10 research outputs found
On the determination of Poisson's ratio of stressed monolayer and bilayer submicron thick films
In this paper, the bulge test is used to determine the mechanical properties
of very thin dielectric membranes. Commonly, this experimental method permits
to determine the residual stress (s0) and biaxial Young's modulus (E/(1-u)).
Associating square and rectangular membranes with different length to width
ratios, the Poisson's ratio (u) can also be determined. LPCVD Si3N4 monolayer
and Si3N4/SiO2 bilayer membranes, with thicknesses down to 100 nm, have been
characterized giving results in agreement with literature for Si3N4, E = 212
14 GPa, s0 = 420 8 and u = 0.29.Comment: Submitted on behalf of EDA Publishing Association
(http://irevues.inist.fr/handle/2042/16838
Multilayer TiB2/X hard coatings by sputtering deposition
Titanium diboride has been investigated as a potential candidate for aerospace
structures, cutting tools, surface coatings of first-wall components and diffusion barriers
in integrated circuit metallization. Titanium diboride is a very stable hard refractory
compound but its brittleness is the main drawback. It was possible to lessen the TiB2
brittleness by producing TiB2/X coating designs by the multi-target RF magnetron
sputtering process. X is the metal layer (Al, Ti, NiCr, Mo) in the composite system.
The influence of the composition wavelength and volume fraction of ceramic
has been studied over a range of sputtering conditions. The most suitable multilayer
coating design (TiB2/NiCr) on steel substrate, for maximum hardness (18.81GPa) and
elastic modulus (304.6GPa) was found to be with a composition wavelength of 50nm
and volume fraction of ceramic of 75%. The greatest improvement of the elastic modulus
measured by nanoindentation was found to be for a TiB2/Al two-layer coating design
either on steel or on aluminium substrate, giving 36.2% and 40% improvement above the
rule of mixtures respectively, when compared with TiB2 coatings deposited under the
same sputtering conditions.
Several pieces of three-point bent apparatus were designed for measuring the inplane elastic modulus of the coatings. The three-point bent test by nanoindenter shows
promise as a method for measuring the in-plane elastic modulus on uncoated beams.
A comparison between traditional and non-traditional methods of measuring
mechanical properties of the coatings was performed in this study. The nanoindentation
technique was found to be an appropriate method to measure the mechanical properties
of multilayer coating designs.Ph
Diffusion of diluents in glassy polymers
Thesis (Ph. D.)--Massachusetts Institute of Technology, Dept. of Chemical Engineering, 1994.Includes bibliographical references.by Paul Franklin NEaley.Ph.D
Stress analysis, dielectric, piezoelectric, and ferroelectric properties of PZT thick films. Fabrication of a 50MHz Tm-pMUT annular array
PZT films up to 35 ΞΌm thick were fabricated, using a composite sol gel route combining a PZT
powder and a PZT sol. The maximum temperature for the process was 710Β°C. A
demonstration of single layer and multilayer structures was given to show the flexibility of this
technology. With Stoneyβs Equation, studies of the in-situ film stress development as a
function of the film thickness and density was effectuated. It helped to understand that the
internal forces increase considerably with the film thickness and density. This study yields to
set up experimental conditions in which a crack free surface finish of a 28ΞΌm thick film
revealed the adaptability of the spin coating technique to fabricate thick films.
The wet etching technology revealed the possibility of a great adaptability to pattern and
shape innovative devices such as bars 10 ΞΌm wide of 21ΞΌm PZT thick film. The results open
the way to a wide range of new industrial application requiring small features and/or multilayer
PZT thick film with embedded electrodes.
The single element and annular array devices have been shown to resonate at approximately
60MHz in air and 50 MHz in water. Three types of the composite thick film β 2C+4S, 2C+5S
and 2C+6S β were used to fabricate the Tm-pMUT devices. In each case the most effective
poling was obtained by maintaining the poling field of 8.4V/ΞΌm during cooling from the poling
temperature (200ΒΊC) to βfreezeβ poled domains in place. This βfreezingβ was required to
prevent the tensile stresses within the film from reorienting the domains at high temperatures
when the poling field is removed.
