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1.
本文采用直接数值模拟方法,对惯性颗粒所见均匀各向同性湍流中具有平均标量梯度的被动标量场统计特性进行了研究。模拟结果表明:与颗粒所见流体速度的自相关特性不同,颗粒所见标量的自相关特性随颗粒惯性的增加而单调减少;颗粒所见标量脉动能随颗粒惯性的增加先减少再增大,在St≈1.0的临界颗粒附近达到最小值,而颗粒所见标量耗散率随颗粒惯性的变化行为与颗粒所见标量脉动能的变化行为相反;数值模拟的结果进一步揭示,在St≈1.0时颗粒所见流体标量脉动能和耗散率的极值是因为St≈1.0的临界颗粒聚集于低涡量、高应变区域和标量场在高应变区域形成强耗散的片状结构所致。  相似文献   

2.
本文采用DNS方法,对惯性颗粒所见各向同性湍流中具有平均标量梯度的被动标量场统计特性进行了研究。结果表明:惯性对颗粒温度脉动强度,两相温度关联,自相关特性以及颗粒热流与两相交叉热流的统计特性具有明显的影响。在PDF方法的框架下,系统地推导了非等温气固两相流的PDF方程,且基于朗之万随机体系对方程进行了封闭,并利用前面的...  相似文献   

3.
In the context of the topcolor-assisted technicolor (TC2) model, we consider the production of the neutral scalar S(πt0 or ht0) associated with a photon at the LHC and compare our results with those given by the minimal supersymmetric extension of the Standard Model (MSSM). We find that its production cross section is larger or smaller than that of the scalar particle predicted by the MSSM model, depending on the values of the relevant free parameters.  相似文献   

4.
The training effect and the hysteresis behaviour of the angular dependence of exchange bias are extensively investigated upon the variation of the IrMn layer thickness tXrMn in a series of Co/IrMn bilayers. When tIrMn is very small, both of them are negligible. Then they increase very sharply with increasing tUMn and then reach maxima at almost the same value OftXrMn. Finally they both decrease when tIrMn is further increased. The similar variation trends suggest that these phenomena arise from irreversible change of antiferromagnet spin orientations, according to the thermal activation model.  相似文献   

5.
本文采用直接数值模拟的方法从颗粒所见的流场拓扑结构这一角度探讨了颗粒在不同拓扑结构下速度统计特性.结果表明,不同惯性的颗粒所见流体的速度特性类似,在Top1和Top2结构中,随时间演化而减少,而在Top3和Top4结构中随时间有波浪性的增长;由于颗粒惯性的差异引起的轨道交叉效应不同,颗粒与颗粒所见流体速度的关联随颗粒增大而衰减加剧,在颗粒与流体相之间的能量传递中,不同拓扑结构明显不同,从颗粒加入时能量由颗粒相向流体传递,各拓扑结构的相对强度为Top2>Top4>Top1>Top3,演化到后期能量由流体相向颗粒相传递,相对强度为Top1>Top2>Top3>Top4;st=1.0和st=10.0的颗粒差别在于演化后期Top2和Top3相对强度的转变.  相似文献   

6.
The scale for visible jets produced in e+e Collisions is studied in some details using Monte Carlo method. It is demonstrated, based on the historical fact that the 3-jet events were firstly observed in e+ e- experiments at √S=17—30GeV,and the relative transverse momentum for visible jets is in the region kt,~5—10GeV/c. It is further shown, using a concrete example, that the number of jets in an event could be correctly evaluated only when kt is in this region. The dynamical fluctuations inside jets determined through different values of kt are compared carefully. It turns out that only when kt,~5—10GeV/c the dynamical fluctuations inside jets will possess the best anomalous scaling property. The relation between the scale 5-10GeV/c of visible jets and the scale 1-2GeV of perturbative QCD is discussed.  相似文献   

7.
A realistic calculation of the inertia for 236U fisson based on the linear response theory is presented, in which the single particle states are provided by Nilsson model. The dependence of the nuclear inertia Mδiδi on the collective variables δ2, δ4 is studied at the range of certain nuclear temperature (0—1 MeV). The pairing effect and the shell effect on the nuclear inertia are discussed. The calculated results show a very prominent structure at level crossing points and when acrossing the critical temperature.  相似文献   

