΎΠ»Π½ΠΎΠ³ΠΎ ΠΌΠ°ΡΡΠ΅Π½ΡΠΈΡΠ½ΠΎΠ³ΠΎ ΠΏΡΠ΅Π²ΡΠ°ΡΠ΅Π½ΠΈΡ ΠΊ 15-ΠΌΡ ΡΠ΅ΡΠΌΠΎΡΠΈΠΊΠ»Ρ ΡΡΠ°Π±ΠΈΠ»ΠΈΠ·ΠΈΡΡΠ΅Ρ Π·Π½Π°ΡΠ΅Π½ΠΈΡ ΡΠ΅ΡΠΌΠΎΠΊΠΈΠ½Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΠΠ‘ Π½Π° 0,16 ΠΌΠ. Π’ΠΎΠ³Π΄Π° ΠΊΠ°ΠΊ ΡΠ΅ΡΠΌΠΎΡΠΈΠΊΠ»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ Π² ΠΈΠ½ΡΠ΅ΡΠ²Π°Π»Π΅ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡ Π½Π΅ΠΏΠΎΠ»Π½ΠΎΠ³ΠΎ ΠΌΠ°ΡΡΠ΅Π½ΡΠΈΡΠ½ΠΎΠ³ΠΎ ΠΏΡΠ΅Π²ΡΠ°ΡΠ΅Π½ΠΈΡ ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡ ΠΊ Π²ΡΡΠΎΠΆΠ΄Π΅Π½ΠΈΡ ΡΠ΅ΡΠΌΠΎΠΊΠΈΠ½Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΠΠ‘: ΠΊ 70-ΠΌΡ ΡΠ΅ΡΠΌΠΎΡΠΈΠΊΠ»Ρ ΠΎΠ½Π° ΡΠΎΡΡΠ°Π²Π»ΡΠ΅Ρ 0,04 ΠΌΠ. Π£Π²Π΅Π»ΠΈΡΠ΅Π½ΠΈΠ΅ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ Π² Π·ΠΎΠ½Π΅ Π½Π°Π³ΡΠ΅Π²Π° Π΄ΠΎ 240 Β°Π‘ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ Π²ΠΎΡΡΡΠ°Π½ΠΎΠ²ΠΈΡΡ Π·Π½Π°ΡΠ΅Π½ΠΈΠ΅ ΡΠ΅ΡΠΌΠΎΠΊΠΈΠ½Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΠΠ‘ Π΄ΠΎ 0,22 ΠΌΠ, ΠΊΠ°ΠΊ ΠΈ Π΄Π»Ρ ΡΠ»ΡΡΠ°Ρ ΠΎΡΠΆΠΈΠ³Π° ΠΏΡΠΈ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ°Ρ
400Γ·800 Β°Π‘. ΠΠ΅Π»ΠΈΡΠΈΠ½Π° ΡΠ΅ΡΠΌΠΎΠΊΠΈΠ½Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΠΠ‘ ΠΏΡΠΈ ΡΠ΅ΡΠΌΠΎΡΠΈΠΊΠ»ΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ ΡΠ²ΡΠ·Π°Π½Π° Ρ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ ΡΠΈΠ·ΠΈΠΊΠΎ-ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ²ΠΎΠΉΡΡΠ² ΡΠΏΠ»Π°Π²Π° ΠΈ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΠ·ΡΠ΅ΡΡΡ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ ΡΡΠ°Π΄ΠΈΠΉΠ½ΠΎΡΡΠΈ ΠΈ ΡΠΌΠ΅ΡΠ΅Π½ΠΈΠ΅ΠΌ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡ ΡΠ°Π·ΠΎΠ²ΠΎΠ³ΠΎ ΠΏΠ΅ΡΠ΅Ρ
ΠΎΠ΄Π°. ΠΠ° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΡΡ
Π΄Π°Π½Π½ΡΡ
ΠΏΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½ ΡΠΏΠΎΡΠΎΠ± ΡΠ΅Π»Π΅Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½Π½ΠΎΠ³ΠΎ Π·Π°Π΄Π°Π½ΠΈΡ ΠΏΡΠΎΡΡΠΆΠ΅Π½Π½ΡΡ
ΡΡΠ°ΡΡΠΊΠΎΠ² TiNi-ΠΏΡΠΎΠ²ΠΎΠ»ΠΎΠΊΠΈ ΡΠΎ Π·Π½Π°ΡΠ΅Π½ΠΈΠ΅ΠΌ ΡΠ΅ΡΠΌΠΎΠΊΠΈΠ½Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΠΠ‘ ΠΎΡ 0 Π΄ΠΎ 0,6 ΠΌΠ, ΠΈΡΠΏΠΎΠ»ΡΠ·ΡΡ ΡΠ°Π·Π»ΠΈΡΠ½ΡΠ΅ ΡΠΏΠΎΡΠΎΠ±Ρ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΡ (ΡΠ΅ΡΠΌΠΎΡΠΈΠΊΠ»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅, Π΄Π΅ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅, ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ Π² Π·ΠΎΠ½Π΅ Π½Π°Π³ΡΠ΅Π²Π°) Π½Π° Π΅Π΅ Π²Π΅Π»ΠΈΡΠΈΠ½Ρ. ΠΡΠ΅Π΄Π»Π°Π³Π°Π΅ΠΌΠΎΠ΅ ΡΠ΅Ρ
Π½ΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΎ Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΡΠΏΠΎΡΠΎΠ±Π° Π·Π°ΠΏΠΈΡΠΈ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠΈ
ΠΠ»ΠΈΡΠ½ΠΈΠ΅ ΡΠ΅ΡΠΌΠΎΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠΈ Π½Π° Π²Π΅Π»ΠΈΡΠΈΠ½Ρ ΡΠ΅ΡΠΌΠΎΠΊΠΈΠ½Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΠΠ‘ ΠΏΡΠΈ ΠΎΠ±ΡΠ°ΡΠ½ΠΎΠΌ ΡΠ°Π·ΠΎΠ²ΠΎΠΌ ΠΏΠ΅ΡΠ΅Ρ ΠΎΠ΄Π΅ Π² Π½ΠΈΠΊΠ΅Π»ΠΈΠ΄Π΅ ΡΠΈΡΠ°Π½Π°
