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TEST OF AN INSTRUMENTAL IMPLEMENTATION OF AN EDGE-LOSS ERROR CORRECTION SYSTEM

机译:测试边缘损耗纠错系统的乐器实现

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Reflectance measurement data for plastics and other translucent materials (e.g. paper) can be in error due to the lateral diffusion of light within the sample. Illuminating light from the measuring instrument can laterally diffuse to sample areas outside of the area which is viewed by instrument photometric measuring system. Figure 1 illustrates an idealized representation of a 45/0 measuring system in which some of the illuminating light laterally diffuses to areas which are outside the view of the measuring detector. This results in a type of measurement error which the author has characterized as lateral diffusion error (LDE) to note the physical process which causes the error. Elsewhere in the literature it has been described as translucent blurring error, translucency error, edge loss error, and stray darkness. While the example in figure 1 shows a 45/0 measurement configuration, LDE can occur with all measurement configurations (e.g. 0/45, d/8, etc. ). It is caused by the instrument illuminating light diffusing lateral within the sample. Lateral diffusion is present in all non-metallic samples to some extent. A common solution for minimizing LDE is to make the area viewed by the detector larger than the area illuminated by the light source. Thus, in the case of the idealized instrument configuration of figure 1, doubling the area viewed by the detector would allow all of the light reflected directly from the illuminated area and the light that was laterally diffused and emerged from the unilluminated surface to be viewed by the detector. An alternative is to leave the area viewed by the detector untouched and to double the area illuminated by the light source. While this may not intuitively seem equivalent to increasing the area viewed while holding the area illuminated constant, optical reciprocity, as defined by Clark and Perry, indicates that this method should give equivalent error reduction. The exact amount of over-viewing or over-illumination area required to minimize LDE is very dependent on the translucency of the sample being measured. This explains, in part, why instruments used for measuring plastics are general not useful for measuring graphic arts products and vise-versa. Also, ideally all areas of the sample illuminated and viewed should have the same surface and color characteristics. This can present a problem in the color control of graphic arts printing where color control strips are included and take up otherwise marketable product space. As a result, the elements of these color strips are kept very small to minimize unmarketable content. This limits the size and amount of over-illumination or over viewing that can be used to minimize LDE.
机译:由于样品内光的横向扩散,塑料的反射率测量数据和其他半透明材料(例如纸张)可能出错。来自测量仪器的照明光可以横向扩散到由仪器光度测量系统观察的区域外的样本区域。图1示出了45/0测量系统的理想化表示,其中一些照明光横向扩散​​到在测量检测器的视图之外的区域。这导致了作者所表征为横向扩散误差(LDE)的测量误差的类型,以记下导致错误的物理过程。文献中的其他地方被描述为半透明模糊误差,半透明误差,边缘损耗误差和杂散黑暗。虽然图1中的示例显示了45/0测量配置,但所有测量配置都可以发生LDE(例如0/45,D / 8等)。它是由仪器照明光在样品内的横向侧向引起的。在一定程度上,在所有非金属样品中存在横向扩散。用于最小化LDE的常见解决方案是使检测器观察的区域大于光源照射的区域。因此,在图1的理想仪器构造的情况下,通过检测器观察的区域将允许直接从照明区域和横向扩散的光反射的所有光,并从未化的表面上观察探测器。替代方案是将检测器观察的区域未被触摸,并将光源照射的区域加倍。虽然这可能不会直观地相当于增加在保持区域观看的区域,但是由克拉克和佩里所定义的照明恒定,光学互惠表明该方法应该给出等效的误差。最小化LDE所需的确切量的过度观察或过度照明区域非常依赖于测量样本的半透明。这部分解释了为什么用于测量塑料的仪器的仪器通常不用于测量图形艺术产品和虎钳。此外,理想情况下,样品的所有区域都照亮和观察应具有相同的表面和颜色特性。这可能在图形艺术印刷的颜色控制中存在问题,其中包括颜色控制条并占用其他可销售产品空间。结果,这些彩色条带的元件保持非常小以最小化未载数量的内容。这限制了可用于最小化LDE的过度照明或过度观看的大小和数量。

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