919 research outputs found
A novel nonlinear approach to suppress resonant vibrations
A novel approach to suppress resonant vibration is presented by employing a single degree of freedom transmissibility system which utilizes a nonlinear damping element. Studies have shown that the nonlinear damping element can reduce the output energy at the driving frequency and at the same time spread the output signal energy over a wider range of harmonics. It will also be shown that the reduction becomes larger as the nonlinear damping characteristic gets stronger and in most cases, the power at the harmonics in the output spectrum will be much less if the nonlinear damping characteristic is an odd function. Hence, an odd polynomial nonlinear damping element can be introduced between the incoming signal and the structure of interest to suppress resonant vibration. An expression is derived to express the transmitted force spectrum in terms of the nonlinear generalized frequency response functions, to clearly show how the energy, at the excitation frequency, is modified by the nonlinearity
Suppressing resonant vibrations using nonlinear springs and dampers
The energy entering the resonant region of a system can be significantly reduced by introducing designed nonlinearities into the system. The basic choice of the nonlinearity can be either a nonlinear spring element or a nonlinear damping element. A numerical algorithm to compute and compare the energy reduction produced by these two types of designed elements is proposed in this study. Analytical results are used to demonstrate the procedure. The numerical results indicate that the designed nonlinear damping element produces low levels of energy at the higher order harmonics and no bifurcations in the system output response. In contrast the nonlinear spring based designs induce significant energy at the harmonics and can produce bifurcation behaviour. The conclusions provide an important basis for the design of nonlinear materials and nonlinear engineering systems
Model structure detection and system identification of metal rubber devices
Metal rubber (MR) devices, a new wire mesh material, have been extensively used in recent years due to several unique properties especially in adverse environments. Although many practical studies have been completed, the related theoretical research on metal rubber is still in its infancy. In this paper, a semi-constitutive dynamic model that involves nonlinear elastic stiffness, nonlinear viscous damping and bilinear hysteresis Coulomb damping is adopted to model MR devices. After approximating the bilinear hysteresis damping using Chebyshev polynomials of the first kind, a very efficient procedure based on the orthogonal least squares (OLS) algorithm and the adjustable prediction error sum of squares (APRESS) criterion is proposed for model structure detection and parameter estimation of an MR device for the first time. The OLS algorithm provides a powerful tool to effectively select the significant model terms step by step, one at a time, by orthogonalizing the associated terms and maximizing the error reduction ratio, in a forward stepwise procedure. The APRESS statistic regularizes the OLS algorithm to facilitate the determination of the optimal number of model terms that should be included into the dynamic model. Because of the orthogonal property of the OLS algorithm, the approach leads to a parsimonious model. Numerical ill-conditioning problems confronted by the conventional least squares algorithm can also be avoided by the new approach. Finally by utilising the transient response of a MR specimen, it is shown how the model structure can be detected in a practical application. The identified model agrees with the experimental measurements very well
Investigation on contribution of inductance harmonics to torque production in multiphase doubly salient synchronous reluctance machines
This paper investigates the contribution of each order inductance harmonic to the torque (both average torque and torque ripple) of multiphase doubly salient synchronous reluctance machines (DS-SRMs). Such machines are similar to switched reluctance machines but supplied with sinewave currents. The investigations in this paper are as follows: first, a general analytical torque model based on Fourier Series analysis of inductances has been built for machines with different phase numbers, slot/pole number combinations and also winding configurations. The instantaneous torque for DS-SRMs with any given phase number can then be accurately predicted. Using such model, contribution of each order inductance harmonic to torque can be investigated separately. It is found that the torque ripple frequency of the DS-SRM only depends on phase number. For example, for a m-phase machine, there will be mΓkth order torque ripple if mod(mk,2)=0, where m is phase number and k is a natural number. This study also explains why certain phase numbers inherently produce lower torque ripple than others. The findings in this paper provide a future direction for potential torque ripple reduction methods either from machine design or advanced control. The simulations have been validated by experiments using a 6-phase DS-SRMs
Study of f_0(980) and f_0(1500) from B_s \to f_0(980)\pi, f_0(1500)\pi Decays
In this paper, we analyze the scalar mesons and from
the decays within Perturbative
QCD approach. From the leading order calculations, we find that (a) in the
allowed mixing angle ranges, the branching ratio of is about , which is smaller than
that of (the difference is a few times even one
order); (b) the decay is better to distinguish
between the lowest lying state or the first excited state for ,
because the branching ratios for two scenarios have about one-order difference
in most of the mixing angle ranges; and (c) the direct CP asymmetries of for two scenarios also exists great difference. In
scenario II, the variation range of the value according to the mixing angle is very small, except for
the values corresponding to the mixing angles being near or
, while the variation range of in scenario I is very large. Compared with the future data for
the decay , it is ease to determine the nature
of the scalar meson .Comment: 16 pages, 3 figures, Revte
Coordinated Control and Estimation of Multiagent Systems with Engineering Applications
Recently, coordinated control and estimation problems have attracted a great deal of attention in different fields especially in biology, physics, computer science, and control engineering. Coordinated control and estimation problems have prominent characteristics of distributed control, local interaction, and self-organization. Research on multiagent coordinated control and estimation problems not only helps better understand the mechanisms of natural collective phenomena but also benefits the applications of cyberphysical systems.