The effect of duration and annealing temperature in the range of 400β800 Β°C on the thermokinetic EMF value in titanium nickelide, the composition of which is close to the equi-atomic one, at a reverse phase transition was investigated. Thermokinetic EMF was measured directly using a digital millivoltmeter MNIPI V7-72. The phase and elemental composition of the alloy and the kinetics of thermoelastic phase transformations have been checked by X-ray diffraction and calorimetric studies, and X-ray microanalysis. Annealing at temperatures of 500 and 800 Β°C leads to an increase in theΒ thermokinetic EMF value from 0.22 to 0.25 mV. Removal of the oxide layer from the sample surface annealed at 700 Β°C for 0.5 h leads to an increase in the thermokinetic EMF value from 0.22 to 0.26 mV for the 1-st thermal cycle. It was found that thermal cycling causes a decrease in the thermokinetic EMF values down to 0.98 mV for the 20th thermal cycle for the samples without an oxide layer and to 0.3 mV for the samples with an oxide layer, respectively. With the increase in annealing time up to 20 h at 700 Β°C, the decrease in the thermokinetic emf value to 0.16 mV was observed. The thermokinetic EMF value after heat treatment is associated with changes in the physical and mechanical properties of the alloy and characterized by a shift of the characteristic temperatures of the phase transition. The research results are important for understanding the physics of thermoelectric phenomena in shape memory alloys during nonstationary heating and can be used both to control the homogeneity of their physical and mechanical properties and to design smart actuators and sensors, mechanisms of control systems.ΠΠΏΡΠ΅Π΄Π΅Π»Π΅Π½Π° Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΡ ΡΠ΅ΡΠΌΠΎΠΊΠΈΠ½Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΠΠ‘ ΠΏΡΠΈ ΠΎΠ±ΡΠ°ΡΠ½ΠΎΠΌ ΡΠ°Π·ΠΎΠ²ΠΎΠΌ ΠΏΠ΅ΡΠ΅Ρ
ΠΎΠ΄Π΅ Π² Π½ΠΈΠΊΠ΅Π»ΠΈΠ΄Π΅ ΡΠΈΡΠ°Π½Π° ΡΠΎΡΡΠ°Π²Π°, Π±Π»ΠΈΠ·ΠΊΠΎΠ³ΠΎ ΠΊ ΡΠΊΠ²ΠΈΠ°ΡΠΎΠΌΠ½ΠΎΠΌΡ, ΠΎΡ ΠΏΡΠΎΠ΄ΠΎΠ»ΠΆΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΠΈ ΠΈ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ ΠΎΡΠΆΠΈΠ³Π° Π² ΠΈΠ½ΡΠ΅ΡΠ²Π°Π»Π΅ 400Γ·800 Β°Π‘. Π’Π΅ΡΠΌΠΎΠΊΠΈΠ½Π΅ΡΠΈΡΠ΅ΡΠΊΡΡ ΠΠΠ‘ ΠΈΠ·ΠΌΠ΅ΡΡΠ»ΠΈ ΠΏΡΡΠΌΡΠΌ ΡΠΏΠΎΡΠΎΠ±ΠΎΠΌ Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΡΠΈΡΡΠΎΠ²ΠΎΠ³ΠΎ ΠΌΠΈΠ»Π»ΠΈΠ²ΠΎΠ»ΡΡΠΌΠ΅ΡΡΠ° ΠΠΠΠΠ Π7-72. ΠΠ½Π°Π»ΠΈΠ· ΡΠ°Π·ΠΎΠ²ΠΎΠ³ΠΎ, ΡΠ»Π΅ΠΌΠ΅Π½ΡΠ½ΠΎΠ³ΠΎ ΡΠΎΡΡΠ°Π²Π° ΡΠΏΠ»Π°Π²Π° ΠΈ ΠΊΠΈΠ½Π΅ΡΠΈΠΊΡ ΡΠ΅ΡΠΌΠΎΡΠΏΡΡΠ³ΠΈΡ
ΡΠ°Π·ΠΎΠ²ΡΡ
ΠΏΡΠ΅Π²ΡΠ°ΡΠ΅Π½ΠΈΠΉ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ Π½Π° ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΠΈ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ² ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΡΡΡΡΠΊΡΡΡΠ½ΡΡ
ΠΈ ΠΊΠ°Π»ΠΎΡΠΈΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ, ΠΌΠΈΠΊΡΠΎΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΡΠΏΠ΅ΠΊΡΡΠ°Π»ΡΠ½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π°. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ ΠΎΡΠΆΠΈΠ³ ΠΏΡΠΈ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ΅ 500 ΠΈ 800 Β°Π‘ ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡ ΠΊ ΡΠΎΡΡΡ ΡΠ΅ΡΠΌΠΎΠΊΠΈΠ½Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΠΠ‘ ΠΎΡ 0,22 Π΄ΠΎ 0,25 ΠΌΠ. Π£Π΄Π°Π»Π΅Π½ΠΈΠ΅ ΠΎΠΊΡΠΈΠ΄Π½ΠΎΠ³ΠΎ ΡΠ»ΠΎΡ Ρ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ ΠΎΠ±ΡΠ°Π·ΡΠ° ΠΏΠΎΡΠ»Π΅ ΠΎΡΠΆΠΈΠ³Π° ΠΏΡΠΈ 700 Β°Π‘ Π² ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ 0,5 Ρ ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡ ΠΊ ΡΠΎΡΡΡ Π²Π΅Π»ΠΈΡΠΈΠ½Ρ ΡΠ΅ΡΠΌΠΎΠΊΠΈΠ½Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΠΠ‘ Π² ΠΏΠ΅ΡΠ²ΠΎΠΌ ΡΠ΅ΡΠΌΠΎΡΠΈΠΊΠ»Π΅ ΠΎΡ 0,22 Π΄ΠΎ 0,26 