A New Model for Microstructure of Liquid Metals

A nanocrystalline model for microstructures of liquid metals is constructed. According to the nanocrystalline model, the intensity curves of x-ray diffraction (XRD) on liquid Cu, A1 and Al65Cu20Fe15 alloy are derived by broadening the XRD peaks of these metals in some crystal structures. These broadening intensity curves are     

磁流体热疗设备的三维电磁场模拟

为清楚了解磁流体热疗设备产生的电磁场的分布,本文采用有限元方法对自制的设备原型建立三维模型并进行了优化,计算了该模型在静态和谐态下产生的电磁场的分布,对磁极中间的气隙宽度在20～40mm范围内变化时的磁场强度进行了对比．选取气隙宽度为30mm时计算电磁场的磁场强度、电感和涡流损耗,所得结果与实验测量值完全吻合,验证了模拟计算的可靠性．     

Astrophysical ~(22)Mg(p,γ)~(23)Al reaction rates from asymptotic normalization coefficient of ~(23)Ne→~(22)Ne+n

The radionuclide ~(22)Na generates the emission of a characteristic 1.275 MeV γ-ray. This is a potential astronomical observable, whose occurrence is suspected in classical novae. The ~(22)Mg(p, γ)~(23)Al reaction is relevant to the nucleosynthesis of ~(22)Na in Ne-rich novae. In this study, employing the adiabatic distorted wave approximation and continuum discretized coupled channel methods, the squared neutron asymptotic normalization coefficients(ANCs)231 for the virtual decay of Ne → ~(22)Ne + n were extracted, and determined as(0.483 ± 0.060) fm~(-1) and(9.7 ± 2.3) fm~(-1) for the ground state and the first excited state from the experimental angular distributions of ~(22)Ne(d, p)~(23)Ne populating the ground state and the first excited state of ~(23)Ne, respectively. Then, the squared proton ANC of ~(23)Al_(g.s.) was obtained as C_(d5/2)~(2)(~(23)Al)(2.65 ± 0.33) × 10~3 fm~(-1) according to the charge symmetry of the strong interaction. The astrophysical S-factors and reaction rates for the direct capture contribution in ~(22)Mg(p, γ)~(23)Al were also presented. Furthermore, the proton width of the first excited state of ~(23)Al was derived to be(57 ± 14) eV from the neutron ANC of its mirror state in ~(23)Ne and used to compute the contribution from the first resonance of ~(23)Al. This result demonstrates that the direct capture dominates the ~(22)Mg(p, γ)~(23)Al reaction at most temperatures of astrophysical relevance for 0.33 T_9 0.64.     

The Kinetic Theory of Growth of Zr-Sn Diffusion Layers on Zr55Cua0Al10Ni5 Metallic Glass

The growth kinetics of the intermetallic compound layer between molten pure Sn and Zr55Cu30AlloNi5 bulk metallic glass （BMG） is mainly controlled by the diffusion mechanism at stage I at which the value of the time exponent is approximately 1/2, also there is unusual or unique stage Ⅱ whose time exponent of the growth is suppressed to 1/3. It is deduced that phase transition such as nucleation, coalescence occurring in the vicinity of the interface of the diffusion layer within the BMG and the average size growing as one-third power of time, called the Lifshitz-Slezov law. A more elegant means of attack is based upon the Fokker-Planck approach, which permits us to calculate directly the probability of the distribution of steady-state thickness fluctuations. Physical implications of the analytical results also give the one-third power of time of distance scale. The transmission of Sn particles through a disorder system of the BMG, scattered by the local fluctuation levels, is the source of the time exponent from 1/2 to 1/3 as a macroscopic cumulative effect.     

Influence of the distance between two voltage contacts on giant magneto-impedance of Co-based amorphous wires

The Co₇₅ Fe_4.2Si₈B₁₂Nb_0.8 amorphous wires of 30 μ m in diameter are produced by melt extraction and annealing at 450 oC for 20 min in vacuum with a longitudinal or transverse field of 40 kA/m. Distances between the two voltage contacts of 6, 5, 4 and 2 mm are obtained by moving the two voltage contacts towards the centre of the sample at the same time. Results indicate that magneto-impedance response is dependent on the distance significantly. As distance decreases from 6 to 2 mm, △Z/Z reduces from 609% to 95% and giant magneto-impedance (GMI) profiles change from two-peak to single-peak. Besides, field sensitivity improves from 0.47%/(A/m) to 0.76%/(A/m) when the single-peak GMI just appears. It is therefore concluded that actual measurements can be made comparable only by taking into account the influence of distance between two voltage contacts for a magneto-impedance measurement.     

肿瘤热疗用交变磁场发生器的研制

装置的磁路部分设计成环回形,磁路中的气隙用于产生高频磁场.在励磁线圈中加入铁氧体磁芯显著增强了装置输出的磁场强度;电路部分采用桥式拓扑结构,因而功率变换效率很高.装置的指标为:频率25～120 kHz,磁场强度6～16 kA/m.对磁场强度的测量表明磁场分布均一.使用该装置加热纳米磁性材料,可使其在室温下升温达28 ℃.这些工作为磁流体肿瘤热疗的临床应用提供了参考.     

聚乙二醇化学改性增韧呋喃树脂的研究

研究了用不同分子量的聚乙二醇(PEG)对呋喃树脂进行改性以改善其脆性较大的缺点.通过化学反应将具有柔性长链结构的聚乙二醇键接到呋喃树脂上从而增加了其韧性.研究结果表明,PEG分子量为400Da时,对呋喃树脂的增韧效果最好;其用量为25wt%时,呋喃树脂的断裂伸长率达到了5.51%,最大拉伸强度可达19.9MPa.