This special issue focuses on theoretical and technological achievements in cooperative multiagent Systems. It contains twenty-six papers, the contents of which are summarized below
Influence of casting temperature on the thermal stability of Cu- and Zr-based metallic glasses: theoretical analysis and experiments
Influence of casting temperature on the thermal stability of Cu- and Zr-based metallic glasses (MGs) was analyzed based on the monomer-cluster structural model using the Johnson-Mehl-Avrami (JMA) equation. The result indicates that increasing the casting temperature can enhance the thermal stability of MGs. It is suggested that it be attributed to the decrease in the amount of the local ordering clusters induced by the elevating casting temperature. The prediction is confirmed by continuous heating transformation diagrams constructed for the Cu- and Zr-amorphous samples obtained under different casting temperatures
Friction and Wear Behavior of Wear-Resistant Belts in Drill Joints for Deep and Ultra-Deep Wells
The friction and wear of an new material for the drill joint were compared with those of traditional wear-resistant belt materials using an SD-1 test rig against a 42Mn2V steel counterface under deep and ultra-deep well conditions. This provides recommendations as to the tribological application of the wear-resistant belt. The results obtained strongly indicate that the friction and wear of a polycrystalline diamond (PCD) composite are much lower than those of the traditional wear-resistant belt materials. Among those materials, the friction and wear behavior of a FeNiNb alloy are higher than those of a FeCrMnMo alloy. Of the three wear-resistant belt materials, the bilateral protection performance of a PCD composite is the best one. It is feasible to use this composite as the wear-resistant belt material in the drill joint for deep and ultra-deep wells. The dominant wear mechanism of the wear-resistant belt materials is the microcutting wear, accompanied by the adhesive one. In addition, the wear degree of the PCD composite is the least one.Π’ΡΠ΅Π½ΠΈΠ΅ ΠΈ ΠΈΠ·Π½ΠΎΡ ΡΡΠ°Π΄ΠΈΡΠΈΠΎΠ½Π½ΡΡ
