68 research outputs found
The cyclic stability of rubber-like behaviour in stress-induced martensite aged Ni49Fe18Ga27Co6 (at.%) single crystals
In present work, the cyclic stability of the rubber-like behaviour (RLB) was investigated in Ni49Fe18Ga27Co6 (at. %) single crystals. Crystals were aged in the martensite phase at 423 K for 1 h under a compressive stress of 450 MPa, applied along the [110]B2[100]L10-direction. The RLB was induced by a preliminary chemical stabilization of the oriented L10-martensite during stress-induced martensite aging (SIM-aging) and following the reversible reorientation of martensitic variants under a compressive stress applied along the [001]B2[001]L10-direction. The high cyclic stability of the RLB was obtained in 200 loading/unloading cycles, due to the low reorientation stresses of the L10-martensite variants (no higher than 140 MPa) and the high strength properties of the L10-martensite (~1.6 GPa). The irreversible strain after 200 cycles did not exceed 0.6%. An increase in the number of cycles did not lead to the effect of destabilization of the L10-martensite
Orientation dependence of superelasticity in quenched high-nickel Ti51.8Ni single crystals
The orientation dependence of the functional and mechanical properties of quenched Ti-51.8at.%Ni single crystals, undergoing a strain-glass transition upon cooling/heating was investigated. It was found that a compressive stress above 800 MPa leads to the B2-B190 martensitic transformation (MT), regardless of orientation. In the high-strength [0 0 1]-orientation, superelasticity (SE) was observed at 203β248 K, with a reversible strain of 2.3%. Degradation of SE at deforming stresses r > 1000 MPa was associated with the formation of {1 1 3}B2 twins during the reverse MT. In the low-strength 1 1 1-orientation, the formation of stress-induced B190 -martensite occurred simultaneously with the plastic deformation of the B2-phase (due to the formation of reorientation bands and dislocation slip) and a reversible strain was not observed
Complex Study of Magnetization Reversal Mechanisms of FeNi/FeMn Bilayers Depending on Growth Conditions
Magnetization reversal processes in the NiFe/FeMn exchange biased structures with various antiferromagnetic layer thicknesses (0β50 nm) and glass substrate temperatures (17β600β¦C) during deposition were investigated in detail. Magnetic measurements were performed in the temperature range from 80 K up to 300 K. Hysteresis loop asymmetry was found at temperatures lower than 150 K for the samples with an antiferromagnetic layer thickness of more than 10 nm. The average grain size of FeMn was found to increase with the AFM layer increase, and to decrease with the substrate temperature increase. Hysteresis loop asymmetry was explained in terms of the exchange spring model in the antiferromagnetic layer. Β© 2022 by the authors. Licensee MDPI, Basel, Switzerland.Ministry of Education and Science of the Russian Federation,Β Minobrnauka: FEUZ-2020-0051;Β AgentΓΊra na Podporu VΓ½skumu a VΓ½voja,Β APVV: APVV-20-0324Funding: This work