共查询到18条相似文献,搜索用时 171 毫秒
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为研究微烧蚀状态下圆形光斑斜入射时激光超声声场的指向性,使用脉冲激光辐照半圆柱形铝质工件表面,并使用压电探头和电磁超声探头分别接收纵波和横波信号。根据速度参数确定了超声信号的类型,提取了信号的峰-峰值,并绘制出声场指向性曲线。通过分析获得以下结论:激光斜入射角度在0~60°范围内变化时,纵波声场的声束轴线方向保持不变,且与工件内法线平行;另外,横波声场的峰-峰值仍然在±35°的方向上取最大值,但是横波指向图形的主瓣易受激光入射方向的影响,当倾斜角度大于等于45°时,横波主瓣的范围变得较宽。 相似文献
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通过实验研究了声束偏转不同角度和声场半径变化时线性相控阵的声场特性,并与基于瞬态波位移解析解的相控阵声场计算方法得到的理论结果进行了对比。首先研究了基于半圆圆弧离面瞬态位移的声场计算方法,并进行了数值计算可靠性的优化。然后建立了一套相控阵瞬态波位移场的测量系统,以半圆形钢板为试件,纵波传感器为接收传感器,测量了偏转角度为-10°,-30°,-50°,-70°,及声场半径为50 mm,75 mm,100 mm和125 mm时线性超声相控阵的声束指向性;同时以基于瞬态波位移解析解的相控阵声场计算方法,计算了相同条件下该相控阵的声束指向性。最后将实验结果与理论结果进行了对比,取得了较好的一致。说明基于瞬态波位移的相控阵声场计算方法可以较好地计算线阵的声场,对于声束偏转较大角度和声场半径变化时也同样有效。 相似文献
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在忽略尺寸激光激励下的超声回波路径分析的基础上,通过设置不同直径的光源对不同厚度的1060铝合金平板进行激励,并在对侧接收信号,获取各次回波达到时间和幅值,用于分析不同尺寸光源激励下的激光超声各次回波传播路径及声场指向性规律。结果显示,在波形混叠处,纵波被淹没在横波内,到达时间难以提取,而横波的到达时间会向前移,偏离理论到达时间,若忽略波形混叠的影响,给出的各次回波到达时间扩展公式的理论值与实验值之间的最大误差不超过0.1μs;通过分析幅值分布情况可以看出,直径≤0.1 mm的激励源可以产生指向性较好的横波声场,而增大激励源直径,纵波声场指向性变好,横波幅值逐渐向法线方向移动,但当直径增加到一定程度,两者声场都会受到热弹效应的影响而向两边扩散。研究结果表明,在实际应用中可针对不同的检测需求选择合适的光源直径。 相似文献
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充水有限长圆柱薄壳声散射:Ⅰ.理论 总被引:2,自引:0,他引:2
研究水中充水有限长圆柱薄壳的声散射。采用弹性薄壳理论结合边界条件导出了有限长圆柱薄壳倾斜入射时散射声场的解析解,内部充水的作用反映在系统总阻抗中增加了内部流体阻抗。数值计算表明,在反向散射声场中,刚性散射部分仅在正横附近有比较大的贡献,而斜入射时起主要作用的是弹性散射部分。散射波相速度频散曲线的计算表明,与内部真空的情况相比内部充水后除正横附近的纵波和剪切波以外,增加了一组内部流体引起的附加波,其对散射声场贡献非常重要。在计算的频率-角度谱图中,内部流体附加波呈现"碗"形共振曲线。 相似文献
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引入四维波矢的概念,推导出弹性波斜入射到多层介质系统时的转移矩阵以及透射系数和反射系数。利用这些公式计算了纵波和横波正入射到一维掺杂声子晶体时纵波和横波的透射系数。得出:当纵波正入射时,透射波中纵波在一定频率范围内出现了禁带,并且在禁带的中心频率处出现了缺陷模。当横波正入射时也有相同的结果。 相似文献
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针对激光对熔石英材料产生致燃损伤过程中存在的激光支持燃烧波,考虑激光作用的温度残余、目标形貌的改变、喷溅物质分布、目标表面气流状况的分布等效应,分阶段对激光支持燃烧波的过程进行建模和仿真研究.通过建立二维轴对称气体动力学模型,模拟研究包含逆韧致辐射、热辐射、热传导和对流过程在内的激光能量传输过程.此外,依据激光支持燃烧波在可见光波段具有明显的辐射特征这一特点,利用阴影法测量了激光对熔石英致燃损伤过程中的燃烧波扩展速度,得到了燃烧波演化过程图像.研究结果表明:在平行激光束作用下,燃烧波的传播是稳态的,气体动力学行为比较稳定;在聚焦激光束作用下,燃烧波的传播是非稳态的.模拟结果中得到的激光支持燃烧波扩展速度及气体动力学结构与实验结果和理论推导结果符合得很好,验证了理论模型的正确性. 相似文献
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Y. Z. Wang L. Liu X. Z. Chen X. J. Wang S. W. Fang W. Q. Cai S. Y. Zhou Y. S. Liu 《Applied physics. B, Lasers and optics》1994,58(4):327-331
This paper reports an experimental study on the collimation and decollimation of an atomic beam in a misaligned standing wave, in which the effective detuning caused by the Doppler effect is affected by the longitudinal velocity of the atomic beam. The experiment shows that in a strong field with red detuning between laser field and atomic transition frequency, laser heating in a normal standing wave becomes laser cooling in a misaligned standing wave for an approriate misalignment angle. For blue detuning, laser cooling in a standing wave can also become laser heating in a misaligned standing wave for an appropriate condition. These results ca be used in controling atomic motion. 相似文献
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基于半经典理论,建立了中性原子与激光驻波场相互作用的模型,分析了中性原子在激光驻波场沟道效应作用下运动轨迹及沉积特性,探讨了球差、色差和原子束发散角对沉积条纹的影响. 得到了上述三种影响因素下纳米光栅的半高宽分别为0.532,12.16,96.70 nm. 仿真结果表明,随着原子束发散角度的增加,沉积条纹的对比度将会下降,当原子束发散角分别为0.1 mard时,其对比度为85.2:1,发散角为0.3 mrad时,条纹对比度为5.33:1,而当发散角增加至0.5 mrad以上时,沉积条纹将会出现分裂现象,导致条纹的恶化.
