共查询到19条相似文献,搜索用时 328 毫秒
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针对用非平行双目视觉系统进行水下拍摄测量时,由于折射所导致的测量误差较大、精度不高的问题,建立了基于折射光路的水下双目视觉系统测量模型,并以Agrawal方法为基础,在已知两摄像机相对位置关系的前提下,对该测量模型参数标定的方法进行了改进。为验证改进的Agrawal方法的可靠性,与Agrawal方法进行水下标定对比实验。结果表明,相较于Agrawal标定算法得到的防水罩法向量这一模型参数,提出的改进算法的结果与真实值更为接近。在此基础上,应用标定后的水下双目视觉系统测量模型对水下靶标标定点间的标准距离进行测量,测量误差平均值为-0.0134 mm,最大误差为0.2073 mm,与空气中双目视觉系统测量精度相当。 相似文献
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对激光在水介质中传输的光学特性进行分析,在此基础上,给出用于水下测量的激光测量系统及测量结果,并对激光在未来海洋探测方面的应用作了展望。 相似文献
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以一个水声被动测量系统的工程项目为平台,介绍与其配套的水下多路水声测量系统的构成、主要电路环节和工作原理。 相似文献
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激光靶测量图象的在线处理与应用 总被引:1,自引:1,他引:0
介绍了图象在线处理系统及其被用于激光靶测量的工作。自行建立了图象处理的自动测量分析系统,研制了适应该系统的图象测量分析的专用软件YANG.EXE。实际测量结果表明,与以前方法比较,本系统测量数据重复性好,实测精度好于以前手工方法,并且可以对靶表面缺陷进行定量测量。已经逐步用于ICF靶与XRL靶的实际测量。 相似文献
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为了准确获取水下运动目标的运动轨迹,提高测量的数据率,提出了一种基于合作目标的激光水下定位方法。通过在被测目标上加装合作目标,利用合作目标的全反射特性,实现了脉冲式激光水下测角与测距的功能。介绍了激光水下定位的方法和系统组成,给出了水下定位的数学模型及测量结果。模拟实验结果表明,该方法具有一定的工程应用价值。最后,结合工程应用,对激光水下定位需要解决的一些实际问题进行了分析。 相似文献
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A new system of sound intensity measurement for impulse field in the room was proposed. This measurement system consists of a repeatable inspiriting sound source and a microphone fixed on a slowly rotating platform, which is equivalent to a circle microphone array composed of many perfectly matched microphones. The test principle was presented and typical application was described. Based upon this system the sound intensity measurement for impulse field in the room was realized. Therefore, not only time but also spatial information of room impulse response can be obtained. 相似文献
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Fundamentals of the direct measurement of sound intensity and practical applications 总被引:1,自引:0,他引:1
Sound intensity is a measure of the magnitude and direction of the flow of sound energy. Developments in sound intensity measurement capabilities in the last quarter century have occurred because of several reasons. The main ones include the derivation of the cross-spectral formulation for sound intensity and developments in digital signal processing. This paper begins with a brief historical introduction of sound intensity measurements. Then elementary theory for sound intensity is presented. A section on sound intensity measurements is then included. The next section of the paper discusses sources of measurement error; the major sources of error are described in some detail. The paper continues with a discussion of the main applications of sound intensity measurements: sound power determination, noise source identification, and transmission loss measurements. The paper concludes with a discussion of ISO and ANSI intensity related standards and relevant references. 相似文献
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利用阻抗管法测量吸声系数是水下吸声材料研制过程中的重要环节,实验测量结果相比理论计算结果更具说服力。然而在待测样品的制备和安装过程中容易引入的系统误差往往被忽略,从而影响实测结果可信度。为了降低系统误差,本文提出缝隙宽、垂直度和光洁度三种可能引入系统误差的因素,搭建传递函数法水下吸声系数测量的有限元模拟实验环境并验证仿真计算算法的正确性,研究相关参量对橡胶吸声系数的影响规律,并给出一定误差下对相关参量的限制要求。所得结论对降低测量误差、提升实测结果可信度具有一定参考价值。 相似文献
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《Journal of sound and vibration》1991,151(2):213-246