ΠΈΠ·Π½ΠΎΡΠΎΡΡΠΎΠΉΠΊΠΈΡ
ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ² Π΄Π»Ρ ΠΏΠΎΡΡΠΎΠ² ΡΡΠ°Π²Π½ΠΈΠ²Π°Π»ΠΈ Ρ ΡΡΠΈΠΌΠΈ ΠΆΠ΅ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠ°ΠΌΠΈ Π½ΠΎΠ²ΠΎΠ³ΠΎ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Π° Π΄Π»Ρ Π±ΡΡΠΎΠ²ΠΎΠ³ΠΎ ΡΠ°Π·ΡΠ΅Π·Π°. ΠΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ ΠΈΡΠΏΡΡΠ°ΡΠ΅Π»ΡΠ½ΡΠΉ ΡΡΠ΅Π½Π΄ SD-1 Ρ ΠΊΠΎΠ½ΡΡΡΠ΅Π»ΠΎΠΌ ΠΈΠ· ΡΡΠ°Π»ΠΈ 42Mn2V, ΠΌΠΎΠ΄Π΅Π»ΠΈΡΡΡΡΠΈΠΉ ΡΠ΅ΠΆΠΈΠΌ Π³Π»ΡΠ±ΠΎΠΊΠΈΡ
ΠΈ ΡΠ²Π΅ΡΡ
Π³Π»ΡΠ±ΠΎΠΊΠΈΡ
ΡΠΊΠ²Π°ΠΆΠΈΠ½, Ρ ΡΠ΅Π»ΡΡ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠΈ ΡΠ΅ΠΊΠΎΠΌΠ΅Π½Π΄Π°ΡΠΈΠ΅ΠΉ ΠΏΠΎ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΠΈΠ·Π½ΠΎΡΠΎΡΡΠΎΠΉΠΊΠΎΠ³ΠΎ ΠΏΠΎΡΡΠ° Π² ΡΡΠ»ΠΎΠ²ΠΈΡΡ
ΡΡΠ΅Π½ΠΈΡ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΡΡΠ΅Π½ΠΈΠ΅ ΠΈ ΠΈΠ·Π½ΠΎΡ ΠΏΠΎΠ»ΠΈΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π°Π»ΠΌΠ°Π·Π½ΠΎΠ³ΠΎ ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠ° Π³ΠΎΡΠ°Π·Π΄ΠΎ Π½ΠΈΠΆΠ΅, ΡΠ΅ΠΌ ΡΡΠ°Π΄ΠΈΡΠΈΠΎΠ½Π½ΡΡ
ΠΈΠ·Π½ΠΎΡΠΎΡΡΠΎΠΉΠΊΠΈΡ
ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ², Π½Π°ΠΏΡΠΈΠΌΠ΅Ρ, ΡΡΠ΅Π½ΠΈΠ΅ ΠΈ ΠΈΠ·Π½ΠΎΡ ΡΠΏΠ»Π°Π²Π° FeNiNb Π²ΡΡΠ΅, ΡΠ΅ΠΌ ΡΠΏΠ»Π°Π²Π° FeCrMnMo. ΠΠ· ΡΡΠ΅Ρ
ΠΈΠ·Π½ΠΎΡΠΎΡΡΠΎΠΉΠΊΠΈΡ
ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ² Π½Π°ΠΈΠ»ΡΡΡΡΡ Π΄Π²ΡΡ
ΡΡΠΎΡΠΎΠ½Π½ΡΡ Π·Π°ΡΠΈΡΡ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠΈΠ²Π°Π΅Ρ Π°Π»ΠΌΠ°Π·Π½ΡΠΉ ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ, ΡΡΠΎ ΠΏΠΎΠ΄ΡΠ²Π΅ΡΠΆΠ΄Π°Π΅Ρ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ Π΅Π³ΠΎ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ Π΄Π»Ρ ΠΏΠΎΡΡΠΎΠ² Π±ΡΡΠΎΠ²ΡΡ
ΡΠ°Π·ΡΠ΅Π·ΠΎΠ² Π² Π³Π»ΡΠ±ΠΎΠΊΠΈΡ
ΠΈ ΡΠ²Π΅ΡΡ
Π³Π»ΡΠ±ΠΎΠΊΠΈΡ
ΡΠΊΠ²Π°ΠΆΠΈΠ½Π°Ρ
