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IMPACT MODEL RESOLUTION ON PAINLEVE’S PARADOX 总被引:1,自引:0,他引:1
Painlevé‘s paradox is one of the basic difficulties for solving LCP of dynamic systems subjected to unilateral constraints. A bi-nonlinear parameterized impact model, consistent with dynamic principles and experimental results, is established on the localized and quasi-static impact model theory. Numerical simulations are carried out on the dynamic motion of Painlevé‘s example. The results confirm ““““impact without collision““““ in the inconsistent states of the system. A ““““critical normal force““““ which brings an important effect on the future movement of the system in the indeterminate states is found. After the motion pattern for the impact process is obtained from numerical results, a rule of the velocity‘s jump that incorporates the tangential impact process is deduced by using an approximate impulse theory and the coefficient of restitution defined by Stronge. The results of the jump rule are quite precise if the system rigidity is big enough. 相似文献
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High-power polarization-division-multiplexing (PDM) systems or functional modules, such as self-phase-modulation (SPM)-based all-optical regenerators, cross-phase-modulation (XPM)-based wavelength convertors or format convertors, all-optical logical gate, and so on, may suffer from the effects of pattern dependence. Such effects are experimentally investigated using relative time delay variation between bit sequences with orthogonal polarization states in a 2 × 10.65 Gb/s high-power on-off keying (OOK) PDM system. Eye-diagram-based signal-to-noise ratio (SNR) and bandwidth of broadened spectrum are measured and compared. An eye-diagram-based SNR fluctuation of up to 4 dB may occur as the delay changes. 相似文献
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<正>By the reaction of cadmium chloride with a reduced Schiff base ligand (H_2L = N-(4- carboxybenzyl)-glycine), a novel Cd(II) compound [Cd(HL)_2]·4H_2O (1) has been obtained. Single-crystal X-ray diffraction analysis reveals that it crystallizes in orthorhombic, space group Pbcn with a = 13.9788(8), b = 24.4204(14), c = 13.9580(8), V = 4764.8(5)~3, Z = 8, M_r = 600.84, D_c = 1.675 g/cm~3, μ = 0.983 mm~(-1), F(000) = 2448, S = 1.084, R = 0.0806 and wR = 0.1705 (I > 2σ(I)). It displays a 2D two-fold interpenetrating structure. The Cd(II) ions are six-coordinated. The cross-linkage of Cd(II) ions by the bridge of HL anions results in a [Cd(HL)_2] layer. Every two [Cd(HL)_2]_n layers are penetrated with each other, resulting in a two-fold interpenetrating double-layer structure by π-π stacking interactions and hydrogen bonds. Such double-layers are further linked by hydrogen bonds into a supramolecular structure. Photoluminescent investigation shows that compound 1 displays strong emission in the purple region. 相似文献
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