共查询到17条相似文献,搜索用时 156 毫秒
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通过数值计算模拟了激光诱导充压柱壳的热力破坏效应,研究了典型结构的动态爆裂过程,获得的破坏模式与实验结果基本一致。给出了三类典型破坏模式及其对应的参数范围,探讨了各类破坏模式的形成机理,并分析了不同光斑尺寸、壳体厚度条件下热软化效应对破坏内压阈值的影响,以及预内压与破坏时间的关系。研究结果表明:光斑半径越大、热软化程度越高,柱壳的破坏内压阈值越低,且破坏内压阈值随着壳体厚度的减小呈线性下降;给定激光参数和壳体参数下破坏时间随预充内压增大而减小并呈二次函数关系。给出了一种通过热软化程度预估激光诱导充压柱壳破坏时间的方法。 相似文献
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采用有限元计算方法对激光辐照下转动充压壳体的热力学问题进行了较为全面的数值计算,获得了激光辐照下转动内压圆柱壳壁上的温升、应力、应变、位移分布等物理图像,为进一步分析转动充压圆柱壳体在激光辐照下的破坏与失效奠定了基础。提出的解决数值计算中移动热流载荷问题的双时间步长法,可以有效提高计算效率,同时提高计算精度。研究结果表明:对于给定的壳体结构,其损伤阈值时间主要取决于靶面激光强度与壳体旋转频率;在辐照过程中,损伤最先出现在最初受激光辐照的区域。 相似文献
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强激光加热旋转薄柱壳的参量选择分析 总被引:1,自引:0,他引:1
为了把激光加热静止圆柱壳的实验测量结果应用到旋转圆柱壳的激光参量估计中,研究了旋转圆柱壳的激光加热效率。用积分变换法得到了旋转圆柱壳的温度分布,分析了最大温升点相对激光峰值强度点的滞后现象。基于静止圆柱壳和薄壳假设,导出了旋转圆柱壳激光加热效率及估计辐照时间的表达式。对于旋转金属圆柱壳,最大温升点相对激光峰值强度点的滞后角和激光加热效率取决于无量纲参量DR(柱壳半径R与束斑半径r0之比)、DL(横向热扩散尺度4ατL与束斑半径r0之比)及DM(加热时间τL与柱壳旋转频率fR的乘积)。达到相同的最大温升时,旋转圆柱壳的激光辐照时间和静止圆柱壳的激光辐照时间之间存在与激光功率无关的非线性关系,而激光功率决定了所需的绝对激光辐照时间。 相似文献
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基于ANSYS有限元软件, 按有无内压作用, 分别对激光辐照下燃烧室壳体的温度场、热应力、应变与损伤进行了计算与分析.分析表明, 壳体的温度场分布与光束的功率分布一致, 光斑中心温度最高.壳体中应力最大值不在光斑中心, 而是位于光斑边缘处, 在壳体吸收的激光功率密度超过1 000 W/cm2时, 壳体中应力大于材料的强度极限, 壳体均会发生软化.在存在内部燃气压力的情况下, 壳体应力会产生局部集中, 沿壳体环向表面通过光斑中心中轴线区域很有可能裂口;相比较无内压的壳体, 存在内压的壳体中的应力和产生的形变均大于无内压时的壳体.因此, 为达到相同的毁伤效果, 在存在内压的情况下, 可以适当的降低激光的辐照强度. 相似文献
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重离子冷却存储环中的束流是高密度的等离子体,这样的束流照射物体将得到超高压强.如果高功率激光照射束流,将产生实验室中从来没有过的超高温度.这些极端的条件为开辟重离子物理研家新领域提供了可能性.在存储环中使用X射线激光可以测显类锂离子的电荷均方根半径绝对值,使核基态性质的研究将有突破性的进展.它开辟了在等离子体物理、金属物理、核物理和天体物理等领域新的实验条件.为惯性聚变的快速点火创造了最好条件. In cooling storage ring heavy ion beam is plasma of high density. when a big power laser interacted on it, it will get ultra-high temperature. This beam irradiated on an object will get ultra-high pressure. This high energy pulse laser can produce X-ray laser. In the cooling storage ring absolute value of charge mean root radius of Lithium-like nuclei will be measured by the X-ray laser. It will be broken through in investigating the property of nuclear ground state. That will create many... 相似文献
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A. N. Baranov T. V. Bukreeva I. V. Marchenko G. S. Plotnikov A. M. Saletsky 《Moscow University Physics Bulletin》2011,66(5):427-431
Polyelectrolyte capsules with molecules of fluorescein isotiocyanate included in the shell have been obtained. The inclusion
of dye molecules in the shell of the capsule allows the photosensibilized destruction of its structure. The measurements of
the fluorescence intensity of a dye that was present in the shell revealed effective dissipation of the energy of photoexcited
molecules by the surrounding organic matrix. The capsule suspension was irradiated by a laser in the absorption band of fluorescein
isotiocyanate molecules. By measuring the size distribution of the capsules before and after irradiation with a laser it was
shown that the capsules are destroyed under the effect of laser radiation. 相似文献
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Y.H. Wang W.J. Duan Z.L. Wu D. Zheng X.W. Zhou B.Y. Zhou L.J. Dai Y.S. Wang 《Journal of luminescence》2012,132(8):1885-1889
ZnO nanorod arrays were grown on quartz slices in the aqueous solution of zinc acetate and hexamethylenetetramine at 90 °C. Then ZnO:Mg shells were epitaxially grown on the nanorods to form core/shell structures in the aqueous solution of zinc acetate, magnesium acetate and hexamethylenetetramine at the same temperature. Effects of the shells and UV laser beam irradiation on the crystal structure and photoluminescence properties of ZnO nanorods were studied. ZnO:Mg shells suppress the green emission and enhance the UV emission intensity of the nanorods by 38 times. Enhancement of the UV emission depends on the Mg content in the shells. Short time UV laser beam irradiation could improve ZnO nanorod emission efficiently. The UV emission intensity of ZnO nanorods is enhanced by 71 times by capping and subsequent UV laser beam irradiation. 相似文献