8.
The solvability of the Lichnerowicz-York equation is discussed on each sliceS t=IR3 of a spacelike, asymptotically Euclidean maximal foliation {S τ}. Following Cantor, the problem is reduced to a discussion of the properties of a smooth, time-dependent, family of conformal transformations,ø t, relating the physical metrich tofS t to a metric ? t =ø 4ht, with vanishing scalar curvature. An estimate is provided for infø t. This allows us to examine the properties of the scale geometry on eachS twhen strong field regions are probed. It is shown that in such regions ? t tends to become degenerate exponentially as a suitable average of the scalar curvature of (S t, h t ) increases. This is interpreted as representing the approach to a singular regime for (S t, h t ). An estimate is also provided for the lapse function-N t defining {S t}. This is found to be in agreement with a similar estimate suggested, on heuristic grounds, by Smarr and York. This latter result indicates that asymptotically flat maximal slicings in general (but not always) avoid reaching regions where the above singular regime is approached.  相似文献   

9.
埃洛石的Birch-Murnaghan状态方程和高压物性   总被引:1,自引:1,他引:0       下载免费PDF全文
 用欧拉有限应变理论分析了埃洛石的冲击Hugoniot实验数据,得到了其低压相和高压相的等熵体积模量K0S及其对压力的一阶导数K′0S。对低压相,在γ=0.43(ρ0/ρ)时,K0S=32.16 GPa,K′0S=7.17;对高压相,在γ=1.0(ρ0/ρ)1.5、且相变能各取579.1 J/g(常压下的值)和1 000 J/g时,K0S、K′0S分别为103.28 GPa 、4.97和95.85 GPa、5.35。根据高压下物性参数的跃变,讨论并分析了其各个相区物质组成的差异。  相似文献   

10.
KNN Based Lead-Free Piezoceramics with Improved Thermal Stability   总被引:1,自引:0,他引:1       下载免费PDF全文
Lead-free piezoelectric ceramics (1 - x) (Na0.53K0.404 Li0.066)Nb0.92 Sb0.08 03 +xZrTiO3 are fabricated by conventional solid-state sintering method, and their dielectric and piezoelectric characteristics are investigated. With the addition of SrTiO3, the growth of the grain size is restrained, meanwhile the phase transition temperature of orthorhombic-tetragonal is shifted below room temperature. It is found that the ceramics with x = 0.010 exhibit excellent piezoelectric properties (d33 = 220 pC/N, kp = 41%, kt = 39%) and improved thermal stability around room temperature. The results indicate that these materials are promising lead-free piezoceramics for practical operations.  相似文献   

11.
无氧铜等熵卸载路径的实验研究   总被引:3,自引:2,他引:1       下载免费PDF全文
 采用化爆加载,以黄铜为飞片、无氧铜为靶板,测量了以抗氢钢(HR2)、重玻璃(SiO2)、铝合金(LY12/LF6)、镁铝合金(MB2)、有机玻璃(PMMA)和空气(Air)为垫块(Anvil)材料中的冲击波速度(上述材料的Hugoniot状态参数C0、λ均为已知),由此确定了无氧铜的等熵卸载路径。结果表明:在冲击态(即初始卸载态)高达219 GPa的压力范围内,无氧铜的等熵卸载过程可用Grüneisen状态方程在ργ=ρ0γ0近似下作很好的描述;各条卸载路径到一个大气压的终态粒子速度US与镜像反演的粒子速度2u的偏差(US-2u)/(2u),随冲击波压力的增加而增大。  相似文献   

