916 research outputs found

    A novel nonlinear approach to suppress resonant vibrations

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    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

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    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

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    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

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    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 mΓ—kth 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

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    In this paper, we analyze the scalar mesons f0(980)f_0(980) and f0(1500)f_0(1500) from the decays BΛ‰s0β†’f0(980)Ο€0,f0(1500)Ο€0\bar B^0_s \to f_0(980)\pi^0, f_0(1500)\pi^0 within Perturbative QCD approach. From the leading order calculations, we find that (a) in the allowed mixing angle ranges, the branching ratio of BΛ‰s0β†’f0(980)Ο€0\bar B^0_s\to f_0(980)\pi^0 is about (1.0∼1.6)Γ—10βˆ’7(1.0\sim1.6)\times 10^{-7}, which is smaller than that of BΛ‰s0β†’f0(980)K0\bar B^0_s\to f_0(980)K^0 (the difference is a few times even one order); (b) the decay BΛ‰s0β†’f0(1500)Ο€0\bar B^0_s \to f_0(1500)\pi^0 is better to distinguish between the lowest lying state or the first excited state for f0(1500)f_0(1500), 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 BΛ‰s0β†’f0(1500)Ο€0\bar B^0_s \to f_0(1500)\pi^0 for two scenarios also exists great difference. In scenario II, the variation range of the value ACPdir(BΛ‰s0β†’f0(1500)Ο€0){\cal A} ^{dir}_{CP}(\bar B^0_s \to f_0(1500)\pi^0) according to the mixing angle is very small, except for the values corresponding to the mixing angles being near 90∘90^\circ or 270∘270^\circ, while the variation range of ACPdir(BΛ‰s0β†’f0(1500)Ο€0){\cal A} ^{dir}_{CP}(\bar B^0_s \to f_0(1500)\pi^0) in scenario I is very large. Compared with the future data for the decay BΛ‰s0β†’f0(1500)Ο€0\bar B^0_s \to f_0(1500)\pi^0, it is ease to determine the nature of the scalar meson f0(1500)f_0(1500).Comment: 16 pages, 3 figures, Revte

    Coordinated Control and Estimation of Multiagent Systems with Engineering Applications

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    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

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    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

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    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’Ρ€Π΅Π½ΠΈΠ΅ ΠΈ износ Ρ‚Ρ€Π°Π΄ΠΈΡ†ΠΈΠΎΠ½Π½Ρ‹Ρ… износостойких ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ² для поясов сравнивали с этими ΠΆΠ΅ характСристиками Π½ΠΎΠ²ΠΎΠ³ΠΎ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π° для Π±ΡƒΡ€ΠΎΠ²ΠΎΠ³ΠΎ Ρ€Π°Π·Ρ€Π΅Π·Π°. Использован ΠΈΡΠΏΡ‹Ρ‚Π°Ρ‚Π΅Π»ΡŒΠ½Ρ‹ΠΉ стСнд SD-1 с ΠΊΠΎΠ½Ρ‚Ρ€Ρ‚Π΅Π»ΠΎΠΌ ΠΈΠ· стали 42Mn2V, ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΡƒΡŽΡ‰ΠΈΠΉ Ρ€Π΅ΠΆΠΈΠΌ Π³Π»ΡƒΠ±ΠΎΠΊΠΈΡ… ΠΈ свСрхглубоких скваТин, с Ρ†Π΅Π»ΡŒΡŽ Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ Ρ€Π΅ΠΊΠΎΠΌΠ΅Π½Π΄Π°Ρ†ΠΈΠ΅ΠΉ ΠΏΠΎ использованию износостойкого пояса Π² условиях трСния. Показано, Ρ‡Ρ‚ΠΎ Ρ‚Ρ€Π΅Π½ΠΈΠ΅ ΠΈ износ поликристалличСского Π°Π»ΠΌΠ°Π·Π½ΠΎΠ³ΠΎ ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ‚Π° Π³ΠΎΡ€Π°Π·Π΄ΠΎ Π½ΠΈΠΆΠ΅, Ρ‡Π΅ΠΌ Ρ‚Ρ€Π°Π΄ΠΈΡ†ΠΈΠΎΠ½Π½Ρ‹Ρ… износостойких ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ², Π½Π°ΠΏΡ€ΠΈΠΌΠ΅Ρ€, Ρ‚Ρ€Π΅Π½ΠΈΠ΅ ΠΈ износ сплава FeNiNb Π²Ρ‹ΡˆΠ΅, Ρ‡Π΅ΠΌ сплава FeCrMnMo. Из Ρ‚Ρ€Π΅Ρ… износостойких ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ² Π½Π°ΠΈΠ»ΡƒΡ‡ΡˆΡƒΡŽ Π΄Π²ΡƒΡ…ΡΡ‚ΠΎΡ€ΠΎΠ½Π½ΡŽΡŽ Π·Π°Ρ‰ΠΈΡ‚Ρƒ обСспСчиваСт Π°Π»ΠΌΠ°Π·Π½Ρ‹ΠΉ ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ‚, Ρ‡Ρ‚ΠΎ ΠΏΠΎΠ΄Ρ‚Π²Π΅Ρ€ΠΆΠ΄Π°Π΅Ρ‚ ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ Π΅Π³ΠΎ использования для поясов Π±ΡƒΡ€ΠΎΠ²Ρ‹Ρ… Ρ€Π°Π·Ρ€Π΅Π·ΠΎΠ² Π² Π³Π»ΡƒΠ±ΠΎΠΊΠΈΡ… ΠΈ свСрхглубоких скваТинах. ΠŸΡ€Π΅ΠΎΠ±Π»Π°Π΄Π°ΡŽΡ‰ΠΈΠΌ ΠΌΠ΅Ρ…Π°Π½ΠΈΠ·ΠΌΠΎΠΌ являСтся ΠΌΠΈΠΊΡ€ΠΎΠ°Π±Ρ€Π°Π·ΠΈΠ²Π½Ρ‹ΠΉ износ, сопровоТдаСмый Π°Π±Ρ€Π°Π·ΠΈΠ²Π½Ρ‹ΠΌ, ΠΏΡ€ΠΈ этом ΡΡ‚Π΅ΠΏΠ΅Π½ΡŒ износа ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ‚Π° наимСньшая