ΠΌΠ. Π’Π΅ΡΠΌΠΎΡΠΈΠΊΠ»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΠΎΠ±ΡΠ°Π·ΡΠΎΠ² Π±Π΅Π· ΠΎΠΊΡΠΈΠ΄Π½ΠΎΠ³ΠΎ ΡΠ»ΠΎΡ Π²ΡΠ·ΡΠ²Π°Π΅Ρ ΡΠΌΠ΅Π½ΡΡΠ΅Π½ΠΈΠ΅ ΡΠ΅ΡΠΌΠΎΠΊΠΈΠ½Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΠΠ‘ Π·Π° 20 ΡΠ΅ΡΠΌΠΎΡΠΈΠΊΠ»ΠΎΠ² Π΄ΠΎ 0,98 ΠΌΠ, Π° ΠΏΡΠΈ Π½Π°Π»ΠΈΡΠΈΠΈ ΠΎΠΊΡΠΈΠ΄Π½ΠΎΠ³ΠΎ ΡΠ»ΠΎΡ β Π΄ΠΎ 0,3ΠΌΠ. Π£Π²Π΅Π»ΠΈΡΠ΅Π½ΠΈΠ΅ Π²ΡΠ΅ΠΌΠ΅Π½ΠΈ ΠΎΡΠΆΠΈΠ³Π° ΠΏΡΠΈ 700 Β°Π‘ Π΄ΠΎ 20 Ρ ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡ ΠΊ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΡ ΡΠ΅ΡΠΌΠΎΠΊΠΈΠ½Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΠΠ‘ Π΄ΠΎ 0,16 ΠΌΠ. ΠΠ΅Π»ΠΈΡΠΈΠ½Π° ΡΠ΅ΡΠΌΠΎΠΊΠΈΠ½Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΠΠ‘ ΠΏΠΎΡΠ»Π΅ ΡΠ΅ΡΠΌΠΎΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠΈ ΡΠ²ΡΠ·Π°Π½Π° Ρ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ ΡΠΈΠ·ΠΈΠΊΠΎ-ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ²ΠΎΠΉΡΡΠ² ΡΠΏΠ»Π°Π²Π° ΠΈ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΠ·ΡΠ΅ΡΡΡ ΡΠΌΠ΅ΡΠ΅Π½ΠΈΠ΅ΠΌ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡ ΡΠ°Π·ΠΎΠ²ΠΎΠ³ΠΎ ΠΏΠ΅ΡΠ΅Ρ
ΠΎΠ΄Π°. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ Π²Π°ΠΆΠ½Ρ Π΄Π»Ρ ΠΏΠΎΠ½ΠΈΠΌΠ°Π½ΠΈΡ ΡΠΈΠ·ΠΈΠΊΠΈ ΠΏΡΠΎΡΠ΅ΠΊΠ°Π½ΠΈΡ ΡΠ΅ΡΠΌΠΎΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ²Π»Π΅Π½ΠΈΠΉ Π² ΡΠΏΠ»Π°Π²Π°Ρ
Ρ ΡΡΡΠ΅ΠΊΡΠΎΠΌ ΠΏΠ°ΠΌΡΡΠΈ ΡΠΎΡΠΌΡ ΠΏΡΠΈ Π½Π΅ΡΡΠ°ΡΠΈΠΎΠ½Π°ΡΠ½ΠΎΠΌ Π½Π°Π³ΡΠ΅Π²Π΅ ΠΈ ΠΌΠΎΠ³ΡΡ Π±ΡΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½Ρ ΠΊΠ°ΠΊ Π΄Π»Ρ ΠΊΠΎΠ½ΡΡΠΎΠ»Ρ ΠΎΠ΄Π½ΠΎΡΠΎΠ΄Π½ΠΎΡΡΠΈ ΠΈΡ
ΡΠΈΠ·ΠΈΠΊΠΎ-ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ²ΠΎΠΉΡΡΠ², ΡΠ°ΠΊ ΠΈ ΠΏΡΠΈ ΠΏΡΠΎΠ΅ΠΊΡΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ ΠΈΡΠΏΠΎΠ»Π½ΠΈΡΠ΅Π»ΡΠ½ΡΡ
ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ², ΠΈΠ½ΡΠ΅Π»Π»Π΅ΠΊΡΡΠ°Π»ΡΠ½ΡΡ
Π΄Π°ΡΡΠΈΠΊΠΎΠ² ΠΈ ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠΎΠ² ΡΠΈΡΡΠ΅ΠΌ ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ
ΠΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΠΎΠ²Π΅Π΄Π΅Π½ΠΈΡ TiNi-ΡΠΏΠ»Π°Π²Π° Ρ TiN-ΠΏΠΎΠΊΡΡΡΠΈΡΠΌΠΈ Π΄Π»Ρ ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΎΠ³ΠΎ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ
The deformation behavior of the titanium nickelide alloy Tiβ55.84 wt. % Ni (TiNi) with titanium nitride (TiN) coatings obtained by arc-PVD has been simulated. Differential scanning calorimetry and three-point bending test were used to study the parameters of martensitic transformations and the deformation behavior of this alloy. The values of the characteristic temperatures for the TiNi alloy that can be used in medical applications were substantiated. The elastic-force characteristics of the alloy related to the properties in the superelastic state were considered. The dependiences of the change in the phase yield strength, the stress of the unloading plateau, and the residual deformation of the TiNi samples with TiN coatings on the ambient temperature range between 6 to 37 Β°C were determined. Based on these dependencies, a deformation curve was obtained that can predict the mechanical behavior of a TiNi product, for example, a stent, before and during its implantation into a human body. TiNi-based shape memory alloys are widely used in various branches of medicine; therefore, the development of technological methods for manufacturing products from TiNi with high corrosion resistance is promising.