197 resultados para Art 29 (2) Código de Comercio


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试图从以下4个方面对热等离子体材料加工现在以及将来的研究与发展进行评价:(1)热等离子体涂镀技术;(2)热等离子体微细粉末合成;(3)热等离子体处理废物;(4)热等离子体球化及致密化.一般来讲,由于热等离子体加工由大量参数决定,实行控制非常必要.在某些情况下,缺乏足够的控制以及经济方面的一些不利因素是热等离子体技术成长的主要障碍.但是,目前的研究与开发工作正在致力于解决这些问题

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从实验和计算两个角度研究液体金属脆机理。利用第一原理和陈难先三维晶格反演方法获得Al-Ga和Ga-Ga有效对势。运用分子动力学研究液态金属吸附对位错发射的影响。结果表明:液体金属吸附后能促进位错的发射、增殖和运动;当吸附促进位错发射和运动达到临界状态时,脆性微裂纹就在原裂纹顶端或在无位错区中形核并解理扩展。

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2 align="center">目录2>

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Abstract This paper presents a hybrid heuristic{triangle evolution (TE) for global optimization. It is a real coded evolutionary algorithm. As in di®erential evolution (DE), TE targets each individual in current population and attempts to replace it by a new better individual. However, the way of generating new individuals is di®erent. TE generates new individuals in a Nelder- Mead way, while the simplices used in TE is 1 or 2 dimensional. The proposed algorithm is very easy to use and e±cient for global optimization problems with continuous variables. Moreover, it requires only one (explicit) control parameter. Numerical results show that the new algorithm is comparable with DE for low dimensional problems but it outperforms DE for high dimensional problems.

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分析了滑移线延长线与楔面交点附近的流动特点,研究了准定常强激波反射中马赫杆的变形,建立了马赫杆突出变形消失的过渡准则,并用激波极曲线方法进行了求解.对马赫杆的变形过程进行了描述,研究了比热比、马赫数的变化对马赫杆突出变形消失条件的影响,并对突出变形消失区域与终点双马赫反射区域进行了比较.结果表明:马赫杆突出变形的消失是低比热比介质中出现的一种激波反射现象.马赫杆突出变形的消失,导致出现一种新的无射流、直马赫杆的双马赫反射结构.

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组建了一套利用静电探针诊断技术测量减压直流非转移弧等离子体射流速度的实验系统.对以纯氩为工质的等离子体,在气流量1.25×10~(-4) kg/s、弧电流80A、真空室压力165 Pa的条件下,测量了射流的速度及其分布.结果表明射流在发生器出口处中心最高速度约为1 200 m/s,在半径20 mm处减小到635 m/s.沿射流轴线方向的速度梯度约为10 (ms~(-1))/mm.射流速度随着弧电流增加而缓慢单调增加;当真空室压力从165 Pa提高到2 kPa时,发生器出口轴线上的射流速度从1200 m/s降至570 m/s.

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Based on the Coulomb friction model, the frictional motion model of workpiece relating to the polishing pad was presented in annular polishing. By the dynamic analysis software, the model was simulated and analysed. The conclusions from the results were that the workpiece did not rotate steadily. When the angular velocity of ring and the direction were the same as that of the polishing pad, the angular velocity of workpiece hoicked at the beginning and at the later stage were the same as that of the polishing pad before contacting with the ring. The angular velocity of workpiece vibrated at the moment of contacting with the ring. After that the angular velocity of workpiece increased gradually and fluctuated at a given value, while the angular velocity of ring decreased gradually and also fluctuated at a given value. Since the contact between the workpiece and the ring was linear, their linear velocities and directions should be the same. But the angular velocity of workpiece was larger than that of the polishing pad on the condition that the radius of the workpiece was less than that of the ring. This did not agree with the pure translation principle and the workpiece surface could not be flat, either. Consequently, it needed to be controlled with the angular velocity of ring and the radii of the ring and the workpiece, besides friction to make the angular velocity of workpiece equal to that of the polishing pad for obtaining fine surface flatness of the workpiece. Copyright © 2007 Inderscience Enterprises Ltd.}

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采用大功率半导体激光器抽运25m掺Yb双包层光纤,在单程装置中,前向(SPF)和后向(SPB)分别获得了1.46w和1.82w最大超荧光功率,斜度效率分别为23.4%0和292%,3dB带宽最大为11nm。采用特定范围波长双色镜作为前腔镜,形成双程前向(DPF)装置,获得最大超荧光输出功率2.12W,此时斜度效率为43.2%,中心波长在1070nm,输出光谱平坦性较好,3dB带宽从单程的11nm提高到42nm。

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由于放电结构及谐振腔的限制,准分子激光光斑呈现不均的分布。介绍了各种均匀器的工作原理,从衡量光束均匀性的各项指标出发,评述分析了各种均匀方法的优缺点及适用范围。