Results are presented of an investigation into the sound intensity distribution in a ventilation duct splitter silencer subject to plane waves incident in the axial direction, under conditions of zero flow. A theory is developed which accounts for the generation of nonplane fields at the cross-sectional discontinuities of the duct-silencer-duct system. A local reaction model of the splitter material is employed, and analytical solutions and numerical results are presented for the sound intensity distribution within the silencer. Experiments were conducted to measure the distribution of sound intensity in a silencer subject to incident plane waves. The conventional cross-spectral method of measuring sound intensity could not be used because of the practical difficulties in manoeuvring the two-microphone assembly through the narrow air passage and obtaining measurements at positions close to the wall of the splitters. Instead, a modified cross-spectral method was devised which employs only one microphone for measurement. In this method, the transfer functions between the loudspeaker input signal and the microphone output signal were measured at an array of microphone positions within the air passages of the silencer. The divergence equation for sound intensity was employed to infer transverse intensity distributions from the computed axial distribution. Reasonable qualitative agreement is obtained between theoretical and observed sound intensity distribution, but the local reaction model of the splitter is found not to be satisfactory at the lower frequencies. 相似文献
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Auditory functional magnetic resonance imaging (fMRI) requires quantification of sound stimuli in the magnetic environment and adequate isolation of background noise. We report the development of two novel sound measurement systems that accurately measure the sound intensity inside the ear, which can simultaneously provide the similar or greater amount of scanner- noise protection than ear-muffs. First, we placed a 2.6 x 2.6-mm microphone in an insert phone that was connected to a headphone [microphone-integrated, foam-tipped insert-phone with a headphone (MIHP)]. This attenuated scanner noise by 37.8+/-4.6 dB, a level better than the reference amount obtained using earmuffs. The nonmetallic optical microphone was integrated with a headphone [optical microphone in a headphone (OMHP)] and it effectively detected the change of sound intensity caused by variable compression on the cushions of the headphone. Wearing the OMHP reduced the noise by 28.5+/-5.9 dB and did not affect echoplanar magnetic resonance images. We also performed an auditory fMRI study using the MIHP system and presented increase in the auditory cortical activation following 10-dB increment in the intensity of sound stimulation. These two newly developed sound measurement systems successfully achieved the accurate quantification of sound stimuli with maintaining the similar level of noise protection of wearing earmuffs in the auditory fMRI experiment. 相似文献
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为了探究超声搅拌磁流变抛光液的制备及优化工艺,利用多物理场数值计算方法,建立了超声搅拌磁流变抛光液的声场仿真模型,并进行了频域分析。研究了不同液位深度、超声变幅杆探入深度,不同功率下磁流变抛光液的声场分布。通过测量磁流变抛光液的声场强度对声场仿真进行了验证。结果表明:随着距变幅杆距离的增加,声强逐渐减弱,高声强区域主要分布在换能器轴线附近。声强在距变幅杆20mm范围内急剧衰减,变幅杆最佳探入深度为10mm,增大功率有助于空化区域的扩大。声场仿真结果与实验测量结果基本一致,对磁流变抛光液的制备提供了数值计算基础。 相似文献
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水下声场的时间积分声强和峰值声强是声呐检测中的重要物理量,而海洋中的内波等动力学过程会造成声场强度的起伏。对南海北部浅海内波环境下定点声起伏实验数据分析,结合数值仿真,总结了试验海域近海底发射和近海底接收条件下内波引起接收信号强度起伏的统计特性.分析结果表明:接收信号的时间积分声强起伏小于峰值声强起伏;时间积分声强与峰值声强起伏的概率分布与对数正态分布较为接近.时间积分声强和峰值声强起伏大小与信号的频率有关,同一收发距离,中心频率650 Hz信号的声强起伏较中心频率310 Hz和375 Hz信号的声强起伏更为剧烈。对于同一频率,当海底较平坦时,声强起伏的闪烁指数随传播距离的增加而增大;当水深随传播距离逐渐变深时,声强起伏规律受内波和水深变化共同影响而更为复杂,闪烁指数先随传播距离增加而增大,之后又随传播距离的增加而逐渐变小. 相似文献