ΠΡΠΏΠΎΠ»Π½Π΅Π½ΠΎ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΠΎΠ²Π΅Π΄Π΅Π½ΠΈΡ ΡΠΏΠ»Π°Π²Π° Π½ΠΈΠΊΠ΅Π»ΠΈΠ΄Π° ΡΠΈΡΠ°Π½Π° Tiβ55,84 ΠΌΠ°Ρ.% Ni (TiNi) Ρ ΠΏΠΎΠΊΡΡΡΠΈΡΠΌΠΈ ΠΈΠ· Π½ΠΈΡΡΠΈΠ΄Π° ΡΠΈΡΠ°Π½Π° (TiN), ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΠΌΠΈ Π²Π°ΠΊΡΡΠΌΠ½ΠΎ-Π΄ΡΠ³ΠΎΠ²ΡΠΌ ΠΎΡΠ°ΠΆΠ΄Π΅Π½ΠΈΠ΅ΠΌ. Π‘ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ² Π΄ΠΈΡΡΠ΅ΡΠ΅Π½ΡΠΈΠ°Π»ΡΠ½ΠΎΠΉ ΡΠΊΠ°Π½ΠΈΡΡΡΡΠ΅ΠΉ ΠΊΠ°Π»ΠΎΡΠΈΠΌΠ΅ΡΡΠΈΠΈ ΠΈ ΡΡΠ΅Ρ
ΡΠΎΡΠ΅ΡΠ½ΠΎΠ³ΠΎ ΠΈΠ·Π³ΠΈΠ±Π° ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΡ ΠΌΠ°ΡΡΠ΅Π½ΡΠΈΡΠ½ΡΡ
ΠΏΡΠ΅Π²ΡΠ°ΡΠ΅Π½ΠΈΠΉ ΠΈ Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΎΠ½Π½ΠΎΠ΅ ΠΏΠΎΠ²Π΅Π΄Π΅Π½ΠΈΠ΅ Π΄Π°Π½Π½ΠΎΠ³ΠΎ ΡΠΏΠ»Π°Π²Π°. ΠΠ±ΠΎΡΠ½ΠΎΠ²Π°Π½Ρ Π·Π½Π°ΡΠ΅Π½ΠΈΡ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡ TiNi Π΄Π»Ρ Π΅Π³ΠΎ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Π° ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΎΠ³ΠΎ Π½Π°Π·Π½Π°ΡΠ΅Π½ΠΈΡ. Π Π°ΡΡΠΌΠΎΡΡΠ΅Π½Ρ ΡΠΏΡΡΠ³ΠΎ-ΡΠΈΠ»ΠΎΠ²ΡΠ΅ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠΈ ΡΠΏΠ»Π°Π²Π°, ΡΠ²ΡΠ·Π°Π½Π½ΡΠ΅ Ρ ΠΏΡΠΎΡΠ²Π»Π΅Π½ΠΈΠ΅ΠΌ ΡΠ²ΠΎΠΉΡΡΠ² Π² ΡΠ²Π΅ΡΡ
ΡΠ»Π°ΡΡΠΈΡΠ½ΠΎΠΌ ΡΠΎΡΡΠΎΡΠ½ΠΈΠΈ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½Ρ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠ°Π·ΠΎΠ²ΠΎΠ³ΠΎ ΠΏΡΠ΅Π΄Π΅Π»Π° ΡΠ΅ΠΊΡΡΠ΅ΡΡΠΈ, Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΡ ΡΠ°Π·Π³ΡΡΠ·ΠΎΡΠ½ΠΎΠ³ΠΎ ΠΏΠ»Π°ΡΠΎ ΠΈ ΠΎΡΡΠ°ΡΠΎΡΠ½ΠΎΠΉ Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΈ ΠΎΠ±ΡΠ°Π·ΡΠΎΠ² TiNi Ρ TiN-ΠΏΠΎΠΊΡΡΡΠΈΡΠΌΠΈ ΠΎΡ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ ΠΎΠΊΡΡΠΆΠ°ΡΡΠ΅ΠΉ ΡΡΠ΅Π΄Ρ Π² Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ ΠΎΡ 6 Π΄ΠΎ 37 Β°Π‘. ΠΠ° ΠΎΡΠ½ΠΎΠ²Π΅ Π΄Π°Π½Π½ΡΡ
Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠ΅ΠΉ ΠΏΠΎΠ»ΡΡΠ΅Π½Π° Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΎΠ½Π½Π°Ρ ΠΊΡΠΈΠ²Π°Ρ, ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡΡΠ°Ρ ΠΏΡΠΎΠ³Π½ΠΎΠ·ΠΈΡΠΎΠ²Π°ΡΡ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΠΏΠΎΠ²Π΅Π΄Π΅Π½ΠΈΠ΅ ΠΈΠ·Π΄Π΅Π»ΠΈΡ ΠΈΠ· Π½ΠΈΠΊΠ΅Π»ΠΈΠ΄Π° ΡΠΈΡΠ°Π½Π°, Π½Π°ΠΏΡΠΈΠΌΠ΅Ρ, ΡΡΠ΅Π½ΡΠ° Π΄ΠΎ ΠΈ Π²ΠΎ Π²ΡΠ΅ΠΌΡ Π΅Π³ΠΎ ΠΈΠΌΠΏΠ»Π°Π½ΡΠ°ΡΠΈΠΈ Π² ΠΎΡΠ³Π°Π½ΠΈΠ·ΠΌ ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ°. Π‘ΠΏΠ»Π°Π²Ρ Ρ ΠΏΠ°ΠΌΡΡΡΡ ΡΠΎΡΠΌΡ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ TiNi ΡΠΈΡΠΎΠΊΠΎ ΠΏΡΠΈΠΌΠ΅Π½ΡΡΡΡΡ Π² ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΠΎΡΡΠ°ΡΠ»ΡΡ
ΠΌΠ΅Π΄ΠΈΡΠΈΠ½Ρ, Π² ΡΠ²ΡΠ·ΠΈ Ρ ΡΡΠΈΠΌ ΠΏΠ΅ΡΡΠΏΠ΅ΠΊΡΠΈΠ²Π½Ρ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠΈ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΡΠΈΠ΅ΠΌΠΎΠ² ΠΈΠ·Π³ΠΎΡΠΎΠ²Π»Π΅Π½ΠΈΡ ΠΈΠ·Π΄Π΅Π»ΠΈΠΉ ΠΈΠ· TiNi Ρ Π²ΡΡΠΎΠΊΠΈΠΌΠΈ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»ΡΠΌΠΈ ΠΊΠΎΡΡΠΎΠ·ΠΈΠΎΠ½Π½ΠΎΠΉ ΡΡΠΎΠΉΠΊΠΎΡΡΠΈ
Π€ΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΠ΅ ΡΠ²ΠΎΠΉΡΡΠ²Π° ΠΎΡΡΠΎΠ΄ΠΎΠ½ΡΠΈΡΠ΅ΡΠΊΠΈΡ ΡΠ²Π΅ΡΡ ΡΠ»Π°ΡΡΠΈΡΠ½ΡΡ Π΄ΡΠ³ ΠΈΠ· Π½ΠΈΠΊΠ΅Π»ΠΈΠ΄Π° ΡΠΈΡΠ°Π½Π° Ρ Π·Π°ΡΠΈΡΠ½ΡΠΌΠΈ ΠΏΠΎΠΊΡΡΡΠΈΡΠΌΠΈ Π½ΠΈΡΡΠΈΠ΄Π° ΡΠΈΡΠ°Π½Π°
