飞行数据可视化回放与分析软件设计

针对原有飞行数据回放软件存在的回放效果不直观、分析效率低、分析结果不规范等情况,提出了一种三维动态可视化飞行数据回放与分析方案,通过对分析判据进行提炼和量化,按照结构化的分析结果模板,实现了分析结果的自动生成与输出;飞行数据可视化回放与分析软件采用成熟技术,经用户在实际飞行任务事后分析中使用,完全满足用户使用要求,飞行数据回放效果更加友好、分析效率更加高效、分析结果更加明了,各方面明显优于原有软件。     

因果图法在仪器分析中的应用

通过分析影响仪器分析质量的5M1E因素,即操作者（Man）,仪器设备（Machine）,分析方法（Method）,分析材料（Material）,管理（Management）,环境（Environment）以及管理（management）,提出建立仪器分析的因果关系图的一般方法,并以原子吸收光谱分析中分析质量的因果关系为例,提出了提高仪器分析质量,减少分析误差的可行性控制措施.分别对因果关系图的绘制,应用和注意问题以及6大因素在仪器分析中的特点及防误措施作了介绍.     

低铝光谱分析技术的开发及应用

研究了影响钢中铝分析的因素,从试样制备、分析曲线的调整以及分析各个环节,进行了分析探讨,总结出低铝分析的特点,对炼钢生产有重要指导作用.     

全反射X荧光分析技术(TRXF)——一种新的高灵敏度元素分析技术

全反射X荧光分析技术,是一种在X 荧光分析技术基础上发展起来的全新的分析技术,其主要特征是通过反射技术去掉在通常X 荧光分析中高能散射本底的影响,提高了分析灵敏度,分析刻度简单,分析样品量少(微克量级),设备简单。于八十年代中期开始出现商品。     

ANSYS在低温压力容器应力分析与优化设计中的应用

介绍了大型有限元软件ANSYS在低温压力容器典型应力分析(不连续区局部应力分析、热应力分析、接触应力分析、复合材料应力分析)与优化设计中的应用,论证了ANSYS作为低温压力容器应力分析与优化设计有效手段的实用性和可靠性,为低温压力容器的应力分析和优化设计找到了一条新途径。     

求诱导含量的一种实用的计算机算法

在直读光谱分析中,当分析高合金钢时,基体元素的含量往往减少到75%以下,这时如果仍旧采用一般的分析方法,则会使分析误差过大。为了提高分析的精度,在分析高合金钢时应采用诱导含量法。求诱导含量必须解多元联立方程组,有多少个分析元素就有多少个联立方程。当分析元素过多时,手工计算很难完成。对于配有计算机的直读光谱仪,这项工作     

分析与综合思维在物理教学中的应用

分析和综合是思维的基本过程,掌握分析与综合思维方法是物理教育的目标之一,考查学生分析与综合能力在高校招生考试中处于重要的地位.本文通过教学案例阐明在教学实践中如何依托教材中不同的教学资源,在概念形成、规律推导、实验探究和习题教学等不同场合、不同情境下全面系统地布局,应用分析与综合的思维方法.实践表明,教师通过教学示范能较好地引导学生养成良好的分析与综合的思维习惯,从而学生也能形成采用分析与综合方法分析问题的意识,提升分析问题、解决问题的能力.     

误差分析知识结构图在普物光学 实验复习教学中的应用

针对大学生在普物光学实验的误差分析中出现的常见错误, 构建了误差分析知识结构图. 对比传统的 实验复习课, 基于误差分析知识结构图的实验复习教学, 能更有效地帮助学生理解误差分析及方法. 误差分析知识 结构图的引入, 为普物光学实验的复习教学提供新的思路     

编写SPnenu安卓软件分析单摆视频计算重力加速度

为了增强"单摆测量重力加速度"实验的效果,编写了运动视频分析安卓应用程序-SPnenu,分析单摆视频,计算重力加速度。首先,介绍了安卓软件的组成模块;然后,使用该应用程序分析单摆运动视频中周期、摆长和视频当地重力加速度;最后,与计算机平台下的视频分析软件Tracker进行对比实验,并对误差进行了讨论分析。实验表明,将基于安卓智能手机的运动视频分析软件引入物理实验教学,有助于打破实验的时间和空间限制,减小了"周期测量"带来的误差,能实现对单摆小球运动轨迹的精确追踪记录和数据分析。     

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基于计算流体动力学(CFD)方法,结合首个完整的模块系统对第一壁以及与其相连接的两个隔板结构进行了热工水力分析,包括压力分析、流速分析、流量分配分析、对流换热系数分析。给出了所有分析的计算结果。同时将数值模拟计算得到的对流换热系数与相关经验公式推导得到的结果进行了比较,基本一致。     

