测量效果: 立体(3D3C)
产地类别: 进口
测量频率: 低频
测速范围: 0-2000m/s
测定准确度: 1%
测量区域大小: 170mm x 110mm x 100mm
看了粒子图像测速仪(PIV)的用户又看了
FlowMaster®-Tomo层析PIV(Tomo-PIV)是一种全新的三维速度场测量技术。颗粒的速度信息是
由在顺序两次曝光时刻重构出来的粒子三维图像的互相关处理得到的。通过全数字化过程,该技术可以在颗粒浓度相对很高的情况下获得高分辨率速度场,而3D粒子跟踪测速仅能适用于颗粒浓度较低的情况(从而得到的速度矢量场的空间分辨率也很低)。这种方法获得的是完全空间体积内的瞬时结果,与平面PIV扫描式工作不同,它很适合需要双曝光间隔dt很小的高速流动以及利用高帧率相机进行高时间分辨率进行测量的情况。
应用领域:
湍流研究
三维流体结构的可视化
完整的三维漩涡分析
流体结构的相互作用
在测量体内的示踪颗粒由高能量的脉冲激光光源照亮,其散射光由4个不同方向拍摄的CCD相机记录下来,然后由三维空间中每一点光强的分布,利用层析重构算法(MART)对三维空间颗粒的分布进行重构。给定的三维诊断区域中颗粒的位移是通过双曝光形成的两个重构颗粒图像进行三维互相
关获得的,其中利用了变形立体网格的多重网格迭代算法以及LaVision公司独创专利的空间体积自标定技术。
德国LaVision PIV/PLIF粒子成像测速场仪
型号:FlowMaster® 150万 - 200万显微粒子成像测速系统(Micro PIV)
型号:FlowMaster®-Micro 80万 - 100万水下粒子成像测速系统(Under Water PIV)
型号:FlowMaster®-UW 200万 - 300万热线风速仪CTA/HWA
型号:IHW-100 10万 - 30万湍流本质上具有三维(3D)立体结构属性。普通的二维(2D)包 括采用激光照明的成像测量无法在所有三个空间维度上分辨湍流 的结构。而利用多视角成像信息,采用层析重构技术则可以在三 个空间维度上同时捕捉记录复杂流动的瞬态结构。应用针对体像 素的三维(3D)相关处理技术,可以由时间相关的体成像数据计 算出瞬态三维空间的流场。 LaVision功能强大的,基于层析粒子成像测速(Tomo-PIV)和层 析粒子跟踪测速(Tomo-PTV)技术的FlowMaster激光成像系统, 能够以极高的空间分辨率记录强湍流,火焰以及喷雾对象的瞬态 体视流场。
Two-dimensional velocity fields around a freely swimming freshwater black shark fish in longitudinal (XZ) plane and transverse (YZ) plane are measured using digital particle image velocimetry (DPIV). By transferring momentum to the fluid, fishes generate thrust. Thrust is generated not only by its caudal fin, but also using pectoral and anal fins, the contribution of which depends on the fish’s morphology and swimming movements. These fins also act as roll and pitch stabilizers for the swimming fish. In this paper, studies are performed on the flow induced by fins of freely swimming undulatory carangiform swimming fish (freshwater black shark, L = 26 cm) by an experimental hydrodynamic approach based on quantitative flow visualization technique. We used 2D PIV to visualize water flow pattern in the wake of the caudal, pectoral and anal fins of swimming fish at a speed of 0.5–1.5 times of body length per second.
Single-shot, tomographic imaging of the three-dimensional concentration field is demonstrated in a turbulent gaseous free jet in co-flow using volumetrically illuminated laser-induced fluorescence. The fourthharmonic output of an Nd:YAG laser at 266 nm is formed into a collimated 15 × 20 mm2 beam to excite the ground singlet state of acetone seeded into the central jet. Subsequent fluorescence is collected along eight lines of sight for tomographic reconstruction using a combination of stereoscopes optically coupled to four two-stage intensified CMOS cameras. The performance of the imaging system is evaluated and shown to be sufficient for recording instantaneous three-dimensional features with high signal-tonoise (130:1) and nominal spatial resolution of 0.6–1.5 mm at x/D = 7–15.5.
LaVision GmbH粒子图像测速FlowMaster®-Tomo的工作原理介绍
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