Today there are many manufacturers of orthodontic archwires composed of a nickel-titanium (TiNi) alloy with different elastic-force characteristics. A limited number of orthodontic archwires is available for initial tooth alignment, since reactive stresses do not always satisfy the condition 160 β€ Οc β€ 200 MPa. The use of orthodontic archwires with polymer coatings having better aesthetics is increasing. However, they show excessive wear and color change during a long-term orthodontic treatment. The aim of this paper is to study and optimize the functional characteristics of superelastic archwires composed of Ti-50.8 Π°Π % Ni alloy with TiN coatings deposited at varying deposition times. A three-point bending test was carried out to evaluate the functional properties. The distance between the supporters was 10 mm. The archwires were subjected to bending at a temperature of 23 Β± 3 Β°C. Each test was continued until deformation of 1.5; 3; 4.5 and 6 % was reached. It has been found that titanium nitride coatings deposited on the Ti-50.8 at. % Ni surface alloy by the vacuum-plasma method act as the barrier layer to prevent the release of nickel ions into biological environment. Heat treatment (~400 Β°C) during deposition allows the required elastic-force characteristics and functional properties of the material to form. The optimal reactive stress (160-200 MPa) and the reverse martensitic transformation temperature occurred near room temperature can be obtained due to an appropriate selection of the deposition parameters. In the martensitic phase at room temperature, the archwire can be deformed. When the archwire sample is placed in oral cavity and heated to temperatures above 30 Β°C the material is in the superelastic state. Further research is needed in terms of coating stability during deformation when the material in superelastic state, as well as conducting corrosion testing, studying biocompatibility of archwire samples with titanium nitride coatings in order to successfully implement the proposed technology in dental practice. The prototypes of orthodontic TiNi archwires with protective and decorative TiN coatings will be obtained for medical application.ΠΡΡΠΎΠΊΠΈΠ΅ ΠΊΠΎΡΡΠΎΠ·ΠΈΠΎΠ½Π½Π°Ρ ΡΡΠΎΠΉΠΊΠΎΡΡΡ ΠΈ Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠ°Ρ ΡΠΎΠ²ΠΌΠ΅ΡΡΠΈΠΌΠΎΡΡΡ Π½Π°ΡΡΠ΄Ρ Ρ Π΄ΡΡΠ³ΠΈΠΌΠΈ ΡΠ½ΠΈΠΊΠ°Π»ΡΠ½ΡΠΌΠΈ ΡΠ²ΠΎΠΉΡΡΠ²Π°ΠΌΠΈ ΡΠΏΠ»Π°Π²ΠΎΠ² Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ Π½ΠΈΠΊΠ΅Π»ΠΈΠ΄Π° ΡΠΈΡΠ°Π½Π° (TiNi) ΠΎΠ±ΡΡΠ»ΠΎΠ²Π»ΠΈΠ²Π°ΡΡ ΡΠΈΡΠΎΠΊΠΈΠ΅ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΠΈ Π΄Π»Ρ ΠΈΡ
ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ Π² ΠΌΠ΅Π΄ΠΈΡΠΈΠ½Π΅. ΠΠΎΡΡΠ°ΡΠΎΡΠ½ΠΎ ΡΠΈΡΠΎΠΊΠΎ ΡΠΈΡΠ°Π½-Π½ΠΈΠΊΠ΅Π»Π΅Π²ΡΠ΅ ΡΠΏΠ»Π°Π²Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΡΡΡΡΡ Π² ΡΡΠΎΠΌΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΠΈ, Π³Π΄Π΅ ΠΈΠ· Π½ΠΈΡ
ΠΈΠ·Π³ΠΎΡΠ°Π²Π»ΠΈΠ²Π°ΡΡ ΠΈΠΌΠΏΠ»Π°Π½ΡΠ°ΡΡ (ΡΡΠΈΡΡΡ, ΡΠΊΠΎΠ±Ρ ΠΈ Π΄Ρ.), ΡΠ½Π΄ΠΎΠ΄ΠΎΠ½ΡΠΈΡΠ΅ΡΠΊΠΈΠΉ ΠΈΠ½ΡΡΡΡΠΌΠ΅Π½ΡΠ°ΡΠΈΠΉ, Π° ΡΠ°ΠΊΠΆΠ΅ ΠΎΡΡΠΎΠ΄ΠΎΠ½ΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΡΡΡΠΎΠΉΡΡΠ²Π° - ΡΠ²Π΅ΡΡ
ΡΠ»Π°ΡΡΠΈΡΠ½ΡΠ΅ Π΄ΡΠ³ΠΈ Π΄Π»Ρ ΠΊΠΎΡΡΠ΅ΠΊΡΠΈΠΈ Π·ΡΠ±Π½ΠΎΠ³ΠΎ ΡΡΠ΄Π°. ΠΠ½ΠΎΠ³ΠΎΠΎΠ±ΡΠ°Π·ΠΈΠ΅ ΠΎΡΡΠΎΠ΄ΠΎΠ½ΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π΄ΡΠ³ ΠΈΠ· TiNi ΡΠΏΠ»Π°Π²ΠΎΠ² Π²ΠΊΠ»ΡΡΠ°Π΅Ρ Π±ΠΎΠ»ΡΡΠΎΠ΅ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²ΠΎ ΠΈΠΌΠΏΠΎΡΡΠ½ΡΡ
ΡΠΎΡΠ³ΠΎΠ²ΡΡ
