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Journal articles on the topic 'Turbid materials'

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Author: Grafiati

Published: 10 March 2023

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1

van Putten, E. G., A. Lagendijk, and A. P. Mosk. "Optimal concentration of light in turbid materials." Journal of the Optical Society of America B 28, no. 5 (April 21, 2011): 1200. http://dx.doi.org/10.1364/josab.28.001200.

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2

Tualle, J. M., E. Tinet, J. Prat, and S. Avrillier. "Light propagation near turbid–turbid planar interfaces." Optics Communications 183, no. 5-6 (September 2000): 337–46. http://dx.doi.org/10.1016/s0030-4018(00)00880-4.

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3

Matousek, P., C. Conti, M. Realini, and C. Colombo. "Micro-scale spatially offset Raman spectroscopy for non-invasive subsurface analysis of turbid materials." Analyst 141, no. 3 (2016): 731–39. http://dx.doi.org/10.1039/c5an02129d.

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4

Schmitt, J. M., and G. Kumar. "Spectral Distortions in Near-Infrared Spectroscopy of Turbid Materials." Applied Spectroscopy 50, no. 8 (August 1996): 1066–73. http://dx.doi.org/10.1366/0003702963905295.

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A liquid suspension consisting of a mixture of H2O, D2O, and polystyrene latex microspheres was used to study the effects of multiple scattering on the near-infrared (800–1600 nm) spectrum of a pure absorber (H2O) in a turbid medium. This simple experimental model enabled us to isolate and explain the spectral distortions introduced by variations in the optical pathlength of scattered photons. We observe the following: (1) Reflectance spectra measured with the detector positioned close to and far from the point of illumination have distinctly different sensitivities to background scattering variations. Within a certain range of detector positions, the use of spectral derivatives to correct for multiplicative scattering effects is most effective. (2) The wavelength dependence of the scattering background of the log(1/ R) spectrum depends not only on particle size but also on the separation between the source and detector probes. And (3) the ratio of the magnitudes of the spectral peaks caused by absorption within the background medium and absorption within the scattering particles decreases as multiple scattering increases. We explain these observations in the context of photon-diffusion theory and point out their significance with respect to the design of diffuse-reflectance spectrometers. Photon diffusion theory proves to be valuable for interpretation of diffuse spectra, but it fails to account for spectral distortions introduced by low-order backscattering at close source–detector separations.

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5

Bolt, René A., and Jaap J. ten Bosch. "On the determination of optical parameters for turbid materials." Waves in Random Media 4, no. 3 (July 1994): 233–42. http://dx.doi.org/10.1088/0959-7174/4/3/002.

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6

Kim, Choong-Jae, Yun-Ho Jung, Chi-Yong Ahn, Young-Ki Lee, and Hee-Mock Oh. "Adsorption of turbid materials by the cyanobacterium Phormidium parchydematicum." Journal of Applied Phycology 22, no. 2 (May 9, 2009): 181–86. http://dx.doi.org/10.1007/s10811-009-9440-y.

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7

Martín-Badosa, Estela. "Trapping through turbid media." Nature Photonics 4, no. 6 (June 2010): 349–50. http://dx.doi.org/10.1038/nphoton.2010.132.

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8

Schmidt, Werner. "A multipurpose, fast scan spectrophotometer for measuring turbid (biological) materials." Experimental Biology Online 2, no. 4 (December 1997): 1–13. http://dx.doi.org/10.1007/s00898-997-0004-9.

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9

El-wakil, S. A., E. M. Abulwafa, A. R. Degheidy, and N. K. Radwan. "The Pomraning-Eddington approximation to diffusion of light in turbid materials." Waves in Random Media 4, no. 2 (April 1994): 127–38. http://dx.doi.org/10.1088/0959-7174/4/2/003.

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10

Brenan, Colin J. H., and Ian W. Hunter. "Volumetric Raman Microscopy Through a Turbid Medium." Journal of Raman Spectroscopy 27, no. 8 (August 1996): 561–70. http://dx.doi.org/10.1002/(sici)1097-4555(199608)27:8<561::aid-jrs7>3.0.co;2-9.

