146 research outputs found
ΠΠ½ΠΎΠΌΠ°Π»ΡΠ½ΡΠΉ ΡΠΎΡΡ Π·Π΅ΡΠ΅Π½ Π² ΠΊΡΠΈΠΎΠ³Π΅Π½Π½ΠΎ-Π΄Π΅ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ ΠΌΠ΅Π΄ΠΈ
Structural changes in cryogenically deformed copper during long-term (up to two years) room-temperature ageing were investigated. It is found that the structure formed under high (e=8.2) cryogenic deformation is unstable and is characterized by abnormalous grain growth. It is shown that the grain growth is preceded by a long (up to a year) incubation period. It is revealed that the structure rapidly losses stability with an increase in accumulated cryogenic strain
Nanostructure and properties of a Cu-Cr composite processed by severe plastic deformation
A Cu-Cr composite was processed by severe plastic deformation to investigate
the role of interphase boundaries on the grain size reduction mechanisms. The
as-deformed material exhibits a grain size of only 20nm. This gives rise to a
dramatic increase of the hardness. Some deformation induced Cu super saturated
solid solutions were clearly exhibited and it is shown that they decrease the
hardness. The formation of such supersaturated solid solution and their
influence on the mechanical properties are discussed
ΠΠ»ΠΈΡΠ½ΠΈΠ΅ ΠΊΡΠΈΠΎΠ³Π΅Π½Π½ΠΎΠΉ ΠΏΡΠΎΠΊΠ°ΡΠΊΠΈ Π½Π° ΠΌΠΈΠΊΡΠΎΡΡΡΡΠΊΡΡΡΡ ΠΈ ΠΌΠ΅Ρ Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΠ²ΠΎΠΉΡΡΠ²Π° ΠΌΠ΅Π΄ΠΈ
The effect of cryogenic rolling on the structure and mechanical properties of copper was studied. The grain structure evolution was shown to be mainly governed by the geometrical effect of the imposed strain whereas the contribution of the mechanical twinning and grain subdivision was found to be not significant. The analysis of the developed texture demonstrated that the plastic flow arises mainly from conventional {111} slip. The cryogenic rolling was shown to increase strength and decrease ductility and both effects might be attributed to the substructure
Π€ΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΠΌΠΈΠΊΡΠΎΡΡΡΡΠΊΡΡΡΡ Π² Ρ ΠΎΠ΄Π΅ ΠΊΡΠΈΠΎΠ³Π΅Π½Π½ΠΎΠΉ ΠΏΡΠΎΠΊΠ°ΡΠΊΠΈ ΠΌΠ΅Π΄ΠΈ
ΠΡΠΎΠ²Π΅Π΄Π΅Π½Π° ΡΡΠ°ΡΠ΅Π»ΡΠ½Π°Ρ Π°ΡΡΠ΅ΡΡΠ°ΡΠΈΡ ΠΌΠΈΠΊΡΠΎΡΡΡΡΠΊΡΡΡΡ ΠΈ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ²ΠΎΠΉΡΡΠ² ΠΌΠ΅Π΄ΠΈ, ΠΏΠΎΠ΄Π²Π΅ΡΠ³Π½ΡΡΠΎΠΉ ΡΠ°Π·Π»ΠΈΡΠ½ΠΎΠΉ ΡΡΠ΅ΠΏΠ΅Π½ΠΈ ΠΊΡΠΈΠΎΠ³Π΅Π½Π½ΠΎΠΉ ΠΏΡΠΎΠΊΠ°ΡΠΊΠΈ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΡΠ²ΠΎΠ»ΡΡΠΈΡ Π·Π΅ΡΠ΅Π½Π½ΠΎΠΉ ΡΡΡΡΠΊΡΡΡΡ, Π² ΠΎΡΠ½ΠΎΠ²Π½ΠΎΠΌ, ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ»Π°ΡΡ Π³Π΅ΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΈΠΌ ΡΡΡΠ΅ΠΊΡΠΎΠΌ Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΈ. ΠΠ° ΠΎΡΠ½ΠΎΠ²Π΅ Π°Π½Π°Π»ΠΈΠ·Π° ΡΠ΅ΠΊΡΡΡΡΠ½ΡΡ
Π΄Π°Π½Π½ΡΡ