ΠΌΠ°ΡΠΎΠΊ Ρ ΡΠΈΡΠΎΠΊΠΈΠΌ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½ΠΎΠΌ ΡΠΏΡΡΠ³ΠΎ-ΡΠΈΠ»ΠΎΠ²ΡΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ. ΠΠ΄Π½Π°ΠΊΠΎ Π΄Π°Π»Π΅ΠΊΠΎ Π½Π΅ Π²ΡΠ΅ ΠΈΠ· Π½ΠΈΡ
ΠΌΠΎΠ³ΡΡ Π±ΡΡΡ ΡΠ΅ΠΊΠΎΠΌΠ΅Π½Π΄ΠΎΠ²Π°Π½Ρ Π½Π° Π½Π°ΡΠ°Π»ΡΠ½ΡΡ
ΡΡΠ°ΠΏΠ°Ρ
ΠΊΠΎΡΡΠ΅ΠΊΡΠΈΠΈ ΠΈΠ·-Π·Π° ΡΠ»ΠΈΡΠΊΠΎΠΌ Π²ΡΡΠΎΠΊΠΈΡ
, ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»ΡΠ½ΠΎ ΡΡΠ°Π²ΠΌΠΎΠΎΠΏΠ°ΡΠ½ΡΡ
, ΡΠ°Π·Π²ΠΈΠ²Π°Π΅ΠΌΡΡ
ΡΡΠΈΠ»ΠΈΠΉ. ΠΡΠ΅ Π±ΠΎΠ»ΡΡΠ΅Π΅ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ Π½Π°Ρ
ΠΎΠ΄ΡΡ ΠΎΡΡΠΎΠ΄ΠΎΠ½ΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π΄ΡΠ³ΠΈ Ρ ΠΏΠΎΠ»ΠΈΠΌΠ΅ΡΠ½ΡΠΌΠΈ ΠΏΠΎΠΊΡΡΡΠΈΡΠΌΠΈ, ΠΈΠΌΠ΅ΡΡΠΈΠΌΠΈ ΡΡΡΠ΅ΡΠΈΡΠ΅ΡΠΊΠΈΠΉ Π²Π½Π΅ΡΠ½ΠΈΠΉ Π²ΠΈΠ΄, ΠΎΠ΄Π½Π°ΠΊΠΎ Π΄Π»Ρ Π½ΠΈΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠ½Ρ ΠΏΠΎΠ²ΡΡΠ΅Π½Π½ΡΠΉ ΠΈΠ·Π½ΠΎΡ ΠΈ ΠΏΠΎΡΠ΅ΠΌΠ½Π΅Π½ΠΈΠ΅ ΡΠ²Π΅ΡΠ° ΠΏΡΠΈ Π΄Π»ΠΈΡΠ΅Π»ΡΠ½ΠΎΠΉ ΡΠΊΡΠΏΠ»ΡΠ°ΡΠ°ΡΠΈΠΈ. ΠΠ²ΡΠΎΡΠ°ΠΌΠΈ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠ°Π½ ΡΠΏΠΎΡΠΎΠ± Π·Π°Π΄Π°Π½ΠΈΡ ΡΠΎΡΠΌΡ Π΄Π»Ρ ΠΎΡΡΠΎΠ΄ΠΎΠ½ΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π΄ΡΠ³ ΠΈΠ· TiNi ΡΠΏΠ»Π°Π²Π° Ρ ΠΎΠ΄Π½ΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΡΠΌ Π½Π°Π½Π΅ΡΠ΅Π½ΠΈΠ΅ΠΌ Π±ΠΈΠΎΠΈΠ½Π΅ΡΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠΊΡΡΡΠΈΡ Π½ΠΈΡΡΠΈΠ΄Π° ΡΠΈΡΠ°Π½Π°. Π ΡΠ°Π±ΠΎΡΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π»ΠΈΡΡ ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΠ΅ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠΈ ΡΠ²Π΅ΡΡ
ΡΠ»Π°ΡΡΠΈΡΠ½ΡΡ
Π΄ΡΠ³ ΠΈΠ· ΡΠΏΠ»Π°Π²Π° Ti-50,8 Π°Ρ. % Ni Ρ ΠΎΡΠ°ΠΆΠ΄Π΅Π½Π½ΡΠΌΠΈ Π²Π°ΠΊΡΡΠΌΠ½ΠΎ-ΠΏΠ»Π°Π·ΠΌΠ΅Π½Π½ΡΠΌ ΡΠΏΠΎΡΠΎΠ±ΠΎΠΌ Π² ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ ΡΠ°Π·Π»ΠΈΡΠ½ΠΎΠ³ΠΎ Π²ΡΠ΅ΠΌΠ΅Π½ΠΈ TiN ΠΏΠΎΠΊΡΡΡΠΈΡΠΌΠΈ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ ΡΠ°ΠΊΠΈΠ΅ ΠΏΠΎΠΊΡΡΡΠΈΡ Π²ΡΡΡΡΠΏΠ°ΡΡ Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ Π±Π°ΡΡΠ΅ΡΠ½ΠΎΠ³ΠΎ ΡΠ»ΠΎΡ Π½Π° ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ ΠΈΠ·Π΄Π΅Π»ΠΈΠΉ Π΄Π»Ρ ΠΏΡΠ΅Π΄ΠΎΡΠ²ΡΠ°ΡΠ΅Π½ΠΈΡ Π²ΡΡ
ΠΎΠ΄Π° Π½ΠΈΠΊΠ΅Π»Ρ Π² ΠΎΠΊΡΡΠΆΠ°ΡΡΡΡ ΡΡΠ΅Π΄Ρ, Π° ΡΠ΅ΡΠΌΠΈΡΠ΅ΡΠΊΠΎΠ΅ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ (~400 Β°Π‘) ΠΏΡΠΈ ΠΎΡΠ°ΠΆΠ΄Π΅Π½ΠΈΠΈ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ ΡΡΠΎΡΠΌΠΈΡΠΎΠ²Π°ΡΡ ΡΡΠ΅Π±ΡΠ΅ΠΌΡΠΉ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡ ΡΠΏΡΡΠ³ΠΎ-ΡΠΈΠ»ΠΎΠ²ΡΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ ΠΈ ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ
ΡΠ²ΠΎΠΉΡΡΠ² Π² ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Π΅ ΠΈΠ·Π΄Π΅Π»ΠΈΡ. Π ΡΠ°ΡΡΠ½ΠΎΡΡΠΈ, Π·Π° ΡΡΠ΅Ρ ΠΏΠΎΠ΄Π±ΠΎΡΠ° Π²ΡΠ΅ΠΌΠ΅Π½ΠΈ ΠΎΡΠ°ΠΆΠ΄Π΅Π½ΠΈΡ ΠΌΠΎΠΆΠ½ΠΎ Π΄ΠΎΡΡΠΈΡΡ ΠΎΠΏΡΠΈΠΌΠ°Π»ΡΠ½ΡΡ
Π·Π½Π°ΡΠ΅Π½ΠΈΠΉ ΡΠ΅Π°ΠΊΡΠΈΠ²Π½ΡΡ
Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΠΉ (160-200 ΠΠΠ°) ΠΈ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ ΠΎΠΊΠΎΠ½ΡΠ°Π½ΠΈΡ ΠΎΠ±ΡΠ°ΡΠ½ΠΎΠ³ΠΎ ΠΌΠ°ΡΡΠ΅Π½ΡΠΈΡΠ½ΠΎΠ³ΠΎ ΠΏΡΠ΅Π²ΡΠ°ΡΠ΅Π½ΠΈΡ, ΡΠ΅Π°Π»ΠΈΠ·ΡΠ΅ΠΌΠΎΠ³ΠΎ Π²Π±Π»ΠΈΠ·ΠΈ ΠΊΠΎΠΌΠ½Π°ΡΠ½ΠΎΠΉ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ
ΠΠ°Π΄Π°Π½ΠΈΠ΅ ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ ΡΠ²ΠΎΠΉΡΡΠ² TiNi ΡΠΏΠ»Π°Π²Π°ΠΌ Π² ΠΏΡΠΎΡΠ΅ΡΡΠ΅ ΠΈΠΎΠ½Π½ΠΎ-ΠΏΠ»Π°Π·ΠΌΠ΅Π½Π½ΠΎΠ³ΠΎ ΠΎΡΠ°ΠΆΠ΄Π΅Π½ΠΈΡ ΠΏΠΎΠΊΡΡΡΠΈΠΉ