12.
A deterministic equation of the Hamilton-Jacobi type is proposed for a single particle:S t+(1/2m)(?S)2+U{S}=0, whereU{S} is a certain operator onS, which has the sense of the potential of the self-generated field of a free particle. Examples are given of potentials that imply instability of uniform rectilinear motion of a free particle and yieldrandom fluctuations of its trajectory. Galilei-invariant turbulence-producing potentials can be constructed using a single universal parameter—Planck's constant. Despite the fact that the classical trajectory concept is retained, the mechanics of the particle then admits quantum-type effects: an uncertainty relation, de Broglie-type waves and their interference, discrete energy levels, and zero-point fluctuations.  相似文献   

13.
Based on planar high-speed Rayleigh scattering measurements of the mixture fraction Z of propane discharging from a turbulent round jet into co-flowing carbon dioxide at nozzle-based Reynolds numbers Re 0 = 3000–8600, we use scalar gradient trajectories to investigate the local structure of the turbulent scalar field with a focus on the scalar turbulent/non-turbulent interface. The latter is located between the fully turbulent part of the jet and the outer flow. Using scalar gradient trajectories, we partition the turbulent scalar field into these three regions according to an approach developed by Mellado et al. (J.P. Mellado, L. Wang, and N. Peters, Gradient trajectory analysis of a scalar field with external intermittency, J. Fluid Mech. 626 (2009), pp. 333–365.). Based on these different regions, we investigate in a next step zonal statistics of the scalar probability density function (pdf) P(Z) as well as the scalar difference along the trajectory ΔZ and its mean scalar value Zm , where the latter two quantities are used to parameterize the scalar profile along gradient trajectories. We show that the scalar pdf P(Z) can be reconstructed from zonal gradient trajectory statistics of the joint pdf P(Zm , ΔZ). Furthermore, on the one hand we relate our results for the scalar turbulent/non-turbulent interface to the findings made in other experimental and numerical studies of the turbulent/non-turbulent interface, and on the other hand discuss them in the context of the flamelet approach and the modelling of pdfs in turbulent non-premixed combustion. Finally, we compare the zonal statistics for P(Z) with the composite model of Effelsberg and Peters (E. Effelsberg and N. Peters, A composite model for the conserved scalar pdf, Combust. Flame 50 (1983), pp. 351–360) and observe a very good qualitative and quantitative agreement.  相似文献   

14.
Near-infrared luminescence is observed from bismuth-doped GeS2-Ga2Sa chalcogenide glasses excited by an 808 nm laser diode. The emission peak with a maximum at about 1260 nm is observed in 80GeS2-2OGa2 Sa:O.fBi glass and it shifts toward the long wavelength with the addition of Bi gradually. The full width of half maximum (FWHM) is about 200 nm. The broadband infrared luminescence of Bi-doped GeS2-Ga2Sa chalcogenide glasses may be predominantly originated from the low valence state of Bi, such as Bi+. Raman scattering is also conducted to claxify the structure of glasses. These Bi-doped GeS2 Ga2Sa chalcogenide glasses can be applied potentially in novel broadband optical fibre amplifiers and broadly tunable laser in optical communication system.  相似文献   

15.
We investigate the plastic deformation and constitutive behaviour of bulk metallic glasses (BMGs). A dimensionless Deborah number DeiD = tr/ti is proposed to characterize the rate effect in BMGs, where tr is the structural relaxing characteristic time of BMGs under shear load, ti is the macroscopic imposed characteristic time of applied stress or the characteristic time of macroscopic deformation. The results demonstrate that the modified free volume model can characterize the strain rate effect in BMGs effectively.  相似文献   

16.
A Particle Resistance Model for Flow through Porous Media   总被引:1,自引:0,他引:1       下载免费PDF全文
A particle model for resistance of flow in isotropic porous media is developed based on the fractal geometry theory and on the drag force flowing around sphere. The proposed model is expressed as a function of porosity, fluid property, particle size, fluid velocity (or Reynolds number) and fractal characters D f of particles in porous media. The model predictions are in good agreement with the experimental data. The validity of the proposed model is thus verified.  相似文献   