Π±ΡΠ» ΡΠ΄Π΅Π»Π°Π½ Π²ΡΠ²ΠΎΠ΄, ΡΡΠΎ ΠΊΡΠΈΠΎΠ³Π΅Π½Π½ΡΠ΅ ΡΡΠ»ΠΎΠ²ΠΈΡ Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΈ Π½Π΅ ΠΏΡΠΈΠ²Π΅Π»ΠΈ ΠΊ ΡΡΠ½Π΄Π°ΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΠΎΠΌΡ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠ° ΠΏΠ»Π°ΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠ΅ΡΠ΅Π½ΠΈΡ, ΠΈ ΠΎΡΠ½ΠΎΠ²Π½ΡΠΌ ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠΎΠΌ Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΈ Π±ΡΠ»ΠΎ Π΄ΠΈΡΠ»ΠΎΠΊΠ°ΡΠΈΠΎΠ½Π½ΠΎΠ΅ {111} ΡΠΊΠΎΠ»ΡΠΆΠ΅Π½ΠΈΠ΅. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ ΠΊΡΠΈΠΎΠ³Π΅Π½Π½Π°Ρ ΠΏΡΠΎΠΊΠ°ΡΠΊΠ° ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡ ΠΊ ΡΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎΠΌΡ ΡΠ²Π΅Π»ΠΈΡΠ΅Π½ΠΈΡ ΠΏΡΠΎΡΠ½ΠΎΡΡΠΈ ΠΈ Π½Π΅ΠΊΠΎΡΠΎΡΠΎΠΌΡ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΡ ΠΏΠ»Π°ΡΡΠΈΡΠ½ΠΎΡΡΠΈ
ΠΠ»ΠΈΡΠ½ΠΈΠ΅ ΠΊΡΠΈΠΎΠ³Π΅Π½Π½ΠΎΠΉ ΠΎΡΠ°Π΄ΠΊΠΈ Π½Π° ΠΌΠΈΠΊΡΠΎΡΡΡΡΠΊΡΡΡΡ ΠΊΠ°ΡΠ°Π½ΠΎΠΉ ΠΌΠ΅Π»ΠΊΠΎΠ·Π΅ΡΠ½ΠΈΡΡΠΎΠΉ ΠΌΠ΅Π΄ΠΈ
ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Π° Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΡ ΡΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎΠ³ΠΎ ΠΈΠ·ΠΌΠ΅Π»ΡΡΠ΅Π½ΠΈΡ Π·Π΅ΡΠ΅Π½ Π² ΡΠ΅Ρ
Π½ΠΈΡΠ΅ΡΠΊΠΈ ΡΠΈΡΡΠΎΠΉ ΠΌΠ΅Π΄ΠΈ ΠΏΡΡΠ΅ΠΌ ΠΊΡΠΈΠΎΠ³Π΅Π½Π½ΠΎΠΉ ΠΎΡΠ°Π΄ΠΊΠΈ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ ΡΠ²ΠΎΠ»ΡΡΠΈΡ ΡΡΡΡΠΊΡΡΡΡ Π² ΡΠ΅Π»ΠΎΠΌ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ»Π°ΡΡ ΡΠΏΠ»ΡΡΠΈΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΈΡΡ
ΠΎΠ΄Π½ΡΡ
Π·Π΅ΡΠ΅Π½ Π² Ρ
ΠΎΠ΄Π΅ Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΈ. ΠΠ½Π°Π»ΠΈΠ· ΡΠ΅ΠΊΡΡΡΡΠ½ΡΡ
Π΄Π°Π½Π½ΡΡ
ΠΈ ΡΠΏΠ΅ΠΊΡΡΠ° ΡΠ°Π·ΠΎΡΠΈΠ΅Π½ΡΠΈΡΠΎΠ²ΠΎΠΊ ΠΏΠΎΠΊΠ°Π·Π°Π», ΡΡΠΎ ΠΎΡΠ½ΠΎΠ²Π½ΡΠΌ ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠΎΠΌ ΠΏΠ»Π°ΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠ΅ΡΠ΅Π½ΠΈΡ ΡΠ²Π»ΡΠ»ΠΎΡΡ ΠΎΠ±ΡΡΠ½ΠΎΠ΅ {111} Π΄ΠΈΡΠ»ΠΎΠΊΠ°ΡΠΈΠΎΠ½Π½ΠΎΠ΅ ΡΠΊΠΎΠ»ΡΠΆΠ΅Π½ΠΈΠ΅ ΠΏΡΠΈ Π½Π΅ΡΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎΠΌ Π²ΠΊΠ»Π°Π΄Π΅ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π΄Π²ΠΎΠΉΠ½ΠΈΠΊΠΎΠ²Π°Π½ΠΈΡ
ΠΡΠΈΠΎΠ³Π΅Π½Π½Π°Ρ Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΡ ΠΌΠ΅Π΄ΠΈ
The effect of cryogenic deformation on the structure refinement of copper was studied
ΠΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΠΈ ΠΎΠΏΡΠΈΠΌΠΈΠ·Π°ΡΠΈΡ ΠΏΡΠΎΡΠ΅ΡΡΠ° ΠΏΠ΅ΡΠ΅ΠΌΠ΅ΡΠ΅Π½ΠΈΡ Π³ΡΡΠ·ΠΎΠ² Π² Π»ΠΎΠ³ΠΈΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡΠ°Π½- ΠΏΠΎΡΡΠ½ΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΠ΅
Network model and algorithm for the solution of optimization problem concerning cargo transportation process within multi-terminal network in accordance with several efficiency criteria of transportation system operation have been constructed and elaborated in the paper.The paper gives the algorithm that makes it possible to trace routes and cyclic routes of maximum carrying capacity of a transportation flow.ΠΠΎΡΡΡΠΎΠ΅Π½Π° ΡΠ΅ΡΠ΅Π²Π°Ρ ΠΌΠΎΠ΄Π΅Π»Ρ ΠΈ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠ°Π½ Π°Π»Π³ΠΎΡΠΈΡΠΌ ΡΠ΅ΡΠ΅Π½ΠΈΡ Π·Π°Π΄Π°ΡΠΈ ΠΎΠΏΡΠΈΠΌΠΈΠ·Π°ΡΠΈΠΈ ΠΏΡΠΎΡΠ΅ΡΡΠ° ΠΏΠ΅ΡΠ΅ΠΌΠ΅ΡΠ΅Π½ΠΈΡ Π³ΡΡΠ·ΠΎΠ² Π² ΠΌΠ½ΠΎΠ³ΠΎΠΏΠΎΠ»ΡΡΠ½ΠΎΠΉ ΡΡΠ°ΠΉΡΠΏΠΎΡΡΠ½ΠΎΠΉ ΡΠ΅ΡΠΈ ΠΏΠΎ Π½Π΅ΡΠΊΠΎΠ»ΡΠΊΠΈΠΌ ΠΊΡΠΈΡΠ΅ΡΠΈΡΠΌ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΡΡΠ½ΠΊΡΠΈΠΎΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΡΡΠ°Π½ΡΠΏΠΎΡΡΠ½ΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ.ΠΡΠΈΠ²Π΅Π΄Π΅Π½ Π°Π»Π³ΠΎΡΠΈΡΠΌ ΠΎΡΡΡΠΊΠ°Π½ΠΈΡ ΠΌΠ°ΡΡΡΡΡΠΎΠ² ΠΈ ΡΠΈΠΊΠ»ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΌΠ°ΡΡΡΡΡΠΎΠ² ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡΠ½ΠΎΠΉ ΠΏΡΠΎΠΏΡΡΠΊΠ½ΠΎΠΉ ΡΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡΠΈ ΡΡΠ°Π½ΡΠΏΠΎΡΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΡΠΎΠΊΠ°
Optimization of the magnetic properties of FePd alloys by severe plastic deformation
A FePd alloy was nanostructured by severe plastic deformation following two
different routes: ordered and disordered states were processed by high pressure
torsion (HPT). A grain size in a range of 50 to 150 nm is obtained in both
cases. Severe plastic deformation induces some significant disordering of the
long range ordered L10 phase. However, Transmission Electron Microscopy (TEM)
data clearly show that few ordered nanocrystals remain in the deformed state.
The deformed materials were annealed to achieve nanostructured long range
ordered alloys. The transformation proceeds via a first order transition
characterized by the nucleation of numerous ordered domains along grain
boundaries. The influence of the annealing conditions (temperature and time) on
the coercivity was studied for both routes. It is demonstrated that starting
with the disorder state prior to HPT and annealing at low temperature
(400\degree C) leads to the highest coercivity (about 1.8 kOe)
Annealing behavior of cryogenically-rolled Cu-30Zn brass
The static-annealing behavior of cryogenically-rolled Cu-30Zn brass over a wide range of temperature (100-900 Β°C) was established. Between 300 and 400 Β°C, microstructure and texture evolution were dominated by discontinuous recrystallization. At temperatures of 500 Β°C and higher, annealing was interpreted in terms of normal grain growth. The recrystallized microstructure developed at 400 Β°C was ultrafine with a mean grain size of 0.8 ΞΌm, fraction of high-angle boundaries of 90 pct., and a weak crystallographic texture
ΠΠ± ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΊΡΠΈΠΎΠ³Π΅Π½Π½ΠΎΠΉ Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΈ Π΄Π»Ρ ΠΈΠ·ΠΌΠ΅Π»ΡΡΠ΅Π½ΠΈΡ ΠΌΠΈΠΊΡΠΎΡΡΡΡΠΊΡΡΡΡ ΠΌΠ΅Π΄ΠΈ
In the work, we studied and compared the microstructures of commercially pure copper subjected to the same strain at room temperature and at liquid-nitrogen temperature. It is found that at rather low plastic strain (slump, e=1.0), cryogenic temperature assists the activation of mechanical twinning and somewhat accelerates the formation of deformation boundaries. At high plastic strain (high-pressure shear, e=8.4), cryogenic temperature adds too little to microstructure refinement
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