. ΠΡΠ΅ΠΎΠ±Π»Π°Π΄Π°ΡΡΠΈΠΌ ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠΎΠΌ ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΌΠΈΠΊΡΠΎΠ°Π±ΡΠ°Π·ΠΈΠ²Π½ΡΠΉ ΠΈΠ·Π½ΠΎΡ, ΡΠΎΠΏΡΠΎΠ²ΠΎΠΆΠ΄Π°Π΅ΠΌΡΠΉ Π°Π±ΡΠ°Π·ΠΈΠ²Π½ΡΠΌ, ΠΏΡΠΈ ΡΡΠΎΠΌ ΡΡΠ΅ΠΏΠ΅Π½Ρ ΠΈΠ·Π½ΠΎΡΠ° ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠ° Π½Π°ΠΈΠΌΠ΅Π½ΡΡΠ°Ρ
Mechanical Properties of GF/pCBT Composites and Their Fusion-Bonded Joints: Influence of Process Parameters
High melting viscosity of thermoplastic composites gives no way of using substantial volume fractions of reinforcing agents. This problem can be solved by in-situ polymerization of an extremely low-viscosity cyclic butylene terephthalate (CBT) resin. Continuous glass fiber-reinforced poly(cyclic butylene terephthalate) (GF/Γ°CBT) composites with high fiber fractions were manufactured, and the mechanical properties as a function of the catalyst mass fraction and fiber filling ratio were studied. The longitudinal tensile strength of the composites was enhanced by increasing the fiber volume fraction, and the influence of the fiber fraction on the bending strength of high fiber filling-ratio composites was evaluated. Furthermore, the mechanical properties and failure modes of GF/Γ°CBT fusion-bonded joints with different number of bonding areas of different lengths were investigated. It was found that high-strength composite materials can be obtained, which are applicable for fusion-bonded structures.ΠΡΡΠΎΠΊΠ°Ρ Π²ΡΠ·ΠΊΠΎΡΡΡ ΠΏΠ»Π°Π²Π»Π΅Π½ΠΈΡ ΡΠ΅ΡΠΌΠΎΠΏΠ»Π°ΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠΈΠΎΠ½Π½ΡΡ
ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ² Π½Π΅ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°ΡΡ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΡΠ΅ ΠΎΠ±ΡΠ΅ΠΌΠ½ΡΠ΅ Π΄ΠΎΠ»Π΅Π²ΡΠ΅ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠΈ Π°ΡΠΌΠΈΡΡΡΡΠΈΡ