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11

Schmitt, J. M., A. Knüttel, and M. Yadlowsky. "Confocal microscopy in turbid media." Journal of the Optical Society of America A 11, no. 8 (August 1, 1994): 2226. http://dx.doi.org/10.1364/josaa.11.002226.

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12

Yuan, Xin, Linxu Guo, Citong Luo, Xiaoteng Zhou, and Changli Yu. "A Survey of Target Detection and Recognition Methods in Underwater Turbid Areas." Applied Sciences 12, no. 10 (May 12, 2022): 4898. http://dx.doi.org/10.3390/app12104898.

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Based on analysis of state-of-the-art research investigating target detection and recognition in turbid waters, and aiming to solve the problems encountered during target detection and the unique influences of turbidity areas, in this review, the main problem is divided into two areas: image degradation caused by the unique conditions of turbid water, and target recognition. Existing target recognition methods are divided into three modules: target detection based on deep learning methods, underwater image restoration and enhancement approaches, and underwater image processing methods based on polarization imaging technology and scattering. The relevant research results are analyzed in detail, and methods regarding image processing, target detection, and recognition in turbid water, and relevant datasets are summarized. The main scenarios in which underwater target detection and recognition technology are applied are listed, and the key problems that exist in the current technology are identified. Solutions and development directions are discussed. This work provides a reference for engineering tasks in underwater turbid areas and an outlook on the development of underwater intelligent sensing technology in the future.

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13

Xiong, Fei Bing, N. Djeu, and Wen Zhang Zhu. "An Optical Fiber Sensor for Measuring Light Absorption in Suspension Solutions." Applied Mechanics and Materials 121-126 (October 2011): 2509–13. http://dx.doi.org/10.4028/www.scientific.net/amm.121-126.2509.

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An optical fiber sensor based on attenuated total reflectance (ATR) for extraction chemical information from highly scattering turbid materials has been evaluated. The influence of particles on bulk absorption and ATR transmitted spectra of micron-sized graphite flakes and spherical glassy carbon suspensions were investigated. The ATR transmitted spectra of coiled fiber-optic sensor in those suspensions with various concentrations are insensitive to scattering of suspended particles, especially for graphite flake suspensions. The reason for different influence of graphite flakes and spherical glassy carbon particles suspensions on e ATR spectra analyzed. This study demonstrates that fiber-optic sensor based on ATR technique is a feasible technique in application for monitoring turbid suspensions.

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14

Joshi, Neel, Craig Donner, and Henrik Wann Jensen. "Noninvasive measurement of scattering anisotropy in turbid materials by nonnormal incident illumination." Optics Letters 31, no. 7 (April 1, 2006): 936. http://dx.doi.org/10.1364/ol.31.000936.

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15

He, Hexiang, Xiangsheng Xie, Yikun Liu, Haowen Liang, and Jianying Zhou. "Exploiting the point spread function for optical imaging through a scattering medium based on deconvolution method." Journal of Innovative Optical Health Sciences 12, no. 04 (July 2019): 1930005. http://dx.doi.org/10.1142/s1793545819300052.

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Visual perception of humans penetrating turbid medium is hampered by scattering. Various techniques have been prompted recently to recover optical imaging through turbid materials. Among them, speckle correlation based on deconvolution is one of the most attractive methods taking advantage of high imaging quality, robustness, ease-of-use, and ease-of-integration. By exploiting the point spread function (PSF) of the scattering system, large Field-of-View, extended Depth-of-Field, noninvasiveness and spectral resoluation are now available as successful solutions for high quality and multifunctional image reconstruction. In this paper, we review the progress of imaging through a scattering medium based on deconvolution method, including the principle, the breakthrough of the limitation of the optical memory effect, the improvement of the deconvolution algorithm and innovative applications.