Increasing values of thickness mode coupling coefficient (kt) were observed with increasing
levels of sol infiltration (decreasing density). Such behaviour is thought to be due to non linear
effects on the piezoelectric coefficient (e33) at high levels of porosity. For very dense thick film
material a kt of 0.47 was observed which is comparable to that observed for the bulk material
Stress analysis, dielectric, piezoelectric, and ferroelectric properties of PZT thick films. Fabrication of a 50MHz Tm-pMUT annular array
PZT films up to 35 ΞΌm thick were fabricated, using a composite sol gel route combining a PZT powder and a PZT sol. The maximum temperature for the process was 710Β°C. A demonstration of single layer and multilayer structures was given to show the flexibility of this technology. With Stoneyβs Equation, studies of the in-situ film stress development as a function of the film thickness and density was effectuated. It helped to understand that the internal forces increase considerably with the film thickness and density. This study yields to set up experimental conditions in which a crack free surface finish of a 28ΞΌm thick film revealed the adaptability of the spin coating technique to fabricate thick films. The wet etching technology revealed the possibility of a great adaptability to pattern and shape innovative devices such as bars 10 ΞΌm wide of 21ΞΌm PZT thick film. The results open the way to a wide range of new industrial application requiring small features and/or multilayer PZT thick film with embedded electrodes. The single element and annular array devices have been shown to resonate at approximately 60MHz in air and 50 MHz in water. Three types of the composite thick film β 2C+4S, 2C+5S and 2C+6S β were used to fabricate the Tm-pMUT devices. In each case the most effective poling was obtained by maintaining the poling field of 8.4V/ΞΌm during cooling from the poling temperature (200ΒΊC) to βfreezeβ poled domains in place. This βfreezingβ was required to prevent the tensile stresses within the film from reorienting the domains at high temperatures when the poling field is removed. Increasing values of thickness mode coupling coefficient (kt) were observed with increasing levels of sol infiltration (decreasing density). Such behaviour is thought to be due to non linear effects on the piezoelectric coefficient (e33) at high levels of porosity. For very dense thick film material a kt of 0.47 was observed which is comparable to that observed for the bulk material.EThOS - Electronic Theses Online ServiceGBUnited Kingdo