    Mechanical Properties of GF/pCBT Composites and Their Fusion-Bonded Joints: Influence of Process Parameters

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    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.Высокая Π²ΡΠ·ΠΊΠΎΡΡ‚ΡŒ плавлСния тСрмопластичСских ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ†ΠΈΠΎΠ½Π½Ρ‹Ρ… ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ² Π½Π΅ позволяСт ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΠΎΠ²Π°Ρ‚ΡŒ Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Π΅ ΠΎΠ±ΡŠΠ΅ΠΌΠ½Ρ‹Π΅ Π΄ΠΎΠ»Π΅Π²Ρ‹Π΅ ΠΊΠΎΠ½Ρ†Π΅Π½Ρ‚Ρ€Π°Ρ†ΠΈΠΈ Π°Ρ€ΠΌΠΈΡ€ΡƒΡŽΡ‰ΠΈΡ… Π½Π°ΠΏΠΎΠ»Π½ΠΈΡ‚Π΅Π»Π΅ΠΉ. Π­Ρ‚Π° ΠΏΡ€ΠΎΠ±Π»Π΅ΠΌΠ° ΠΌΠΎΠΆΠ΅Ρ‚ Π±Ρ‹Ρ‚ΡŒ Ρ€Π΅ΡˆΠ΅Π½Π° ΠΏΡƒΡ‚Π΅ΠΌ in-situ ΠΏΠΎΠ»ΠΈΠΌΠ΅Ρ€ΠΈΠ·Π°Ρ†ΠΈΠΈ Ρ†ΠΈΠΊΠ»ΠΎΠ±ΡƒΡ‚ΠΈΠ»Π΅Π½Ρ‚Π΅Ρ€Π΅Ρ„Ρ‚Π°Π»Π°Ρ‚Π½ΠΎΠΉ смолы с Ρ‡Ρ€Π΅Π·Π²Ρ‹Ρ‡Π°ΠΉΠ½ΠΎ Π½ΠΈΠ·ΠΊΠΎΠΉ Π²ΡΠ·ΠΊΠΎΡΡ‚ΡŒΡŽ. Π‘Ρ‹Π»ΠΈ ΠΈΠ·Π³ΠΎΡ‚ΠΎΠ²Π»Π΅Π½Ρ‹ ΠΏΠΎΠ»ΠΈ(Ρ†ΠΈΠΊΠ»ΠΎΠ±ΡƒΡ‚ΠΈΠ»Π΅Π½Ρ‚Π΅Ρ€Π΅Ρ„Ρ‚Π°Π»Π°Ρ‚Π½Ρ‹Π΅) ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ†ΠΈΠΎΠ½Π½Ρ‹Π΅ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Ρ‹, Π°Ρ€ΠΌΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Π΅ Π½Π΅ΠΏΡ€Π΅Ρ€Ρ‹Π²Π½Ρ‹ΠΌ стСкловолокном (CF/pCBT) с высоким Π΅Π³ΠΎ содСрТаниСм, ΠΈΠ·ΡƒΡ‡Π΅Π½Ρ‹ мСханичСскиС свойства с ΡƒΡ‡Π΅Ρ‚ΠΎΠΌ вСсовой Π΄ΠΎΠ»ΠΈ ΠΊΠ°Ρ‚Π°Π»ΠΈΠ·Π°Ρ‚ΠΎΡ€Π° ΠΈ стСпСни наполнСния Π²ΠΎΠ»ΠΎΠΊΠ½ΠΎΠΌ. ΠŸΡ€Π΅Π΄Π΅Π» прочности ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ†ΠΈΠΎΠ½Π½Ρ‹Ρ… ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ² ΠΏΡ€ΠΈ растяТСнии Π² ΠΏΡ€ΠΎΠ΄ΠΎΠ»ΡŒΠ½ΠΎΠΌ Π½Π°ΠΏΡ€Π°Π²Π»Π΅Π½ΠΈΠΈ возрос Π·Π° счСт увСличСния объСмной Π΄ΠΎΠ»ΠΈ ΠΊΠΎΠ½Ρ†Π΅Π½Ρ‚Ρ€Π°Ρ†ΠΈΠΈ Π²ΠΎΠ»ΠΎΠΊΠ½Π°, ΠΈΠ·ΡƒΡ‡Π΅Π½ΠΎ влияниС объСмной Π΄ΠΎΠ»ΠΈ Π²ΠΎΠ»ΠΎΠΊΠ½Π° Π½Π° ΠΏΡ€ΠΎΡ‡Π½ΠΎΡΡ‚ΡŒ ΠΏΡ€ΠΈ ΠΈΠ·Π³ΠΈΠ±Π΅ для ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ†ΠΈΠΎΠ½Π½Ρ‹Ρ… ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ² с высокой ΡΡ‚Π΅ΠΏΠ΅Π½ΡŒΡŽ наполнСния Π²ΠΎΠ»ΠΎΠΊΠ½ΠΎΠΌ. ΠšΡ€ΠΎΠΌΠ΅ Ρ‚ΠΎΠ³ΠΎ, исслСдованы мСханичСскиС свойства ΠΈ Ρ€Π΅ΠΆΠΈΠΌΡ‹ Ρ€Π°Π·Ρ€ΡƒΡˆΠ΅Π½ΠΈΡ GF/pCBT сварСнных ΠΏΠ»Π°Π²Π»Π΅Π½ΠΈΠ΅ΠΌ соСдинСний с Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹ΠΌ количСством Π·ΠΎΠ½ связывания Ρ€Π°Π·Π½ΠΎΠΉ Π΄Π»ΠΈΠ½Ρ‹. УстановлСно, Ρ‡Ρ‚ΠΎ ΠΌΠΎΠΆΠ½ΠΎ ΠΏΠΎΠ»ΡƒΡ‡Π°Ρ‚ΡŒ высокопрочныС ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ†ΠΈΠΎΠ½Π½Ρ‹Π΅ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Ρ‹, ΠΏΡ€ΠΈΠ³ΠΎΠ΄Π½Ρ‹Π΅ для сварСнных ΠΏΠ»Π°Π²Π»Π΅Π½ΠΈΠ΅ΠΌ конструкций

