{"title":"基于光学相干层析成像的产业相关流分析综述","authors":"Antti I. Koponen, Sanna Haavisto","doi":"10.14356/KONA.2020003","DOIUrl":null,"url":null,"abstract":"Fig. 3 c) A closer look at the measurement optics. Here U is the real velocity, v is the component of velocity in the direction of the measurement beam, and nf is the refractive index of the medium. Angle α is obtained by calculating first angle δ by applying the Snell’s law of refraction to the two interfaces. On page 46 the paragraph related to Eq. (3) should be: Fig. 3b shows as an example a measurement setup of pipe flow. From Fig. 3c, we get the real axial velocity in the pipe to be","PeriodicalId":17828,"journal":{"name":"KONA Powder and Particle Journal","volume":null,"pages":null},"PeriodicalIF":2.6000,"publicationDate":"2020-01-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"9","resultStr":"{\"title\":\"Analysis of Industry-Related Flows by Optical Coherence Tomography—A Review\",\"authors\":\"Antti I. Koponen, Sanna Haavisto\",\"doi\":\"10.14356/KONA.2020003\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Fig. 3 c) A closer look at the measurement optics. Here U is the real velocity, v is the component of velocity in the direction of the measurement beam, and nf is the refractive index of the medium. Angle α is obtained by calculating first angle δ by applying the Snell’s law of refraction to the two interfaces. On page 46 the paragraph related to Eq. (3) should be: Fig. 3b shows as an example a measurement setup of pipe flow. From Fig. 3c, we get the real axial velocity in the pipe to be\",\"PeriodicalId\":17828,\"journal\":{\"name\":\"KONA Powder and Particle Journal\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":2.6000,\"publicationDate\":\"2020-01-10\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"9\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"KONA Powder and Particle Journal\",\"FirstCategoryId\":\"88\",\"ListUrlMain\":\"https://doi.org/10.14356/KONA.2020003\",\"RegionNum\":4,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"ENGINEERING, CHEMICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"KONA Powder and Particle Journal","FirstCategoryId":"88","ListUrlMain":"https://doi.org/10.14356/KONA.2020003","RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"ENGINEERING, CHEMICAL","Score":null,"Total":0}
Analysis of Industry-Related Flows by Optical Coherence Tomography—A Review
Fig. 3 c) A closer look at the measurement optics. Here U is the real velocity, v is the component of velocity in the direction of the measurement beam, and nf is the refractive index of the medium. Angle α is obtained by calculating first angle δ by applying the Snell’s law of refraction to the two interfaces. On page 46 the paragraph related to Eq. (3) should be: Fig. 3b shows as an example a measurement setup of pipe flow. From Fig. 3c, we get the real axial velocity in the pipe to be
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KONA publishes papers in the broad field of powder science and technology, ranging from fundamental principles to practical applications. Papers describing technological experience and critical reviews of existing knowledge in special areas are also welcome.
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