The design of a microfabricated air electrode for liquid electrolyte fuel cells
Thesis (Ph. D.)--Massachusetts Institute of Technology, Dept. of Mechanical Engineering, 2007.Includes bibliographical references.In this dissertation, the microfabricated electrode (MFE) concept was applied to the design of an air electrode for liquid electrolyte fuel cells. The catalyst layer of the electrode is envisioned to be fabricated by using a microfabricated die to apply a three-dimensionally patterned macro-texture upon a microporous carbon matrix. The resulting dual porosity structure consists of an array of cylindrical holes that are formed from the die and micropores present in the carbon matrix. The holes are used for gas transport while the micropores are saturated with a liquid electrolyte for ion transport. The catalyst is loaded into the microfabricated structure by electrodepositing thin catalyst films within the cylindrical holes. In this dissertation, three issues concerning the design of the MFE were investigated: 1) identification of the best material to use for the microporous carbon matrix, 2) the study of electrokinetic parameters of electrodeposited Pt films, and 3) the study of oxygen transport behavior within a Pt film supported on the surface of a microporous carbon matrix. Two types of polymer-bonded carbon materials have been identified as suitable materials for the carbon matrix. They are carbon black particles bonded into a microporous matrix either by polytetrafluoroethylene (PTFE) fibrils or by polyethersulfone (PES), which is a soluble polymer in common solvents. Experiments and modeling have indicated that these materials will allow the microfabricated catalyst layer to have an effective ionic conductivity that is 4 to 5 times greater than the conventional catalyst layer. Rotating disk electrode experiments on electrodeposited Pt films in 0.5 M sulfuric acid show that these films have an oxygen reduction reaction mass activity that is 2.5 times greater than that of Pt particles supported on carbon black.(cont.) Furthermore, oxygen gain experiments on electrodeposited Pt films supported on a microporous membrane indicate that these films experienced no oxygen transport losses in air, up to a current density of 130 mA/cm2. These results strongly support the use of thin catalyst film technology in catalyst layers of fuel cells. The experimental results presented this dissertation were used to develop a half-cell model of the MFE in concentrated phosphoric acid. The results of the model suggest that the MFE is capable of producing a current density 3.5 times greater than that of the conventional electrode. It is believed that such potential improvements in the performance of the air electrode support continued efforts to fabricate and test the MFE design concept presented in this dissertation.by Pierre Fritz, Jr.Ph.D