Magnetization and magnetic phase diagrams of a spin-1/2 ferrimagnetic diamond chain at low temperature

We used the Jordan–Wigner transform and the invariant eigenoperator method to study the magnetic phase diagram and the magnetization curve of the spin-1/2 alternating ferrimagnetic diamond chain in an external magnetic field at finite temperature. The magnetization versus external magnetic field curve exhibits a 1/3 magnetization plateau at absolute zero and finite temperatures, and the width of the 1/3 magnetization plateau was modulated by tuning the temperature and the exchange interactions. Three critical magnetic field intensities H_(CB), H_(CE) and H_(CS) were obtained, in which the H_(CB) and H_(CE) correspond to the appearance and disappearance of the 1/3 magnetization plateau, respectively, and the higher H_(CS) correspond to the appearance of fully polarized magnetization plateau of the system. The energies of elementary excitation ωσ,k(σ = 1, 2, 3) present the extrema of zero at the three critical magnetic fields at 0 K, i.e., [hω_(3,k)(HCB)]_(min)= 0, [hω_(2,k)(H_(CE))]_(max)= 0 and [hω _(2,k)(H_(CS))]_(min)= 0, and the magnetic phase diagram of magnetic field versus different exchange interactions at 0 K was established by the above relationships. According to the relationships between the system's magnetization curve at finite temperatures and the critical magnetic field intensities, the magnetic field-temperature phase diagram was drawn. It was observed that if the magnetic phase diagram shows a three-phase critical point, which is intersected by the ferrimagnetic phase, the ferrimagnetic plateau phase, and the Luttinger liquid phase, the disappearance of the1/3 magnetization plateau would inevitably occur. However, the 1/3 magnetization plateau would not disappear without the three-phase critical point. The appearance of the 1/3 magnetization plateau in the low temperature region is the macroscopic manifestations of quantum effect.     

Effect of Dy substitution on magnetic properties and magnetocaloric effects of Tb6Co1.67Si3 compounds

The magnetic and magnetocaloric properties of(Tb1-xDyx) 6 Co 1.67 Si 3(0 ≤ x ≤ 0.8) have been experimentally investigated.The compounds exhibit a Ce6Ni2Si3-type hexagonal structure and undergo a second-order magnetic transition.The Curie temperature decreases from ～ 187 K to 142 K as the content of Dy grows from 0 to 0.8.The maximal magnetic entropy change,for a field change of 0-5 T,varies between ～ 6.2 and ～ 7.4 J/kg.K,slightly decreasing when Dy is introduced.The substitution of Dy leads to a remarkable increase in refrigeration capacity(RC).A large RC value of ～ 626 J/kg is achieved for x = 0.4 under a field change of 0-5 T.     

Giant magnetocaloric effect in Tb5Ge2-xSi2-xMn2x compounds

The crystal structure,magnetic and magnetocaloric characteristics of the pseduo ternary compounds of Tb5Ge2 xSi2 xMn2x(0 ≤ 2x ≤ 0.1) were investigated by x-ray powder diffraction and magnetization measurements.The x-ray powder diffraction results show that all compounds preserve the monoclinic phase as the majority phase and all the synthesized compounds were observed to be ferromagnetic from magnetization measurements.Magnetic phase transitions were interpreted in terms of Landau theory.Maximum isothermal magnetic entropy change value(20.84 J.kg-1.K-1) was found for Tb5Ge1.95Si1.95Mn0.1 at around 123 K in the magnetic field change of 5 T.     

Topology of toroidal helical fields in non-circular cross-sectional tokamaks

The ordinary differential magnetic field line equations are solved numerically; the tokamak magnetic structure is studied on Hefei Tokamak-7 Upgrade （HT-TU） when the equilibrium field with a monotonic q-profile is perturbed by a helical magnetic field. We find that a single mode （m, n） helical perturbation can cause the formation of islands on rational surfaces with q=m/n and q=（m±1,±2,±3,...）/n due to the toroidicity and plasma shape （i.e. elongation and triangularity）, while there are many undestroyed magnetic surfaces called Kolmogorov-Arnold-Moser （KAM） barriers on irrational surfaces. The islands on the same rational surface do not have the same size. When the ratio between the perturbing magnetic field Br（r） and the toroidal magnetic field amplitude Bφ0 is large enough, the magnetic island chains on different rational surfaces will overlap and chaotic orbits appear in the overlapping area, and the magnetic field becomes stochastic. It is remarkable that the stochastic layer appears first in the plasma edge region.     