The aim of the present work is to study the influence of the technological parameters of the ion-plasma treatment (IPT) on the functional properties of a TiNi shape memory alloy and its biocompatibility. The object of the study was the Tiβ50.8 at. % Ni alloy, widely applied in medical devices. IPT was carried out by vacuum-arc evaporation of a titanium cathode at different values of the bias potential (0, β100, and β500 V), followed by TiN deposition. The functional properties of the TiNi alloy after IPT were investigated using differential scanning calorimetry. The biocompatible properties were evaluated using atomic emission spectrometry to measure a nickel concentration after one year holding TiN-coated TiNi samples in the 0.9 % NaCl solution. It has been determined that by setting the temperature regime of heating of Tiβ50.8 at. % Ni alloy samples due to the technological parameters of the IPT process, it is possible to change the interval of realization of thermoelastic martensitic transformations, and, consequently, the temperature response of devices made of this alloy, i. e. to set the necessary functional properties. The comparative analysis of the characteristic temperatures after heat and ion-plasma treatments allow us to conclude that the proposed method for calculation of the TiNi substrate temperature is correct at IPT. The calculated temperature of the TiNi samples was ~275 Β°C at the zero potential, which is sufficient to shift the characteristic temperatures of the alloy. The substrate temperature during deposition was ~400 Β°C at a β 100 V bias and above 600 Β°C at a β 500 V bias, respectively. The Ni concentration in the model solution did not exceed 0.14 mg/l after one year holding, which indicates the high biocompatibility of the TiN-coated TiNi samples.Π Π°Π±ΠΎΡΠ° ΠΏΠΎΡΠ²ΡΡΠ΅Π½Π° ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ Π²Π»ΠΈΡΠ½ΠΈΡ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΠΏΡΠΎΡΠ΅ΡΡΠ° ΠΈΠΎΠ½Π½ΠΎ-ΠΏΠ»Π°Π·ΠΌΠ΅Π½Π½ΠΎΠΉ ΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠΈ (ΠΠΠ) Π½Π° ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΠ΅ ΡΠ²ΠΎΠΉΡΡΠ²Π° TiNi ΡΠΏΠ»Π°Π²Π° Ρ ΡΡΡΠ΅ΠΊΡΠΎΠΌ ΠΏΠ°ΠΌΡΡΠΈ ΡΠΎΡΠΌΡ ΠΈ Π΅Π³ΠΎ Π±ΠΈΠΎΡΠΎΠ²ΠΌΠ΅ΡΡΠΈΠΌΠΎΡΡΡ. Π ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΠΎΠ±ΡΠ΅ΠΊΡΠ° ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ Π²ΡΠ±ΡΠ°Π½ ΡΠΏΠ»Π°Π² Tiβ50,8 Π°Ρ. % Ni, ΡΠΈΡΠΎΠΊΠΎ ΠΏΡΠΈΠΌΠ΅Π½ΡΠ΅ΠΌΡΠΉ Π² ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΈΡ
ΠΈΠ·Π΄Π΅Π»ΠΈΡΡ
ΠΈ ΡΡΡΡΠΎΠΉΡΡΠ²Π°Ρ
. ΠΠΎΠ½Π½ΠΎ-ΠΏΠ»Π°Π·ΠΌΠ΅Π½Π½ΡΡ ΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΡ ΠΎΡΡΡΠ΅ΡΡΠ²Π»ΡΠ»ΠΈ ΠΏΡΡΠ΅ΠΌ Π²Π°ΠΊΡΡΠΌΠ½ΠΎ-Π΄ΡΠ³ΠΎΠ²ΠΎΠ³ΠΎ ΠΈΡΠΏΠ°ΡΠ΅Π½ΠΈΡ ΠΊΠ°ΡΠΎΠ΄Π° ΠΈΠ· ΡΠΈΡΠ°Π½Π° ΠΏΡΠΈ Π·Π½Π°ΡΠ΅Π½ΠΈΡΡ
ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»Π° ΡΠΌΠ΅ΡΠ΅Π½ΠΈΡ 0, β100 ΠΈ β500 Π Ρ ΠΏΠΎΡΠ»Π΅Π΄ΡΡΡΠΈΠΌ ΠΎΡΠ°ΠΆΠ΄Π΅Π½ΠΈΠ΅ΠΌ Π·Π°ΡΠΈΡΠ½ΠΎ-Π΄Π΅ΠΊΠΎΡΠ°ΡΠΈΠ²Π½ΠΎΠ³ΠΎ TiN ΠΏΠΎΠΊΡΡΡΠΈΡ. ΠΠΎΠ½ΡΡΠΎΠ»ΡΠ½ΡΡ Π³ΡΡΠΏΠΏΡ ΠΎΠ±ΡΠ°Π·ΡΠΎΠ² ΠΏΠΎΠ΄Π²Π΅ΡΠ³Π°Π»ΠΈ ΡΠ΅ΡΠΌΠΎΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠ΅ ΠΏΡΠΈ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ°Ρ