Microgravity Science and Applications: Program Tasks and Bibliography for Fiscal Year 1996
NASA's Microgravity Science and Applications Division (MSAD) sponsors a program that expands the use of space as a laboratory for the study of important physical, chemical, and biochemical processes. The primary objective of the program is to broaden the value and capabilities of human presence in space by exploiting the unique characteristics of the space environment for research. However, since flight opportunities are rare and flight research development is expensive, a vigorous ground-based research program, from which only the best experiments evolve, is critical to the continuing strength of the program. The microgravity environment affords unique characteristics that allow the investigation of phenomena and processes that are difficult or impossible to study an Earth. The ability to control gravitational effects such as buoyancy driven convection, sedimentation, and hydrostatic pressures make it possible to isolate phenomena and make measurements that have significantly greater accuracy than can be achieved in normal gravity. Space flight gives scientists the opportunity to study the fundamental states of physical matter-solids, liquids and gasses-and the forces that affect those states. Because the orbital environment allows the treatment of gravity as a variable, research in microgravity leads to a greater fundamental understanding of the influence of gravity on the world around us. With appropriate emphasis, the results of space experiments lead to both knowledge and technological advances that have direct applications on Earth. Microgravity research also provides the practical knowledge essential to the development of future space systems. The Office of Life and Microgravity Sciences and Applications (OLMSA) is responsible for planning and executing research stimulated by the Agency's broad scientific goals. OLMSA's Microgravity Science and Applications Division (MSAD) is responsible for guiding and focusing a comprehensive program, and currently manages its research and development tasks through five major scientific areas: biotechnology, combustion science, fluid physics, fundamental physics, and materials science. FY 1996 was an important year for MSAD. NASA continued to build