has been supported by the grant of the Slovak Research and Development Agency under the contract No APVV-20-0324. This work was in part financially supported by the Ministry of Science and Higher Education of the Russian Federation, Subject of the state task No. FEUZ-2020-0051. The electron microscopy investigations were carried out on the equipment of Krasnoyarsk Regional Center of Research Equipment of Federal Research Center Β«Krasnoyarsk Science Center SB RASΒ»
Π‘ΠΈΠ½ΡΠ΅Π·, ΠΌΠΈΠΊΡΠΎΡΡΡΡΠΊΡΡΡΠ° ΠΈ ΠΌΠ°Π³Π½ΠΈΡΠ½ΡΠ΅ ΡΠ²ΠΎΠΉΡΡΠ²Π° ΠΌΠ°Π³Π½ΠΈΡΠΎΠΌΡΠ³ΠΊΠΈΡ ΠΏΠ»Π΅Π½ΠΎΠΊ Π‘ΠΎΠ
Soft magnetic thin CoP films were obtained by means of chemical metallization from aqueous cobalt salt solution in the presence of sodium hydroxide, citric acid and sodium hypophosphite as the reducing agent. The optimal values of the magnetic film parameters (saturation magnetization and width of ferromagnetic resonance line) were obtained by variation of composition of work solutions. It allows to reduce losses in their application in microwave devices. Microphotographs of magnetic film indicate a grain structure with a grain size of about 50 nm and presence of inclusions with the size of 3-5 nm. To determine the magnetic parameters of the investigated films the method of ferromagnetic resonance (FMR) absorption curves processing is used. The values of FMR line width and an effective magnetization of film material saturation were obtained.ΠΡΠΈΠ²Π΅Π΄Π΅Π½Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΡΠ²ΠΎΠΉΡΡΠ² ΠΌΠ°Π³Π½ΠΈΡΠΎΠΌΡΠ³ΠΊΠΈΡ
ΡΠΎΠ½ΠΊΠΈΡ
ΠΏΠ»Π΅Π½ΠΎΠΊ Π‘ΠΎΠ , ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ Ρ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΌΠ΅ΡΠ°Π»Π»ΠΈΠ·Π°ΡΠΈΠΈ ΠΈΠ· Π²ΠΎΠ΄Π½ΠΎΠ³ΠΎ ΡΠ°ΡΡΠ²ΠΎΡΠ° Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΡΠΈΡΡΠ°ΡΠ½ΡΡ
ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠΎΠ² Ρ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΡΠ΅Π»ΠΎΡΠ½ΠΎΠ³ΠΎ ΡΠ΅Π°Π³Π΅Π½ΡΠ° NaOH. Π‘ ΠΏΠΎΠΌΠΎΡΡΡ Π²Π°ΡΠΈΠ°ΡΠΈΠΈ ΡΠΎΡΡΠ°Π²ΠΎΠ² ΡΠ°Π±ΠΎΡΠΈΡ
ΡΠ°ΡΡΠ²ΠΎΡΠΎΠ² ΠΏΠΎΠ»ΡΡΠ΅Π½Ρ ΠΎΠΏΡΠΈΠΌΠ°Π»ΡΠ½ΡΠ΅ Π·Π½Π°ΡΠ΅Π½ΠΈΡ ΠΌΠ°Π³Π½ΠΈΡΠ½ΡΡ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΠΏΠ»Π΅Π½ΠΎΠΊ: Π½Π°ΠΌΠ°Π³Π½ΠΈΡΠ΅Π½Π½ΠΎΡΡΠΈ Π½Π°ΡΡΡΠ΅Π½ΠΈΡ ΠΈ ΡΠΈΡΠΈΠ½Ρ Π»ΠΈΠ½ΠΈΠΈ ΡΠ΅ΡΡΠΎΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠ³ΠΎ ΡΠ΅Π·ΠΎΠ½Π°Π½ΡΠ°
The Clusters Self-Assembled Crystal and Magnetic Structure During the Martensite Transition in Fe86mn13c Alloy
In bulk and thin film state Fe86Mn13C alloy observed experimentally self-assembly of the crystal
and magnetic structures on multiscale levels. Offered self-assembly cluster model of atomic
structure based on the concept of a liquid-like state of the material in localized areas, formed in
the waves of plastic deformation
Influences of metal magnetic state and MIS structure composition on magnetoimpedance effect caused by interface states
Phase with Spinel Structure Type in Plastically Deformed Niti
ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ ΠΎΠ±ΡΠ°Π·ΡΡ ΡΠΏΠ»Π°Π²Π° Ni51Ti49, ΠΏΠΎΠ΄Π²Π΅ΡΠ³Π½ΡΡΡΠ΅ ΠΏΠ»Π°ΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΈ.