First-order reversal curves of magnetic recording tapes

The interaction and its variation between magnetic grains in two kinds of magnetic recording tapes are investigated by first-order reversal curves (FORC) and the $\delta M$ method. The composition and microstructure of the samples are characterised by x-ray diffraction and scanning electron microscope. The FORC diagram can provide more accurate information of the interaction and its variation, but the $\delta M$ curves cannot. The positive interaction field and the large variation of the interaction field have opposite effects on the $\delta M$ curve.     

Magnetocrystalline anisotropy and dynamic spin reorientation of half-doped Nd_(0.5)Pr_(0.5)FeO_3 single crystal

The single crystals of Nd_(0.5)Pr_(0.5)FeO_3 were successfully grown by optical floating zone method.Room temperature x-ray diffraction and Laue photograph declared the homogeneity and high quality of the crystal.The significant magnetic anisotropy and multiple magnetic transitions illustrate the complex magnetic structure.At high temperatures(T 66 K),it shows the typical characteristics of Γ_4(G_x,A_y,F_z) state.With the decrease of the temperature,it undergoes a first-order spin reorientation transition from Γ_4(G_x,A_y,F_z) to Γ_2(F_x,C_y,G_z) state in the temperature window of 45-66 K under an applied magnetic field of 0.01 T.As the temperature drops to ～17 K,a new magnetic interaction mechanism works,which results in a further enhancement of magnetization.The T-H phase diagram of Nd_(0.5)Pr_(0.5)FeO_3 single crystal was finally constructed.     

Magnetic properties and magnetocaloric effect in RE55Co30Al10Si5 (RE = Er and Tm) amorphous ribbons

The magnetic and magnetocaloric effects (MCE) of the amorphous $RE_{55}$Co$_{30}$Al$_{10}$Si$_{5}$ ($RE={\rm Er}$ and Tm) ribbons were systematically investigated in this paper. Compounds with $R ={\rm Er}$ and Tm undergo a second-order magnetic phase transition from ferromagnetic (FM) to paramagnetic (PM) around Curie temperature $T_{\rm C} \sim 9.3$ K and 3 K, respectively. For Er$_{55}$Co$_{30}$Al$_{10}$Si$_{5}$ compound, an obvious magnetic hysteresis and thermal hysteresis were observed at low field below 6 K, possibly due to spin-glass behavior. Under the field change of 0 T-5 T, the maximum values of magnetic entropy change ($-\Delta S_{\rm M}^{\rm max}$) reach as high as 15.6 J/kg$\cdot$K and 15.7 J/kg$\cdot$K for Er$_{55}$Co$_{30}$Al$_{10}$Si$_{5}$ and Tm$_{55}$Co$_{30}$Al$_{10}$Si$_{5}$ compounds, corresponding refrigerant capacity (RC) values are estimated as 303 J/kg and 189 J/kg, respectively. The large MCE makes amorphous $RE_{55}$Co$_{30}$Al$_{10}$Si$_{5 }$ ($RE={\rm Er}$ and Tm) alloys become very attractive magnetic refrigeration materials in the low-temperature region.     

磁性材料进展

磁性材料大体上分为两类 :其一为铁磁有序的金属磁性材料 ;其二绝大多数为亚铁磁有序、具有半导体导电性质的非金属磁性材料 .5 0年代以前 ,金属磁性材料占绝对优势 ;5 0年代以后 ,非金属磁性材料发展成为磁性材料的主流 ,除电力工业用的高饱和磁化强度FeSi合金外 ,铁氧体几乎应用于各个领域 .历史似乎按螺旋形的方式发展 ,90年代后 ,金属磁性材料又以新的面貌出现 ,3d (4f,4d ,5d ,5f… )合金与化合物、非晶、纳米微晶磁性材料重领风骚 ,其性能远超越铁氧体 .纳米磁性材料将成为新的功能材料 .文章重点介绍了永磁材料与软磁材料 ,其他如磁记录材料、磁致冷材料、磁致伸缩材料等将作简单介绍 .     

Entanglement of a two-qubit anisotropic Heisenberg XYZ chain in nonuniform magnetic fields with intrinsic decoherence

Taking the intrinsic decoherence effect into account, this paper investigates the entanglement of a two-qubit anisotropic Heisenberg XYZ model in the presence of nonuniform external magnetic fields by employing the concurrence as entanglement measure. It is found that both the intrinsic decoherence and the anisotropy of the system give a significant suppression to the entanglement. Moreover it finds that the initial state of the system plays an important role in the time evolution of the entanglement, which means that the entanglement of the system is independent of the nonuniformity and uniformity of the magnetic field when the system is in the initial state ｜ψ （0）） = ｜00） and [ψ′ （0）） = m ｜01） ＋ n ｜10）, respectively.