Π½Π°ΠΏΠΎΠ»Π½ΠΈΡΠ΅Π»Π΅ΠΉ. ΠΡΠ° ΠΏΡΠΎΠ±Π»Π΅ΠΌΠ° ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ ΡΠ΅ΡΠ΅Π½Π° ΠΏΡΡΠ΅ΠΌ in-situ ΠΏΠΎΠ»ΠΈΠΌΠ΅ΡΠΈΠ·Π°ΡΠΈΠΈ ΡΠΈΠΊΠ»ΠΎΠ±ΡΡΠΈΠ»Π΅Π½ΡΠ΅ΡΠ΅ΡΡΠ°Π»Π°ΡΠ½ΠΎΠΉ ΡΠΌΠΎΠ»Ρ Ρ ΡΡΠ΅Π·Π²ΡΡΠ°ΠΉΠ½ΠΎ Π½ΠΈΠ·ΠΊΠΎΠΉ Π²ΡΠ·ΠΊΠΎΡΡΡΡ. ΠΡΠ»ΠΈ ΠΈΠ·Π³ΠΎΡΠΎΠ²Π»Π΅Π½Ρ ΠΏΠΎΠ»ΠΈ(ΡΠΈΠΊΠ»ΠΎΠ±ΡΡΠΈΠ»Π΅Π½ΡΠ΅ΡΠ΅ΡΡΠ°Π»Π°ΡΠ½ΡΠ΅) ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠΈΠΎΠ½Π½ΡΠ΅ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ, Π°ΡΠΌΠΈΡΠΎΠ²Π°Π½Π½ΡΠ΅ Π½Π΅ΠΏΡΠ΅ΡΡΠ²Π½ΡΠΌ ΡΡΠ΅ΠΊΠ»ΠΎΠ²ΠΎΠ»ΠΎΠΊΠ½ΠΎΠΌ (CF/pCBT) Ρ Π²ΡΡΠΎΠΊΠΈΠΌ Π΅Π³ΠΎ ΡΠΎΠ΄Π΅ΡΠΆΠ°Π½ΠΈΠ΅ΠΌ, ΠΈΠ·ΡΡΠ΅Π½Ρ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΠ²ΠΎΠΉΡΡΠ²Π° Ρ ΡΡΠ΅ΡΠΎΠΌ Π²Π΅ΡΠΎΠ²ΠΎΠΉ Π΄ΠΎΠ»ΠΈ ΠΊΠ°ΡΠ°Π»ΠΈΠ·Π°ΡΠΎΡΠ° ΠΈ ΡΡΠ΅ΠΏΠ΅Π½ΠΈ Π½Π°ΠΏΠΎΠ»Π½Π΅Π½ΠΈΡ Π²ΠΎΠ»ΠΎΠΊΠ½ΠΎΠΌ. ΠΡΠ΅Π΄Π΅Π» ΠΏΡΠΎΡΠ½ΠΎΡΡΠΈ ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠΈΠΎΠ½Π½ΡΡ
ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ² ΠΏΡΠΈ ΡΠ°ΡΡΡΠΆΠ΅Π½ΠΈΠΈ Π² ΠΏΡΠΎΠ΄ΠΎΠ»ΡΠ½ΠΎΠΌ Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½ΠΈΠΈ Π²ΠΎΠ·ΡΠΎΡ Π·Π° ΡΡΠ΅Ρ ΡΠ²Π΅Π»ΠΈΡΠ΅Π½ΠΈΡ ΠΎΠ±ΡΠ΅ΠΌΠ½ΠΎΠΉ Π΄ΠΎΠ»ΠΈ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠΈ Π²ΠΎΠ»ΠΎΠΊΠ½Π°, ΠΈΠ·ΡΡΠ΅Π½ΠΎ Π²Π»ΠΈΡΠ½ΠΈΠ΅ ΠΎΠ±ΡΠ΅ΠΌΠ½ΠΎΠΉ Π΄ΠΎΠ»ΠΈ Π²ΠΎΠ»ΠΎΠΊΠ½Π° Π½Π° ΠΏΡΠΎΡΠ½ΠΎΡΡΡ ΠΏΡΠΈ ΠΈΠ·Π³ΠΈΠ±Π΅ Π΄Π»Ρ ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠΈΠΎΠ½Π½ΡΡ
ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ² Ρ Π²ΡΡΠΎΠΊΠΎΠΉ ΡΡΠ΅ΠΏΠ΅Π½ΡΡ Π½Π°ΠΏΠΎΠ»Π½Π΅Π½ΠΈΡ Π²ΠΎΠ»ΠΎΠΊΠ½ΠΎΠΌ. ΠΡΠΎΠΌΠ΅ ΡΠΎΠ³ΠΎ, ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΠ²ΠΎΠΉΡΡΠ²Π° ΠΈ ΡΠ΅ΠΆΠΈΠΌΡ ΡΠ°Π·ΡΡΡΠ΅Π½ΠΈΡ GF/pCBT ΡΠ²Π°ΡΠ΅Π½Π½ΡΡ
ΠΏΠ»Π°Π²Π»Π΅Π½ΠΈΠ΅ΠΌ ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠΉ Ρ ΡΠ°Π·Π»ΠΈΡΠ½ΡΠΌ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²ΠΎΠΌ Π·ΠΎΠ½ ΡΠ²ΡΠ·ΡΠ²Π°Π½ΠΈΡ ΡΠ°Π·Π½ΠΎΠΉ Π΄Π»ΠΈΠ½Ρ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ ΠΌΠΎΠΆΠ½ΠΎ ΠΏΠΎΠ»ΡΡΠ°ΡΡ Π²ΡΡΠΎΠΊΠΎΠΏΡΠΎΡΠ½ΡΠ΅ ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠΈΠΎΠ½Π½ΡΠ΅ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ, ΠΏΡΠΈΠ³ΠΎΠ΄Π½ΡΠ΅ Π΄Π»Ρ ΡΠ²Π°ΡΠ΅Π½Π½ΡΡ
ΠΏΠ»Π°Π²Π»Π΅Π½ΠΈΠ΅ΠΌ ΠΊΠΎΠ½ΡΡΡΡΠΊΡΠΈΠΉ
Evaluation of the Dynamic Characteristics of AZ91D Crankcase Covers and Boxes