ΠΠΈΠΊΡΠΎΡΡΡΡΠΊΡΡΡΠ° ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π»Π°ΡΡ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ ΠΏΡΠΎΡΠ²Π΅ΡΠΈΠ²Π°ΡΡΠ΅ΠΉ ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠΉ ΠΌΠΈΠΊΡΠΎΡΠΊΠΎΠΏΠΈΠΈ
ΠΈ ΠΌΠΈΠΊΡΠΎΠ΄ΠΈΡΡΠ°ΠΊΡΠΈΠΈ Π½Π° ΠΌΠΈΠΊΡΠΎΡΠΊΠΎΠΏΠ΅ Hitachi 7700. ΠΠ»Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΎΠ±ΡΠ°Π·ΡΠΎΠ² ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌΠΈ
ΠΏΡΠΎΡΠ²Π΅ΡΠΈΠ²Π°ΡΡΠ΅ΠΉ ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠΉ ΠΌΠΈΠΊΡΠΎΡΠΊΠΎΠΏΠΈΠΈ (ΠΠΠ) Ρ Π·ΠΎΠ½Ρ ΡΠ°Π·ΡΡΠ²Π° ΡΠ°ΡΡΡΠ½ΡΡΡΡ
ΠΎΠ±ΡΠ°Π·ΡΠΎΠ²
Π²ΡΡΠ΅Π·Π°Π»ΠΈ Π΄ΠΈΡΠΊΠΈ Π΄ΠΈΠ°ΠΌΠ΅ΡΡΠΎΠΌ 3 ΠΌΠΌ, ΠΊΠΎΡΠΎΡΡΠ΅ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈ ΡΡΠΎΠ½ΡΠ»ΠΈ, Π·Π°ΡΠ΅ΠΌ ΡΠ»Π΅ΠΊΡΡΠΎΡ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΈΠΌ
ΡΠΏΠΎΡΠΎΠ±ΠΎΠΌ ΡΡΠ°Π²ΠΈΠ»ΠΈ Π΄ΠΎ ΠΏΠΎΡΠ²Π»Π΅Π½ΠΈΡ ΠΎΡΠ²Π΅ΡΡΡΠΈΡ Π² ΡΠ΅Π½ΡΡΠ΅ Π΄ΠΈΡΠΊΠ°. Π€ΠΈΠ½Π°Π»ΡΠ½ΡΠΌ ΡΡΠ°ΠΏΠΎΠΌ ΠΏΠΎΠ΄Π³ΠΎΡΠΎΠ²ΠΊΠΈ
ΡΠ²Π»ΡΠ»ΠΎΡΡ ΠΈΠΎΠ½Π½ΠΎΠ΅ ΡΡΠ°Π²Π»Π΅Π½ΠΈΠ΅ Π½Π° ΡΡΡΠ°Π½ΠΎΠ²ΠΊΠ΅ PIPS (Gatan). Π£ΡΠΎΠ½Π΅Π½Π½ΡΠ΅ Π΄Π»Ρ ΠΏΡΠΎΡΠ²Π΅ΡΠΈΠ²Π°ΡΡΠ΅ΠΉ
ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠΉ ΠΌΠΈΠΊΡΠΎΡΠΊΠΎΠΏΠΈΠΈ ΠΎΠ±ΡΠ°Π·ΡΡ Π±ΡΠ»ΠΈ ΠΏΠΎΠ΄Π²Π΅ΡΠ³Π½ΡΡΡ ΠΊΡΠΈΠΎΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠ΅ ΠΏΡΡΠ΅ΠΌ
ΡΠΈΠΊΠ»ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΎΡ
Π»Π°ΠΆΠ΄Π΅Π½ΠΈΡ Π² ΠΆΠΈΠ΄ΠΊΠΎΠΌ Π°Π·ΠΎΡΠ΅. Π€Π°Π·ΠΎΠ²ΡΠΉ ΡΠΎΡΡΠ°Π² ΠΎΠ±ΡΠ°Π·ΡΠΎΠ² ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ»ΠΈ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ
Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΈ ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΠ²ΡΠΊΠΈΡ
Π»ΡΡΠ΅ΠΉ Π² Π΄ΠΈΡΡΠ°ΠΊΡΠΎΠΌΠ΅ΡΡΠ΅ Β«BrukerΒ» Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ
ΠΌΠ΅Π΄ΠΈ. Π Π·ΠΎΠ½Π°Ρ
Π»ΠΎΠΊΠ°Π»ΠΈΠ·Π°ΡΠΈΠΈ Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΈ ΠΎΠ±Π½Π°ΡΡΠΆΠ΅Π½Ρ Π»ΠΈΠ½Π·ΠΎΠ²ΠΈΠ΄Π½ΡΠ΅ ΠΊΡΠΈΡΡΠ°Π»Π»Ρ ΡΠ°Π·Ρ Ni2Ti3,
ΡΠΎΠ΄Π΅ΡΠΆΠ°ΡΠΈΠ΅ ΠΈΠ·Π³ΠΈΠ±Π½ΡΠ΅ ΡΠΊΡΡΠΈΠ½ΠΊΡΠΈΠΎΠ½Π½ΡΠ΅ ΠΊΠΎΠ½ΡΡΡΡ, ΠΊΠΎΡΠΎΡΡΠ΅ ΡΠ²ΠΈΠ΄Π΅ΡΠ΅Π»ΡΡΡΠ²ΡΡΡ ΠΎ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎΠΉ
ΠΊΡΠΈΠ²ΠΈΠ·Π½Π΅ ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠ΅ΡΠ΅ΡΠΊΠΈ, ΠΏΠΎΡΠ²Π»ΡΡΡΠ΅ΠΉΡΡ Π² Π·ΠΎΠ½Π°Ρ
Π»ΠΎΠΊΠ°Π»ΠΈΠ·Π°ΡΠΈΠΈ ΠΏΠ»Π°ΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ
Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΈ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠ°Ρ ΡΡΡΡΠΊΡΡΡΠ° Π»ΠΈΠ½Π·ΠΎΠ²ΠΈΠ΄Π½ΡΡ