200β700 Β°Π‘ Π² ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ 20 ΠΌΠΈΠ½. Π€ΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΠ΅ ΡΠ²ΠΎΠΉΡΡΠ²Π° TiNi ΡΠΏΠ»Π°Π²Π° ΠΏΠΎΡΠ»Π΅ ΠΠΠ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π»ΠΈ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ Π΄ΠΈΡΡΠ΅ΡΠ΅Π½ΡΠΈΠ°Π»ΡΠ½ΠΎΠΉ ΡΠΊΠ°Π½ΠΈΡΡΡΡΠ΅ΠΉ ΠΊΠ°Π»ΠΎΡΠΈΠΌΠ΅ΡΡΠΈΠΈ. ΠΠΈΠΎΡΠΎΠ²ΠΌΠ΅ΡΡΠΈΠΌΡΠ΅ ΡΠ²ΠΎΠΉΡΡΠ²Π° ΠΎΡΠ΅Π½ΠΈΠ²Π°Π»ΠΈ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ Π°ΡΠΎΠΌΠ½ΠΎ-ΡΠΌΠΈΡΡΠΈΠΎΠ½Π½ΠΎΠΉ ΡΠΏΠ΅ΠΊΡΡΠΎΠΌΠ΅ΡΡΠΈΠΈ, ΠΈΠ·ΠΌΠ΅ΡΡΡ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²ΠΎ Π½ΠΈΠΊΠ΅Π»Ρ Π² 0,9 %-Π½ΠΎΠΌ ΡΠ°ΡΡΠ²ΠΎΡΠ΅ NaCl ΠΏΠΎΡΠ»Π΅ Π²ΡΠ΄Π΅ΡΠΆΠΊΠΈ Π² Π½Π΅ΠΌ TiNi ΠΎΠ±ΡΠ°Π·ΡΠΎΠ² Ρ TiN ΠΏΠΎΠΊΡΡΡΠΈΠ΅ΠΌ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ Π·Π°Π΄Π°Π²Π°Ρ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ½ΡΠΉ ΡΠ΅ΠΆΠΈΠΌ Π½Π°Π³ΡΠ΅Π²Π° ΠΎΠ±ΡΠ°Π·ΡΠΎΠ² ΠΈΠ· ΡΠΏΠ»Π°Π²Π° Tiβ50,8 Π°Ρ. % Ni Π·Π° ΡΡΠ΅Ρ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΠΏΡΠΎΡΠ΅ΡΡΠ° ΠΠΠ, ΠΌΠΎΠΆΠ½ΠΎ ΠΌΠ΅Π½ΡΡΡ ΠΈΠ½ΡΠ΅ΡΠ²Π°Π» ΡΠ΅Π°Π»ΠΈΠ·Π°ΡΠΈΠΈ ΡΠ΅ΡΠΌΠΎΡΠΏΡΡΠ³ΠΈΡ
ΠΌΠ°ΡΡΠ΅Π½ΡΠΈΡΠ½ΡΡ
ΠΏΡΠ΅Π²ΡΠ°ΡΠ΅Π½ΠΈΠΉ, Π° ΡΠ»Π΅Π΄ΠΎΠ²Π°ΡΠ΅Π»ΡΠ½ΠΎ, ΠΈ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ ΡΡΠ°Π±Π°ΡΡΠ²Π°Π½ΠΈΡ ΡΡΡΡΠΎΠΉΡΡΠ², ΠΈΠ·Π³ΠΎΡΠ°Π²Π»ΠΈΠ²Π°Π΅ΠΌΡΡ
ΠΈΠ· ΡΡΠΎΠ³ΠΎ ΡΠΏΠ»Π°Π²Π°, Ρ. Π΅. Π·Π°Π΄Π°Π²Π°ΡΡ ΠΈΠΌ Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΡΠ΅ ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΠ΅ ΡΠ²ΠΎΠΉΡΡΠ²Π°. Π‘ΠΎΠΏΠΎΡΡΠ°Π²ΠΈΡΠ΅Π»ΡΠ½ΡΠΉ Π°Π½Π°Π»ΠΈΠ· Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡ ΠΏΠΎΡΠ»Π΅ ΡΠ΅ΡΠΌΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΈ ΠΈΠΎΠ½Π½ΠΎ-ΠΏΠ»Π°Π·ΠΌΠ΅Π½Π½ΠΎΠΉ ΠΎΠ±ΡΠ°Π±ΠΎΡΠΎΠΊ ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ» ΡΠ΄Π΅Π»Π°ΡΡ Π²ΡΠ²ΠΎΠ΄ ΠΎ ΠΊΠΎΡΡΠ΅ΠΊΡΠ½ΠΎΡΡΠΈ ΠΏΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½Π½ΠΎΠ³ΠΎ ΠΌΠ΅ΡΠΎΠ΄Π° ΡΠ°ΡΡΠ΅ΡΠ° ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ TiNi ΠΏΠΎΠ΄Π»ΠΎΠΆΠΊΠΈ ΠΏΡΠΈ ΠΠΠ. Π Π°ΡΡΠ΅ΡΠ½Π°Ρ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ° ΠΎΠ±ΡΠ°Π·ΡΠΎΠ² TiNi ΠΏΡΠΈ Π½ΡΠ»Π΅Π²ΠΎΠΌ ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»Π΅ ΡΠΎΡΡΠ°Π²ΠΈΠ»Π° ~275 Β°Π‘, ΡΡΠΎ Π΄ΠΎΡΡΠ°ΡΠΎΡΠ½ΠΎ Π΄Π»Ρ ΡΠΌΠ΅ΡΠ΅Π½ΠΈΡ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡ ΡΠΏΠ»Π°Π²Π°. ΠΡΠ°ΠΆΠ΄Π΅Π½ΠΈΠ΅ ΠΏΡΠΈ ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»Π΅ β100 Π ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠΈΠ»ΠΎ Π½Π°Π³ΡΠ΅Π² ΠΏΠΎΠ΄Π»ΠΎΠΆΠΊΠΈ Π΄ΠΎ ~400 Β°Π‘, ΠΏΡΠΈ β500 Π β ΡΠ²ΡΡΠ΅ 600 Β°Π‘. ΠΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΡ Ni Π² ΠΌΠΎΠ΄Π΅Π»ΡΠ½ΠΎΠΌ ΡΠ°ΡΡΠ²ΠΎΡΠ΅ ΠΏΠΎΡΠ»Π΅ Π³ΠΎΠ΄ΠΎΠ²ΠΎΠΉ Π²ΡΠ΄Π΅ΡΠΆΠΊΠΈ Π½Π΅ ΠΏΡΠ΅Π²ΡΡΠ°Π»Π° 0,14 ΠΌΠ³/Π», ΡΡΠΎ ΡΠ²ΠΈΠ΄Π΅ΡΠ΅Π»ΡΡΡΠ²ΡΠ΅Ρ ΠΎ Π²ΡΡΠΎΠΊΠΎΠΉ Π±ΠΈΠΎΡΠΎΠ²ΠΌΠ΅ΡΡΠΈΠΌΠΎΡΡΠΈ TiNi ΡΠΏΠ»Π°Π²Π° Ρ TiN ΠΏΠΎΠΊΡΡΡΠΈΠ΅ΠΌ
Functional properties of bimetal composite of βstainless steelβTiNi alloyβ produced by explosion welding
AbstractThe functional properties of βTiNiβstainless steelβ bimetal composite produced by explosion welding were studied. The influence of the ratio of the TiNi layer thickness to the total thickness of the sample as well as the influence of preliminary deformation on the recoverable strain and a temperature of shape memory effect were studied. It was found that the best combination of strain variation observed in repeated thermal cycles was demonstrated by the bimetal sample in which the thickness of the TiNi layer was 64% of the thickness of the sample. The preliminary deformation resulted in an increase in stress stored in the sample and led to an increase in recoverable strain