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721.
Based on the Reddy ‘s theory of plates with the effect of higher-order shear deformations, the governing equations for bending of orthotropic plates with finite deformations were established. The differential quadrature ( DQ ) method of nonlinear analysis to the problem was presented. New DQ approach, presented by Wang and Bert ( DQWB), is extended to handle the multiple boundary conditions of plates. The techniques were also further extended to simplify nonlinear computations. The numerical convergence and comparison of solutions were studied. The results show that the DQ method presented is very reliable and valid. Moreover, the influences of geometric and material parameters as well as the transverse shear deformations on nonlinear bending were investigated. Numerical results show the influence of the shear deformation on the static bending of orthotropic moderately thick plate is significant. 相似文献
722.
In this paper we derive necessary and sufficient conditions for strong ellipticity in several classes of anisotropic linearly
elastic materials. Our results cover all classes in the rhombic system (nine elasticities), four classes of the tetragonal
system (six elasticities) and all classes in the cubic system (three elasticities). As a special case we recover necessary
and sufficient conditions for strong ellipticity in transversely isotropic materials. The central result shows that for the
rhombic system strong ellipticity restricts some appropriate combinations of elasticities to take values inside a domain whose
boundary is the third order algebraic surface defined by x
2+y
2+z
2−2xyz−1=0 situated in the cube , , . For more symmetric situations, the general analysis restricts combinations of elasticities to range inside either a plane
domain (for four classes in the tetragonal system) or in an one-dimensional interval (for the hexagonal systems, transverse
isotropy and cubic system). The proof involves only the basic statement of the strong ellipticity condition.
相似文献
723.
In this paper, the saturate spacing of transverse cracks of the 90° ply is originally calculated by the 3-D finite element method. Thus, a new approach is put forward for predicting the saturate spacing of transverse cracks. 相似文献
724.
Impact of lepton p_T threshold on charge asymmetry predictions for inclusive W boson production in pp collisions at 13 TeV
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Kadir Ocalan 《中国物理C(英文版)》2021,45(8):083103-083103-9
This paper presents the impact of the lepton transverse momentum p_T~l threshold on the W boson charge asymmetry predictions in perturbative QCD for the inclusive W~++X→l~±v+X production in proton-proton(pp)collisions.The predictions are obtained at various low-p_T~l thresholds p_T~l 20,25,30,and 40 GeV in a fiducial region encompassing both the central and forward detector acceptances in terms of the lepton pseudorapidity0 ≤η_l≤4.5.The predicted distributions for the lepton charge asymmetry,which is defined by η_l(A_(η_l)),at the nextto-next-to-leading order(NNLO) accuracy are compared with the CMS and LHCb data at 8 TeV center-of-mass collision energy.The 8 TeV predictions reproduce the data fairly well within the quoted uncertainties.The predictions from the CT14 parton distribution function(PDF) model are in a slightly better agreement with the data over the other PDF sets that are tested.The 13 TeV predictions using various p_T~l thresholds are reported for A_(η_l) and the charge asymmetries that are defined in terms of the differential cross sections in bins of the W boson rapidity yw(A_(y_w)) and transverse momentum p_T~W(A_(p_T~W)).The NNLO predictions for the A_(η_l),A_(y_w).and A_(p_T~W) distributions are assessed to be in close correlation with the p_T~l value.The A_(η_l) and A_(y_w) distributions are particularly shown to be more correlated at a higher p_T~l threshold.The A_(p_T~W) distributions are also reported from the merged predictions with improved accuracy by the inclusion of the next-to-next-to-next-to-leading logarithm(N'LL) corrections,i.e.,at NNLO+N~3 LL.The predicted distributions from various p_T~l thresholds represent a finer probe in terms of the capability to provide more constraints on the ratio of u and d quark distribution functions in the parton momentum fraction range 10~(-4) x1. 相似文献
725.
Using the string melting version of a multiphase transport (AMPT) model, we analyze the transverse momentum dependence of the HBT radius \begin{document}$R_{\rm s}$\end{document} ![]()
![]()
and the single-pion angle distribution on the transverse plane in central Au+Au collisions at \begin{document}$\sqrt{S_{NN}}$\end{document} ![]()
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=19.6, 27, 39, 62.4, and 200 GeV. Additionally, a numerical connection between these two phenomena is established with a series of functions. We can estimate the single-pion angle distribution on the transverse plane from HBT analysis. 相似文献
726.
727.
墙—桩—土共同作用的位移影响系数的计算 总被引:2,自引:0,他引:2
本文根据Mindlin方程积分,推导出地下连续墙作为承重结构的墙-桩-土共同作用位移影响系数为计算公式,得到了共同作用柔度矩阵用于地下连续墙作承重结构与桩,筏(箱)基础和地基及上部结构共同作用分析中,可以得出比较满意的结果。 相似文献
728.
V. M. Tikhomirov P. G. Surovin 《Journal of Applied Mechanics and Technical Physics》2004,45(1):112-117
Experimental studies of the extension of mixedmode fatigue cracks were performed on rail steel samples. The direction of growth of fatigue cracks was studied for three types of loading: alternate transverse shear and transverse and longitudinal shears under compressing stresses. For all tested samples, the following common feature in the extension of fatigue cracks was established: the direction of crack growth coincides with the propagation direction of the principal stresses having minimum absolute values. 相似文献
729.
Change of type in the governing equations of equilibrium is examined in the context of a base neo-Hookean response augmented
with unidirectional reinforcing that is characterized by a single additional constitutive parameter for strength of reinforcement.
Plane deformations interpreted in terms of both local and global plane strain are considered. Loss of ordinary ellipticity
is found to occur for sufficiently large strength of reinforcement under sufficiently severe deformation which necessarily
involves contraction in the reinforcing direction. Loss of ellipticity in local plane strain is easily characterized, and
its incipient breakdown is associated with the possible emergence of surfaces of weak discontinuity with orientation normals
in the reinforcing direction. Loss of ellipticity in global plane strain is given a two-dimensional manifold characterization
in a space involving 2 deformation parameters and the strength of reinforcing parameter. Orientation normals for the associated
surfaces of weak discontinuity at incipient breakdown do not in general conform to the reinforcing direction.
This revised version was published online in August 2006 with corrections to the Cover Date. 相似文献
730.
Transport of dissolved species by a carrier fluid in a porous medium comprises advection and diffusion/dispersion processes. Hydrodynamic dispersion is commonly characterized by an empirical relationship, in which the dispersion mechanism is described by contributions of molecular diffusion and mechanical dispersion expressed as a function of the molecular Peclét number. Mathematically these two phenomena are modeled by a constant diffusion coefficient and by velocity dependent dispersion coefficients, respectively. Here, the commonly utilized Bear--Scheidegger dispersion model of linear proportionality between mechanical dispersion and velocity, and the more complicated Bear--Bachmat model derived on a streamtube array model porous medium and better describing observed dispersion coefficients in the moderate molecular Peclét number range, will be considered. Analyzing the mixing flow of two parallelly flowing confluent fluids with different concentrations of a dissolved species within the frames of boundary layer theory one has to deal with transverse mixing only. With the Boussinesq approximation being adopted approximate analytical solutions of the corresponding boundary layer system of equations show that there is no effect of density coupling on concentration distributions across the mixing layer in the pure molecular diffusion regime case. With the Peclét number of the oncoming flow growing beyond unity, density coupling has an increasing influence on the mixing zone. When the Peclét number grows further this influence is successively reduced until its disappearance in the pure mechanical dispersion regime. 相似文献