ΠΊΡΠΈΡΡΠ°Π»Π»ΠΎΠ²
ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»ΡΠ΅Ρ ΡΠΎΠ±ΠΎΠΉ ΡΠ°Π·Ρ, ΠΎΠ±Π»Π°Π΄Π°ΡΡΡΡ ΡΡΡΡΠΊΡΡΡΠ½ΡΠΌ ΡΠΈΠΏΠΎΠΌ ΡΠΏΠΈΠ½Π΅Π»ΠΈ Ρ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠΌ
ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠ΅ΡΠ΅ΡΠΊΠΈ 11,53Β±0,03 Γ
. ΠΠ»Ρ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π»ΠΈΠ½Π·ΠΎΠ²ΠΈΠ΄Π½ΡΡ
ΠΊΡΠΈΡΡΠ°Π»Π»ΠΎΠ²
Π½Π΅ΡΠ°Π²Π½ΠΎΠ²Π΅ΡΠ½ΠΎΠΉ ΡΠ°Π·Ρ Ni2Ti3 Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΠΎ ΠΏΠ΅ΡΠ΅ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½ΡΠΎΠ² ΠΈΡΡ
ΠΎΠ΄Π½ΠΎΠ³ΠΎ ΡΠ²Π΅ΡΠ΄ΠΎΠ³ΠΎ
ΡΠ°ΡΡΠ²ΠΎΡΠ° ΠΈΠ»ΠΈ ΠΈΠ½ΡΠ΅ΡΠΌΠ΅ΡΠ°Π»Π»ΠΈΠ΄Π½ΡΡ
ΡΠ°Π·. Π ΡΡΠ»ΠΎΠ²ΠΈΡΡ
Π»ΠΎΠΊΠ°Π»ΡΠ½ΠΎΠΉ ΠΊΡΠΈΠ²ΠΈΠ·Π½Ρ ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΎΠΉ
ΡΠ΅ΡΠ΅ΡΠΊΠΈ Π² Π·ΠΎΠ½Π°Ρ
ΡΠ²Π΅Π»ΠΈΡΠ΅Π½Π½ΡΡ
ΠΌΠ΅ΠΆΠ°ΡΠΎΠΌΠ½ΡΡ
ΡΠ°ΡΡΡΠΎΡΠ½ΠΈΠΉ Π²ΠΎΠ·Π½ΠΈΠΊΠ°ΡΡ ΠΎΡΠΎΠ±ΡΠ΅ ΡΡΡΡΠΊΡΡΡΠ½ΡΠ΅
ΡΠΎΡΡΠΎΡΠ½ΠΈΡ, ΠΊΠΎΡΠΎΡΡΠ΅ ΠΏΠΎΠ²ΡΡΠ°ΡΡ ΡΠΈΡΠ»ΠΎ ΡΡΠ΅ΠΏΠ΅Π½Π΅ΠΉ ΡΠ²ΠΎΠ±ΠΎΠ΄Ρ Π² Π΄Π΅ΡΠΎΡΠΌΠΈΡΡΠ΅ΠΌΠΎΠΌ ΡΠ²Π΅ΡΠ΄ΠΎΠΌ ΡΠ΅Π»Π΅ ΠΈ
ΡΠ°ΠΊΠΈΠΌ ΠΎΠ±ΡΠ°Π·ΠΎΠΌ ΡΠΏΠΎΡΠΎΠ±ΡΡΠ²ΡΡΡ ΠΏΠΎΡΠ²Π»Π΅Π½ΠΈΡ Π½ΠΎΠ²ΡΡ
ΡΠ°Π·The alloy samples Ni51Ti49, subjected to plastic deformation were investigated. The microstructure and
the microdiffraction were investigated by transmission electron microscopy Hitachi 7700. Discs with
a diameter of 3 mm for investigation by transmission electron microscopy (TEM) was cut from the
fracture zone of the stretched sample. They were mechanically thinned, then electrochemically etched
until the hole in the center. The final step was to prepare ion etching in install PIPS (Gatan). TEM
specimens were subjected cryomechanical processing. This was done by in liquid nitrogen cooling
cyclically. The phase composition of the samples was determined by X-ray diffraction diffractometer
"Bruker" using copper radiation. The lens-form crystals Ni2Ti3, containing bending contours, indicating
significant internal stresses in the zones of stress localization were detected. The lens-form crystals
can be represented as a non-equilibrium phase Ni2Ti3 with spinel structure type with lattice parameter
11,53 Β± 0,03 Γ
. For the formation of lenticular crystals of nonequilibrium phase Ni2Ti3 it is necessary
redistribution of the original solid solution components. In local curvature of the crystalline lattice