Dynamic tests are performed on similarly structured crankcase covers and boxes made of AZ91D magnesium and A380 aluminum alloys. The real vibration and noise control effect of an AZ91D magnesium alloy is evaluated, based on the behavior of the integral frequency response function, which is derived from the measured surface vibrations of the crankcase cover under operating conditions. The results indicate that crankcase covers and boxes made of AZ91D magnesium and A380 aluminum alloys with the same geometry possess similar normal characteristics. Both materials are interchangeable. However, the stiffness of AZ91D crankcase covers and boxes is poor. It is also difficult to obtain good engineering vibration and noise effects in the real structure due to an AZ91D high damping capacity. At the same excitation and frequency response at different structure characteristics, the measurement analysis of time-domain response indicates that methods to strengthen the crankcase box stiffness, such as embedding a main bearing steel sleeve, is favorable for improving the dynamic characteristics of an AZ91D crankcase box.ΠΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΈΡΠΏΡΡΠ°Π½ΠΈΡ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ Π½Π° ΠΊΠ°ΡΡΠ΅ΡΠ½ΡΡ
ΠΊΡΡΡΠΊΠ°Ρ
ΠΈ ΠΏΠΎΠ΄Π΄ΠΎΠ½Π°Ρ
Π°Π½Π°Π»ΠΎΠ³ΠΈΡΠ½ΠΎΠΉ ΠΊΠΎΠ½ΡΡΡΡΠΊΡΠΈΠΈ, ΠΈΠ·Π³ΠΎΡΠΎΠ²Π»Π΅Π½Π½ΡΡ
ΠΈΠ· ΠΌΠ°Π³Π½ΠΈΠ΅Π²ΠΎΠ³ΠΎ AZ91D ΠΈ Π°Π»ΡΠΌΠΈΠ½ΠΈΠ΅Π²ΠΎΠ³ΠΎ Π380 ΡΠΏΠ»Π°Π²ΠΎΠ². ΠΡΠ΅Π½Π΅Π½ ΡΡΡΠ΅ΠΊΡ ΠΎΡ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΌΠ°Π³Π½ΠΈΠ΅Π²ΠΎΠ³ΠΎ ΡΠΏΠ»Π°Π²Π° AZ91D Π΄Π»Ρ ΠΊΠΎΠ½ΡΡΠΎΠ»Ρ ΡΠ΅Π°Π»ΡΠ½ΠΎΠΉ Π²ΠΈΠ±ΡΠ°ΡΠΈΠΈ ΠΈ ΡΡΠΌΠ° Π½Π° ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΠΈ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠ° ΠΈΠ½ΡΠ΅Π³ΡΠ°Π»ΡΠ½ΠΎΠΉ ΡΠ°ΡΡΠΎΡΠ½ΠΎΠΉ ΡΡΠ½ΠΊΡΠΈΠΈ ΠΎΡΠΊΠ»ΠΈΠΊΠ°, ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΠΎΠΉ ΠΏΠΎ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ°ΠΌ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΡ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠ½ΠΎΠΉ Π²ΠΈΠ±ΡΠ°ΡΠΈΠΈ ΠΊΠ°ΡΡΠ΅ΡΠ½ΠΎΠΉ ΠΊΡΡΡΠΊΠΈ Π² ΡΠ°Π±ΠΎΡΠ΅ΠΌ ΡΠ΅ΠΆΠΈΠΌΠ΅. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΏΠΎΠΊΠ°Π·ΡΠ²Π°ΡΡ, ΡΡΠΎ ΠΊΠ°ΡΡΠ΅ΡΠ½ΡΠ΅ ΠΊΡΡΡΠΊΠΈ ΠΈ ΠΏΠΎΠ΄Π΄ΠΎΠ½Ρ, ΠΈΠ·Π³ΠΎΡΠΎΠ²Π»Π΅Π½Π½ΡΠ΅ ΠΈΠ· ΠΌΠ°Π³Π½ΠΈΠ΅Π²ΠΎΠ³ΠΎ AZ91D ΠΈ Π°Π»ΡΠΌΠΈΠ½ΠΈΠ΅Π²ΠΎΠ³ΠΎ Π380 ΡΠΏΠ»Π°Π²ΠΎΠ², Ρ ΠΎΠ΄ΠΈΠ½Π°ΠΊΠΎΠ²ΡΠΌΠΈ Π³Π΅ΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠ°ΠΌΠΈ ΠΈΠΌΠ΅ΡΡ Π°Π½Π°Π»ΠΎΠ³ΠΈΡΠ½ΡΠ΅ Π½ΠΎΡΠΌΠ°Π»ΡΠ½ΡΠ΅ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠΈ. ΠΠ±Π° ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Π° Π²Π·Π°ΠΈΠΌΠΎΠ·Π°ΠΌΠ΅Π½ΡΠ΅ΠΌΡ. ΠΠ΄Π½Π°ΠΊΠΎ ΠΊΠ°ΡΡΠ΅ΡΠ½Π°Ρ ΠΊΡΡΡΠΊΠ° ΠΈ ΠΏΠΎΠ΄Π΄ΠΎΠ½ ΠΈΠ· ΡΠΏΠ»Π°Π²Π° AZ91D ΠΎΠ±Π»Π°Π΄Π°ΡΡ Π½ΠΈΠ·ΠΊΠΎΠΉ ΠΆΠ΅ΡΡΠΊΠΎΡΡΡΡ. ΠΠΎΡΡΠΈΡΡ Π½ΠΎΡΠΌΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΡΠ΅Ρ
Π½ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΡΠΎΠ²Π½Ρ Π²ΠΈΠ±ΡΠ°ΡΠΈΠΈ ΠΈ ΡΡΠΌΠ° Π² ΡΠ΅Π°Π»ΡΠ½ΠΎΠΉ ΠΊΠΎΠ½ΡΡΡΡΠΊΡΠΈΠΈ ΡΠ°ΠΊΠΆΠ΅ Π·Π°ΡΡΡΠ΄Π½ΠΈΡΠ΅Π»ΡΠ½ΠΎ, ΠΏΠΎΡΠΊΠΎΠ»ΡΠΊΡ ΡΠΏΠ»Π°Π² AZ91D ΠΎΠ±Π»Π°Π΄Π°Π΅Ρ Π²ΡΡΠΎΠΊΠΎΠΉ Π΄Π΅ΠΌΠΏΡΠΈΡΡΡΡΠ΅ΠΉ ΡΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡΡΡ. ΠΡΠΈ ΠΎΠ΄ΠΈΠ½Π°ΠΊΠΎΠ²ΠΎΠΌ Π²ΠΎΠ·Π±ΡΠΆΠ΄Π΅Π½ΠΈΠΈ ΠΈ ΡΠ°ΡΡΠΎΡΠ½ΠΎΠΉ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠ΅ ΠΊΠΎΠ½ΡΡΡΡΠΊΡΠΈΠΈ Ρ ΡΠ°Π·Π»ΠΈΡΠ½ΡΠΌΠΈ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠ°ΠΌΠΈ Π°Π½Π°Π»ΠΈΠ· ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΡ Π²ΡΠ΅ΠΌΠ΅Π½Π½ΠΎΠΉ ΠΎΠ±Π»Π°ΡΡΠΈ ΠΏΠΎΠΊΠ°Π·ΡΠ²Π°Π΅Ρ, ΡΡΠΎ ΠΌΠ΅ΡΠΎΠ΄Ρ ΡΠ²Π΅Π»ΠΈΡΠ΅Π½ΠΈΡ ΠΆΠ΅ΡΡΠΊΠΎΡΡΠΈ ΠΊΠ°ΡΡΠ΅ΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ΄Π΄ΠΎΠ½Π°, Π½Π°ΠΏΡΠΈΠΌΠ΅Ρ Π²ΠΌΠΎΠ½ΡΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ Π³Π»Π°Π²Π½ΠΎΠ³ΠΎ ΡΡΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ΄ΡΠΈΠΏΠ½ΠΈΠΊΠ° ΡΠΊΠΎΠ»ΡΠΆΠ΅Π½ΠΈΡ, ΡΠΏΠΎΡΠΎΠ±ΡΡΠ²ΡΡΡ ΡΠ»ΡΡΡΠ΅Π½ΠΈΡ Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ ΠΊΠ°ΡΡΠ΅ΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ΄Π΄ΠΎΠ½Π° ΠΈΠ· ΡΠΏΠ»Π°Π²Π° AZ91D
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