基于Proteus的IC总线技术仿真

研究了IC总线的硬件连接和数据传输协议，设计了一款有3个IC存储器的仿真电路，主控制器采用单片机，控制程序采用汇编语言编写.Proteus软件仿真测试表明，结果正确.     

Computational analysis of dense gas shock tube flow

Nonclassical phenomena associated with the classical dynamics of real gases in a conventional shock tube are studied. A TVD predictor-corrector (TVD-MacCormack) scheme with reflective endwall boundary conditions is used for the one-dimensional Euler equations to simulate the evolution of the wave field of a van der Waals gas. Depending upon the initial conditions of the gas, wave fields are produced that contain nonclassical phenomena such as expansion shocks, composite waves, splitting shocks, etc. In addition, the interactions of waves reflected from the endwalls produce both classical and nonclassical phenomena. Wave field evolution is depicted using plots of the flow variables at specific times and withx-t diagrams.     

如何快速制得大量甲烷

本文对教材中的甲烷制取演示实验,从改进装置着手,对温度、药品的配比及用量进行了研究,取得了较好的效果,可快速、大量地制取甲烷。     

一种新型多元素X射线荧光分析仪的研制

新研制的一种用于建材的新型多元素Ｘ射线荧光分析仪与传统的技术方案不同，采用了小功率Ｘ光管激发，薄铍窗正比计数管探测，在低号元素Ａｌ、Ｓｉ的测量方面，具有特色。并简要介绍了仪器的工作原理、组成、技术指标及工业应用效果。     

内爆炸加载条件下圆筒的膨胀、破裂规律研究

以经典热粘塑性本构关系 (John Cook本构关系和Powerlaw本构关系 )为基础 ,建立了更适当表征材料特征的新的、解耦的本构关系。采用SHPB(分离式霍普金森杆 )技术测定了常用弹箭材料 35CrMnSiA的不同应变率下的应力、应变关系 ,并采用拟合的方法确定了本构方程中的材料常数。与高速摄影技术测得的径向位移函数及圆筒材料的损伤演化方程相结合 ,建立了控制内爆炸加载圆筒膨胀 ,直至破裂的完备方程组 ,完成了内爆炸加载圆筒问题的数值模拟 ,计算结果与以往有关箭弹材料圆筒膨胀的实验结果符合较好。     

电热双金属复合管热传导的数值分析

导出变物性下电热复合管热传导的离散近似方程式，源项采用切线方案予以局部线性化．结合一个典型实例计算，指出此类实验件的固有热特点，以及外壁温、总电流、内径测量偏差与内壁温、电功率计算值之间的数值联系．对比解析解和传热实验数据，表明数值分析是可靠有效的．本文为这一构思新颖的电传热实验件工作参数和结构尺寸的设定提供了方法和依据．     

用水冷管热流法测定固态电渣导热系数

提出了改进前人所提出的测定含CaF_2固态渣导热系数的方法,通过测定有渣壳和无渣壳的铜-氧化铝水冷套管中热流值,即可求出渣壳的导热系数,测定了ANF—6(70％CaF_2—30％Al_2O_3)与L_4(15％CaF_2—50％Al_2O_3—30％CaO—5％MgO)渣的导热系数,其温度范围分别为637～1273℃及760～1188℃,其导热系数均随温度升高而增大,并求出了两种渣导热系数与温度的关系式,在1000℃下L_4渣的导热系数较ANF-6渣少50％,此法简便可靠。     

行波管放大器中辐射场的极限环振荡和混沌

以行波管放大器中辐射场的非线性不稳定阈值分析为基础，对辐射场从频率分叉到混沌的演化过程和不同区域这些非线性不稳定态的时间特性和频率特性进行了研究.在“软”非线性区域，辐射场表现为极限环振荡和频率分岔，频谱是离散的且相对于载波频率是不对称的.这种不稳定是阵发性的，适当的调节控制参量，可使器件工作在所需的定态或极限环振荡态上；在“硬”非线性区域，辐射场表现为非周期的随机振荡和频率混沌，频谱连续且频带很宽，场幅值较大的成分集中在接近于零频的低频范围里.这种不稳定是连续性的，不能通过调节参量来消除. 关键词： 行波管 辐射场 分岔 极限环 混沌     

Determination of the field dependence of the intergranular critical current in a YBCO tube by horizontal traversals

The magnetic flux density in the cavity of a sintered tube of Yttrium Barium Copper Oxide (YBCO) is measured as a function of H, the axial magnetic field impressed and removed after zero field cooling (ZFC). We note that, in a short thick-walled hollow cylinder of a weak-linked polycrystalline high-T_c superconductor, the magnetic field in the cavity of the tube, H_z hole, rises above the applied field H when it is initially increasing. Consequently the standard approach to determine the critical current density from an ascending sweep of H alone, or a descending sweep alone cannot be exploited. However the field dependence of the intergranular critical current density J_cm can be reliably obtained from the horizontal traversals of H_z hole vs H. Comparison of the experimental data with model calculations for the horizontal traversals of the hysteresis curves show that the intergranular critical current density in the YBCO tube has a Kim-like field dependence. The magnetization of the grains has a significant influence on the flux density in the cavity of the tube.     

The onset of flow-rate limitation and flow-induced oscillations in collapsible tubes

Experiments were mounted to investigate the onset in a ‘Starling resistor’ of collapsible-tube oscillation, at the lowest possible Reynolds number so as to facilitate matched numerical simulations. The protocol adopted was to set pressure outside the tube and inside the tube at the upstream end, constant and equal to each other, then to progressively lower the downstream pressure past the point of tube collapse and, when this occurred, of oscillation onset. The working fluid was a glycerine/water mixture, and the silicone-rubber tube was suspended horizontally in air. Measurements were made of pressures and flow-rates and of the cross-sectional area at the approximate location of maximum oscillation; separately, the cross-sectional area of the tube in relation to transmural pressure was measured. Parameters varied in the flow experiments were the length of rigid pipe downstream of the collapsing tube, and the fluid viscosity. The pressure/flow-rate coordinates of both the point of peak flow-rate achieved before flow-rate limitation, and the point of oscillation onset, were satisfactorily independent of the pipe length downstream. Both points occurred at flow-rates that decreased with increasing fluid viscosity, so that the corresponding Reynolds numbers decreased more so. Oscillation did not break out below a Reynolds number of about 290 unless there was external mechanical agitation of the apparatus. The amplitude of oscillation decreased progressively towards zero at this point as viscosity was raised. After the flow-rate peak, flow limitation causes a local flow-rate minimum. When oscillation occurred, it started just before this minimum, and died away at the minimum.