areas, the increased interatomic distances created the special structural states. These states increase
the number of degrees of freedom in a deformable solid and thus contribute to the emergence of new
phase
Tunable magnetic properties of Ni-doped CoFe2O4 nanoparticles prepared by the sol\u2013gel citrate self-combustion method
The nanostructured spinel ferrites with complex stoichiometry are an important family of the materials in a number of applications, especially in electronics through their good electrical and magnetic properties. In the framework of this study, a set of mixed cobalt and nickel ferrites was prepared with the sol\u2013gel self-combustion route. The structural and morphological features of particles were studied with X-ray diffraction (XRD), Scanning Transmission Electron Microscopy (STEM) and Energy Dispersive X-ray analysis (EDX) techniques. The prepared particles show a crystalline nature with a monotonic distribution of the elements and particles size distribution in the range of 17\u201329 nm. The obtained particles demonstrate good magnetic properties with tunable saturation magnetization and magnetic anisotropy, i.e., coercivity depending on chemical composition
ΠΠ»Π°ΡΡΠ΅ΡΠ½Π°Ρ ΡΠ°ΠΌΠΎΠΎΡΠ³Π°Π½ΠΈΠ·Π°ΡΠΈΡ ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΈ ΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠΉ ΡΡΡΡΠΊΡΡΡ Π² ΠΏΡΠΎΡΠ΅ΡΡΠ΅ ΠΌΠ°ΡΡΠ΅Π½ΡΠΈΡΠ½ΠΎΠ³ΠΎ ΠΏΡΠ΅Π²ΡΠ°ΡΠ΅Π½ΠΈΡ Π² ΡΠΏΠ»Π°Π²Π΅ Fe86Mn13C
In bulk and thin film state Fe86Mn13C alloy observed experimentally self-assembly of the crystal
and magnetic structures on multiscale levels. Offered self-assembly cluster model of atomic
structure based on the concept of a liquid-like state of the material in localized areas, formed in
the waves of plastic deformationΠ ΠΌΠ°ΡΡΠΈΠ²Π½ΡΡ
ΠΈ ΡΠΎΠ½ΠΊΠΎΠΏΠ»Π΅Π½ΠΎΡΠ½ΡΡ
ΠΎΠ±ΡΠ°Π·ΡΠ°Ρ
ΡΠΏΠ»Π°Π²Π° Fe86Mn13C ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΠΎ Π½Π°Π±Π»ΡΠ΄Π°Π΅ΡΡΡ
ΡΠ°ΠΌΠΎΠΎΡΠ³Π°Π½ΠΈΠ·Π°ΡΠΈΡ ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΈ ΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠΉ ΡΡΡΡΠΊΡΡΡ Π½Π° ΡΠ°Π·Π½ΠΎΠΌΠ°ΡΡΡΠ°Π±Π½ΡΡ
ΡΡΠΎΠ²Π½ΡΡ
.
ΠΡΠ΅Π΄Π»Π°Π³Π°Π΅ΡΡΡ ΠΊΠ»Π°ΡΡΠ΅ΡΠ½Π°Ρ ΠΌΠΎΠ΄Π΅Π»Ρ Π°ΡΠΎΠΌΠ½ΠΎΠΉ ΡΠ°ΠΌΠΎΠΎΡΠ³Π°Π½ΠΈΠ·Π°ΡΠΈΠΈ, ΠΎΡΠ½ΠΎΠ²Π°Π½Π½Π°Ρ Π½Π° ΠΊΠΎΠ½ΡΠ΅ΠΏΡΠΈΠΈ
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