    Evaluation of the Dynamic Characteristics of AZ91D Crankcase Covers and Boxes

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    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.ДинамичСскиС испытания ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ Π½Π° ΠΊΠ°Ρ€Ρ‚Π΅Ρ€Π½Ρ‹Ρ… ΠΊΡ€Ρ‹ΡˆΠΊΠ°Ρ… ΠΈ ΠΏΠΎΠ΄Π΄ΠΎΠ½Π°Ρ… Π°Π½Π°Π»ΠΎΠ³ΠΈΡ‡Π½ΠΎΠΉ конструкции, ΠΈΠ·Π³ΠΎΡ‚ΠΎΠ²Π»Π΅Π½Π½Ρ‹Ρ… ΠΈΠ· ΠΌΠ°Π³Π½ΠΈΠ΅Π²ΠΎΠ³ΠΎ AZ91D ΠΈ алюминиСвого А380 сплавов. ΠžΡ†Π΅Π½Π΅Π½ эффСкт ΠΎΡ‚ примСнСния ΠΌΠ°Π³Π½ΠΈΠ΅Π²ΠΎΠ³ΠΎ сплава AZ91D для контроля Ρ€Π΅Π°Π»ΡŒΠ½ΠΎΠΉ Π²ΠΈΠ±Ρ€Π°Ρ†ΠΈΠΈ ΠΈ ΡˆΡƒΠΌΠ° Π½Π° основании Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€Π° ΠΈΠ½Ρ‚Π΅Π³Ρ€Π°Π»ΡŒΠ½ΠΎΠΉ частотной Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΈ ΠΎΡ‚ΠΊΠ»ΠΈΠΊΠ°, ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½ΠΎΠΉ ΠΏΠΎ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π°ΠΌ измСрСния повСрхностной Π²ΠΈΠ±Ρ€Π°Ρ†ΠΈΠΈ ΠΊΠ°Ρ€Ρ‚Π΅Ρ€Π½ΠΎΠΉ ΠΊΡ€Ρ‹ΡˆΠΊΠΈ Π² Ρ€Π°Π±ΠΎΡ‡Π΅ΠΌ Ρ€Π΅ΠΆΠΈΠΌΠ΅. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΠΏΠΎΠΊΠ°Π·Ρ‹Π²Π°ΡŽΡ‚, Ρ‡Ρ‚ΠΎ ΠΊΠ°Ρ€Ρ‚Π΅Ρ€Π½Ρ‹Π΅ ΠΊΡ€Ρ‹ΡˆΠΊΠΈ ΠΈ ΠΏΠΎΠ΄Π΄ΠΎΠ½Ρ‹, ΠΈΠ·Π³ΠΎΡ‚ΠΎΠ²Π»Π΅Π½Π½Ρ‹Π΅ ΠΈΠ· ΠΌΠ°Π³Π½ΠΈΠ΅Π²ΠΎΠ³ΠΎ AZ91D ΠΈ алюминиСвого А380 сплавов, с ΠΎΠ΄ΠΈΠ½Π°ΠΊΠΎΠ²Ρ‹ΠΌΠΈ гСомСтричСскими ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Π°ΠΌΠΈ ΠΈΠΌΠ΅ΡŽΡ‚ Π°Π½Π°Π»ΠΎΠ³ΠΈΡ‡Π½Ρ‹Π΅ Π½ΠΎΡ€ΠΌΠ°Π»ΡŒΠ½Ρ‹Π΅ характСристики. Оба ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π° взаимозамСняСмы. Однако картСрная ΠΊΡ€Ρ‹ΡˆΠΊΠ° ΠΈ ΠΏΠΎΠ΄Π΄ΠΎΠ½ ΠΈΠ· сплава AZ91D ΠΎΠ±Π»Π°Π΄Π°ΡŽΡ‚ Π½ΠΈΠ·ΠΊΠΎΠΉ ΠΆΠ΅ΡΡ‚ΠΊΠΎΡΡ‚ΡŒΡŽ. Π”ΠΎΡΡ‚ΠΈΡ‡ΡŒ Π½ΠΎΡ€ΠΌΠ°Π»ΡŒΠ½ΠΎΠ³ΠΎ тСхничСского уровня Π²ΠΈΠ±Ρ€Π°Ρ†ΠΈΠΈ ΠΈ ΡˆΡƒΠΌΠ° Π² Ρ€Π΅Π°Π»ΡŒΠ½ΠΎΠΉ конструкции Ρ‚Π°ΠΊΠΆΠ΅ Π·Π°Ρ‚Ρ€ΡƒΠ΄Π½ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ, ΠΏΠΎΡΠΊΠΎΠ»ΡŒΠΊΡƒ сплав AZ91D ΠΎΠ±Π»Π°Π΄Π°Π΅Ρ‚ высокой Π΄Π΅ΠΌΠΏΡ„ΠΈΡ€ΡƒΡŽΡ‰Π΅ΠΉ ΡΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡ‚ΡŒΡŽ. ΠŸΡ€ΠΈ ΠΎΠ΄ΠΈΠ½Π°ΠΊΠΎΠ²ΠΎΠΌ Π²ΠΎΠ·Π±ΡƒΠΆΠ΄Π΅Π½ΠΈΠΈ ΠΈ частотной характСристикС конструкции с Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹ΠΌΠΈ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Π°ΠΌΠΈ Π°Π½Π°Π»ΠΈΠ· измСрСния Π²Ρ€Π΅ΠΌΠ΅Π½Π½ΠΎΠΉ области ΠΏΠΎΠΊΠ°Π·Ρ‹Π²Π°Π΅Ρ‚, Ρ‡Ρ‚ΠΎ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ‹ увСличСния ТСсткости ΠΊΠ°Ρ€Ρ‚Π΅Ρ€Π½ΠΎΠ³ΠΎ ΠΏΠΎΠ΄Π΄ΠΎΠ½Π°, Π½Π°ΠΏΡ€ΠΈΠΌΠ΅Ρ€ Π²ΠΌΠΎΠ½Ρ‚ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ Π³Π»Π°Π²Π½ΠΎΠ³ΠΎ ΡΡ‚Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ подшипника скольТСния, ΡΠΏΠΎΡΠΎΠ±ΡΡ‚Π²ΡƒΡŽΡ‚ ΡƒΠ»ΡƒΡ‡ΡˆΠ΅Π½ΠΈΡŽ динамичСских характСристик ΠΊΠ°Ρ€Ρ‚Π΅Ρ€Π½ΠΎΠ³ΠΎ ΠΏΠΎΠ΄Π΄ΠΎΠ½Π° ΠΈΠ· сплава AZ91D
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