a solid research community for the coming space station era. During FY 1996, the NASA Microgravity Research Program continued investigations selected from the 1994 combustion science, fluid physics, and materials science NRAS. MSAD also released a NASA Research Announcement in microgravity biotechnology, with more than 130 proposals received in response. Selection of research for funding is expected in early 1997. The principal investigators chosen from these NRAs will form the core of the MSAD research program at the beginning of the space station era. The third United States Microgravity Payload (USMP-3) and the Life and Microgravity Spacelab (LMS) missions yielded a wealth of microgravity data in FY 1996. The USMP-3 mission included a fluids facility and three solidification furnaces, each designed to examine a different type of crystal growth
ΠΠ΅ΠΆΠ΄ΡΠ½Π°ΡΠΎΠ΄Π½Π°Ρ ΠΊΠΎΠ½ΡΠ΅ΡΠ΅Π½ΡΠΈΡ "Π€ΠΈΠ·ΠΈΡΠ΅ΡΠΊΠ°Ρ ΠΌΠ΅Π·ΠΎΠΌΠ΅Ρ Π°Π½ΠΈΠΊΠ°. ΠΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ Ρ ΠΌΠ½ΠΎΠ³ΠΎΡΡΠΎΠ²Π½Π΅Π²ΠΎΠΉ ΠΈΠ΅ΡΠ°ΡΡ ΠΈΡΠ΅ΡΠΊΠΈ ΠΎΡΠ³Π°Π½ΠΈΠ·ΠΎΠ²Π°Π½Π½ΠΎΠΉ ΡΡΡΡΠΊΡΡΡΠΎΠΉ ΠΈ ΠΈΠ½ΡΠ΅Π»Π»Π΅ΠΊΡΡΠ°Π»ΡΠ½ΡΠ΅ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΡΡΠ²Π΅Π½Π½ΡΠ΅ ΡΠ΅Ρ Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ", ΠΏΠΎΡΠ²ΡΡΠ΅Π½Π½Π°Ρ 90-Π»Π΅ΡΠΈΡ ΡΠΎ Π΄Π½Ρ ΡΠΎΠΆΠ΄Π΅Π½ΠΈΡ ΠΎΡΠ½ΠΎΠ²Π°ΡΠ΅Π»Ρ ΠΈ ΠΏΠ΅ΡΠ²ΠΎΠ³ΠΎ Π΄ΠΈΡΠ΅ΠΊΡΠΎΡΠ° ΠΠ€ΠΠ Π‘Π Π ΠΠ Π°ΠΊΠ°Π΄Π΅ΠΌΠΈΠΊΠ° ΠΠΈΠΊΡΠΎΡΠ° ΠΠ²Π³Π΅Π½ΡΠ΅Π²ΠΈΡΠ° ΠΠ°Π½ΠΈΠ½Π° Π² ΡΠ°ΠΌΠΊΠ°Ρ ΠΠ΅ΠΆΠ΄ΡΠ½Π°ΡΠΎΠ΄Π½ΠΎΠ³ΠΎ ΠΌΠ΅ΠΆΠ΄ΠΈΡΡΠΈΠΏΠ»ΠΈΠ½Π°ΡΠ½ΠΎΠ³ΠΎ ΡΠΈΠΌΠΏΠΎΠ·ΠΈΡΠΌΠ° "ΠΠ΅ΡΠ°ΡΡ ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ: ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠ° ΠΈ ΠΏΡΠΈΠ»ΠΎΠΆΠ΅Π½ΠΈΡ Π΄Π»Ρ Π½ΠΎΠ²ΡΡ ΡΠ΅Ρ Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ ΠΈ Π½Π°Π΄Π΅ΠΆΠ½ΡΡ ΠΊΠΎΠ½ΡΡΡΡΠΊΡΠΈΠΉ", 5-9 ΠΎΠΊΡΡΠ±ΡΡ 2020 Π³ΠΎΠ΄Π°, Π’ΠΎΠΌΡΠΊ, Π ΠΎΡΡΠΈΡ : ΡΠ΅Π·ΠΈΡΡ Π΄ΠΎΠΊΠ»Π°Π΄ΠΎΠ²
ΠΠ·Π΄Π°Π½ΠΈΠ΅ ΡΠΎΠ΄Π΅ΡΠΆΠΈΡ ΡΠ΅Π·ΠΈΡΡ ΠΠ΅ΠΆΠ΄ΡΠ½Π°ΡΠΎΠ΄Π½ΠΎΠΉ ΠΊΠΎΠ½ΡΠ΅ΡΠ΅Π½ΡΠΈΠΈ "Π€ΠΈΠ·ΠΈΡΠ΅ΡΠΊΠ°Ρ ΠΌΠ΅Π·ΠΎΠΌΠ΅Ρ
Π°Π½ΠΈΠΊΠ°. ΠΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ Ρ ΠΌΠ½ΠΎΠ³ΠΎΡΡΠΎΠ²Π½Π΅Π²ΠΎΠΉ ΠΈΠ΅ΡΠ°ΡΡ
ΠΈΡΠ΅ΡΠΊΠΈ ΠΎΡΠ³Π°Π½ΠΈΠ·ΠΎΠ²Π°Π½Π½ΠΎΠΉ ΡΡΡΡΠΊΡΡΡΠΎΠΉ ΠΈ ΠΈΠ½ΡΠ΅Π»Π»Π΅ΠΊΡΡΠ°Π»ΡΠ½ΡΠ΅ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΡΡΠ²Π΅Π½Π½ΡΠ΅ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ", ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠΌΠΎΠΉ Π² ΡΠ°ΠΌΠΊΠ°Ρ
ΠΠ΅ΠΆΠ΄ΡΠ½Π°ΡΠΎΠ΄Π½ΠΎΠ³ΠΎ Π΄ΠΈΡΡΠΈΠΏΠ»ΠΈΠ½Π°ΡΠ½ΠΎΠ³ΠΎ ΡΠΈΠΌΠΏΠΎΠ·ΠΈΡΠΌΠ° "ΠΠ΅ΡΠ°ΡΡ
ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ: ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠ° ΠΈ ΠΏΡΠΈΠ»ΠΎΠΆΠ΅Π½ΠΈΡ Π΄Π»Ρ Π½ΠΎΠ²ΡΡ
ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ ΠΈ Π½Π°Π΄Π΅ΠΆΠ½ΡΡ
ΠΊΠΎΠ½ΡΡΡΡΠΊΡΠΈΠΉ". Π€ΠΈΠ·ΠΈΡΠ΅ΡΠΊΠ°Ρ ΠΌΠ΅Π·ΠΎΠΌΠ΅Ρ
Π°Π½ΠΈΠΊΠ° ΡΠ²Π»ΡΠ΅ΡΡΡ Π½Π°ΡΡΠ½ΡΠΌ Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½ΠΈΠ΅ΠΌ, Π² ΡΠ°ΠΌΠΊΠ°Ρ
ΠΊΠΎΡΠΎΡΠΎΠ³ΠΎ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π» ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»ΡΠ΅ΡΡΡ ΠΊΠ°ΠΊ ΠΈΠ΅ΡΠ°ΡΡ
ΠΈΡΠ΅ΡΠΊΠ°Ρ ΡΠΈΡΡΠ΅ΠΌΠ° Π²Π·Π°ΠΈΠΌΠΎΡΠ²ΡΠ·Π°Π½Π½ΡΡ
ΡΡΡΡΠΊΡΡΡΠ½ΡΡ
(ΠΌΠ°ΡΡΡΠ°Π±Π½ΡΡ
) ΡΡΠΎΠ²Π½Π΅ΠΉ. Π ΠΊΠ½ΠΈΠ³Π΅ ΠΎΡΡΠ°ΠΆΠ΅Π½Ρ ΠΏΠΎΡΠ»Π΅Π΄Π½ΠΈΠ΅ Π΄ΠΎΡΡΠΈΠΆΠ΅Π½ΠΈΡ Π² ΠΎΠ±Π»Π°ΡΡΠΈ ΡΠ°Π·Π²ΠΈΡΠΈΡ ΠΏΡΠΈΠ½ΡΠΈΠΏΠΎΠ² ΠΈ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ»ΠΎΠ³ΠΈΠΈ ΡΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΌΠ΅Π·ΠΎΠΌΠ΅Ρ
Π°Π½ΠΈΠΊΠΈ ΠΈ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈΡ
ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΊ ΡΠΎΠ·Π΄Π°Π½ΠΈΡ ΠΏΠ΅ΡΡΠΏΠ΅ΠΊΡΠΈΠ²Π½ΡΡ
ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ² Π² ΠΈΠ½ΡΠ΅ΡΠ΅ΡΠ°Ρ
ΡΠ°Π·Π²ΠΈΡΠΈΡ Π½ΠΎΠ²ΡΡ
ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΡΡΠ²Π΅Π½Π½ΡΡ
ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ, ΠΎΡΠ²ΠΎΠ΅Π½ΠΈΡ ΠΊΠΎΡΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΏΡΠΎΡΡΡΠ°Π½ΡΡΠ²Π°, Π² ΡΠΎΠΌ ΡΠΈΡΠ»Π΅ Π΄Π°Π»ΡΠ½Π΅Π³ΠΎ ΠΊΠΎΡΠΌΠΎΡΠ°, ΡΠ»Π΅ΠΊΡΡΠΎΠ½ΠΈΠΊΠΈ, Π°ΡΠΎΠΌΠ½ΠΎΠΉ ΡΠ½Π΅ΡΠ³Π΅ΡΠΈΠΊΠΈ, Π½Π΅ΡΡΠ΅Π³Π°Π·ΠΎΠ²ΠΎΠ³ΠΎ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ°, ΠΌΠ΅Π΄ΠΈΡΠΈΠ½Ρ, ΡΡΠ°Π½ΡΠΏΠΎΡΡΠ° ΠΈ Π΄Ρ. ΠΠ½ΠΈΠ³Π° Π°Π΄ΡΠ΅ΡΠΎΠ²Π°Π½Π° Π½Π°ΡΡΠ½ΡΠΌ ΡΠΎΡΡΡΠ΄Π½ΠΈΠΊΠ°ΠΌ, ΠΈΠ½ΠΆΠ΅Π½Π΅ΡΠ°ΠΌ, Π°ΡΠΏΠΈΡΠ°Π½ΡΠ°ΠΌ ΠΈ ΡΠΏΠ΅ΡΠΈΠ°Π»ΠΈΡΡΠ°ΠΌ, Π·Π°Π½ΠΈΠΌΠ°ΡΡΠΈΠΌΡΡ Π²ΠΎΠΏΡΠΎΡΠ°ΠΌΠΈ ΡΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΌΠ΅Π·ΠΎΠΌΠ΅Ρ
Π°Π½ΠΈΠΊΠΈ, ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠΈ Π½Π°Π½ΠΎΡΡΡΡΠΊΡΡΡΠ½ΡΡ
ΠΎΠ±ΡΠ΅ΠΌΠ½ΡΡ
ΠΈ Π½Π°Π½ΠΎΡΠ°Π·ΠΌΠ΅ΡΠ½ΡΡ
ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ², Π½Π°Π½ΠΎΡΡΡΡΠΊΡΡΡΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠ½ΡΡ
ΡΠ»ΠΎΠ΅Π², ΡΠΎΠ½ΠΊΠΈΠΌΠΈ ΠΏΠ»Π΅Π½ΠΊΠ°ΠΌΠΈ ΠΈ ΠΏΠΎΠΊΡΡΡΠΈΡΠΌΠΈ, Π½Π°Π½ΠΎΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΡΠΌΠΈ, ΠΊΠΎΠΌΠΏΡΡΡΠ΅ΡΠ½ΡΠΌ ΠΊΠΎΠ½ΡΡΡΡΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π½ΠΎΠ²ΡΡ
ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ² ΠΈ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ ΠΈΡ
ΠΏΠΎΠ»ΡΡΠ΅Π½ΠΈΡ, ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΡΠΌΠΈ Π»ΠΎΠΊΠ°Π»ΡΠ½ΠΎΠΉ Π½Π΅ΡΡΠ°ΡΠΈΠΎΠ½Π°ΡΠ½ΠΎΠΉ ΠΌΠ΅ΡΠ°Π»Π»ΡΡΠ³ΠΈΠΈ ΠΈ ΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠΈ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ², Π½Π΅ΡΠ°Π·ΡΡΡΠ°ΡΡΠΈΠΌΠΈ ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌΠΈ ΠΊΠΎΠ½ΡΡΠΎΠ»Ρ