关键词:
激光驻波场
纳米光栅
沟道效应 相似文献
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The far field of surface mounted elastic wave transducers, as used in Non-Destructive Testing (NDT), is analyzed in order to understand the mechanisms that determine the directivity of these devices. To model the physical configuration, a moving distribution of normal traction, acting at the free surface of an elastic half-space, is used. The exact field expression consists of a spatial superposition of the elementary waves emitted by the hypothetical point sources that make up the finite source. The current aim is to derive approximate far field expressions that are physically instructive and numerically fast. This is achieved through a paraxial approximation of the elementary waves and a Taylor approximation of their arrival times. The approximate expressions thus obtained, consist of a time convolution of a paraxial wave and a transfer function. The latter represents the influence of the source geometry. Besides elucidating the mechanisms of directivity, the analysis renders a rule of thumb for synthesizing a source with a desired directivity pattern. Numerical experiments show that the approximations reduce the computational effort by a factor of 1000, and that the accuracy of the approximate far field and directivity proves excellent at distances beyond a few times the characteristic source size. 相似文献
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WU Di LI Mingxuan WANG Xiaomin CHENG Yue 《声学学报:英文版》2007,26(1):85-96
The field of horizontally polarized ultrasonic shear wave radiated by a 2/2 piezoelectric composite normal probe was studied. The strictly analytic field solutions for two different surface forces were deduced and the field distribution and directivity patterns were given by numerical calculations. The vertical radiated field of shear wave was obtained theoretically and compared with experiment. The experimental result of directivity pattern conformed the theoretical prediction, which provided the theoretical basis for the engineering application of the transducer. 相似文献
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通过建立微波激励下的非对称条形多铁纳磁体的微磁模型,研究了倾斜角和缺陷角对该形纳磁体的铁磁共振谱和自旋波模式的影响.通过对微磁仿真得到的动态磁化数据进行分析发现,非对称条形纳磁体倾斜角度增加,铁磁共振频率随之增加,而这一现象与纳磁体的缺陷角度无关.倾斜角不变,非对称条形纳磁体的铁磁共振频率与缺陷角度呈单调递增关系,并且不同缺陷角度纳磁体的自旋波模式显示出极大的差异.非对称条形纳磁体与矩形纳磁体相比,它的自旋波模式局部化,具体为非对称条形纳磁体的自旋波模式不对称且高进动区域存在于边缘,表现为非对称边缘模式.倾斜角改变导致纳磁体内部退磁场变化,引起纳磁体边缘模式的移动,而中心模式对倾斜角的变化并不敏感.最后,对建立的模型在高频微波磁场激励下的磁损耗进行了分析,验证了模型的可靠性.这些结论说明缺陷角和倾斜角可用于纳磁体自旋波模式和铁磁共振频率的调谐,所得结果为可调纳磁微波器件的设计提供了重要的理论依据和思路. 相似文献
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This paper examines the sound insulation of a single-leaf wall driven by a spherical wave. The transmitted sound field of an infinite elastic plate under a spherical wave incidence is theoretically analyzed and insulation mechanisms are considered. The displacement of the plate is formulated using the Hankel transform in wavenumber space and the transmitted sound pressure in the far-field is obtained by Rayleigh’s formula in an explicit closed form. Moreover, a reduction index is also derived in a closed form by introducing an approximation into the vibration characteristics of the plate. Deterioration of the insulation performance under the spherical wave incidence is caused by an apparent decrease of wall impedance that depends on the directivity of the transmitted sound wave. The mass law for a spherical wave incidence is different from that for a normal plane wave incidence: doubling the weight of the wall or the frequency gives an increase of 3 dB (c.f. 6 dB for a normal plane wave incidence), which is also smaller than the field incidence mass law. 相似文献