17.
The focus of this paper is on the mixing of a conserved passive scalar for Sc = 1 (Sc is the Schmidt number) in axisymmetric turbulence for which the initial injections of turbulent kinetic energy and scalar variance are similar. Two confined-opposed-jets (COJ) are experimentally studied through simultaneous PIV (particle image velocimetry) and PLIF (planar laser induced fluorescence) measurements, for different flow regimes. One-point transport equation for the scalar variance is assessed through experimental data, along the common axis of the two opposed jets, and different physical phenomena are revealed (production, diffusion, dissipation). The production of scalar variance is equilibrated by the diffusion term (~75%) and the mean dissipation of the scalar variance (~25%). To further assess the scalar behaviour at each scale in this anisotropic, but axisymmetric, flow, a scale-by-scale scalar variance budget equation is derived for axisymmetric turbulence. This equation reduces to Yaglom's 4/3 law, under additional restrictions. The equation is assessed through experimental data, in the impingement region between the two COJ. In particular, the anisotropic energy transfer along different directions is quantified. It is shown that for scales smaller than the size of the central region, Δ, the cascade of the scalar variance is completely inhibited, independently of the particular direction. For scales larger than Δ, the apparent aspect of the energy transfer is that of an inverse cascade, with positive values of the scalar variance transfer. Nonetheless, inhomogeneity of the flow and mixing at those scales is directly responsible for these positive values.  相似文献   

18.
在相对论平均场理论(RMFT)框架内,使用GL91参数组结合超核数据和大质量中子星的观测数据限定超子标量耦合参数Xσ=0.59~1.0,用慢转近似计算了大质量中子星和前中子星的转动惯量。当Xσ从0.59增加到1.0,中子星(前中子星)的最大转动惯量增幅达89%(60%)。在同样的变化范围内,用Crab的观测数据,计算得到中子星(前中子星)的最大能量损失(dE/dt)的增幅为44%(25%),最大磁场增幅为48%(38%)。相比于前中子星,中子星的性质对超子参数更为敏感。当Xσ从0.59增加到1.0,PSR J0348+0432的转动惯量和dE/dt的增幅均为14%,而磁场减幅为10%。如果天文观测能够给出中子星转动惯量的上限,或者同时精确测量中子星的质量和转动惯量,能帮助人们进一步限定超子参数。In the framework of the relativistic mean field theory(RMFT) with GL91 cets, the momentum of inertia (I) of slowly rotating neutron stars is studied by perturbative approach. The scalar hyperon coupling should lie in the range of Xσ=0.59~1.0 to be compatible with massive neutron stars. As Xσ increases from 0.59 to 1.0, the maximum momentum of inertia(Imax) of neutron (protoneutron) stars increases by 89% (60%). According to the data of Crab, the maximum energy loss(dE/dt) of neutron (protoneutron) stars will increase by 44%(25%)and the maximum magnetic field (B) will increase by 48%(38%). I and dE/dt of PSR J0348+0432 both increase by 14%, while B decreases by 10% as Xσ increases from 0.59 to 1.0. So if the upper bound of I, or the accurate values of both the mass and I of neutron stars could be provided by the astronomical observations, the hyperon couplings should be further constrained in the future.  相似文献   

19.
The properties of baryons in nuclear matter are analysed in the relativistic mean-field theory(RMF). It is found that the scalar field σ meson affects the properties of baryon at high density. A density dependent scalar coupling gσN is determined according to the idea of quark-meson coupling model and extended to RMF. It is shown that gσN affects the property of nuclear matter weakly at low density, but strongly at high density. The relation between the scalar density ρS and the nuclear density ρ and the effective mass of the pentaquark Θ+ are studied with the density dependent coupling constant. The density dependent scalar coupling obviously affects the effective masses of baryons in nuclear matter, especially at high density.  相似文献   

20.
In this paper the experimental value of radiative correction Δr was derived from the new data of sin 2θw and W boson mass Mw given by LEP,CDF and other collaborations.A careful comparison of (Δr)exp with the standard model expectation was carried out.We first calculated the Δr at full one-loop level,and then the main two-loop contributions were included.More stringent upper bounds on Mt were obtained from the analysis of probability distribution:Mt175GeV at 95%C.L. for a given MH=100GeV.The effects on Nt from other experimental and theoretical errors were also computed.  相似文献   

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