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16

Reble, Carina, Ingo Gersonde, Stefan Andree, Hans Joachim Eichler, and Jürgen Helfmann. "Quantitative Raman spectroscopy in turbid media." Journal of Biomedical Optics 15, no. 3 (2010): 037016. http://dx.doi.org/10.1117/1.3456370.

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17

Kienle, Alwin. "Light diffusion through a turbid parallelepiped." Journal of the Optical Society of America A 22, no. 9 (September 1, 2005): 1883. http://dx.doi.org/10.1364/josaa.22.001883.

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18

Soloviev, Vadim Y. "Light transport in refractive turbid media." Journal of the Optical Society of America A 33, no. 3 (February 23, 2016): 383. http://dx.doi.org/10.1364/josaa.33.000383.

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19

Gorodnichev, E. E., S. V. Ivliev, A. I. Kuzovlev, and D. B. Rogozkin. "Transmission of polarized light through turbid media." Optics and Spectroscopy 110, no. 4 (April 2011): 586–94. http://dx.doi.org/10.1134/s0030400x11040114.

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20

Thompson, Jonathan V., Brett H. Hokr, Wihan Kim, Charles W. Ballmann, Brian E. Applegate, Javier Jo, Alexey Yamilov, Hui Cao, Marlan O. Scully, and Vladislav V. Yakovlev. "Enhanced coupling of light into a turbid medium through microscopic interface engineering." Proceedings of the National Academy of Sciences 114, no. 30 (July 12, 2017): 7941–46. http://dx.doi.org/10.1073/pnas.1705612114.

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There are many optical detection and sensing methods used today that provide powerful ways to diagnose, characterize, and study materials. For example, the measurement of spontaneous Raman scattering allows for remote detection and identification of chemicals. Many other optical techniques provide unique solutions to learn about biological, chemical, and even structural systems. However, when these systems exist in a highly scattering or turbid medium, the optical scattering effects reduce the effectiveness of these methods. In this article, we demonstrate a method to engineer the geometry of the optical interface of a turbid medium, thereby drastically enhancing the coupling efficiency of light into the material. This enhanced optical coupling means that light incident on the material will penetrate deeper into (and through) the medium. It also means that light thus injected into the material will have an enhanced interaction time with particles contained within the material. These results show that, by using the multiple scattering of light in a turbid medium, enhanced light–matter interaction can be achieved; this has a direct impact on spectroscopic methods such as Raman scattering and fluorescence detection in highly scattering regimes. Furthermore, the enhanced penetration depth achieved by this method will directly impact optical techniques that have previously been limited by the inability to deposit sufficient amounts of optical energy below or through highly scattering layers.

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21

Huang, Ching-Chuan, and Chun-Chang Liao. "Abrasion damage of geogrids induced by turbid flow." Geotextiles and Geomembranes 25, no. 2 (April 2007): 128–38. http://dx.doi.org/10.1016/j.geotexmem.2006.07.004.

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22

Ntwampe, I. O. "Treatment of AMD using a combination of saw dust, bentonite clay and phosphate in the removal of turbid materials and toxic metals." Water Practice and Technology 16, no. 2 (February 18, 2021): 541–56. http://dx.doi.org/10.2166/wpt.2021.014.

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Abstract Acid mine drainage collected from the western decant in South Africa was treated in a series of small-scale laboratory experiments. 200 mL of the sample was poured into five 500 mL glass beakers using flocculants formed by mixing size-optimized 1.5 g of bentonite clay with 3.5 g saw dust and 1.0 g of Na3PO4 in triplicates (experiment A). Four similar sets of control experiments were conducted using the same amount of bentonite clay and saw dust with varying Na3PO4, contents in AMD treatment; the rationale being to determine the efficiency of Na3PO4 (experiments B, C and D). The results show that conductivity has an influence in the removal of the turbid materials. The removal efficiency of toxic metals using a flocculant containing 220 μm bentonite clay particle size and 0.012 or 0.25 M of Na3PO4 is higher than 96% when compared to that of the samples dosed with a flocculant containing 0.05 M Na3PO4, which is less than 91%. The flocculant also showed optimal removal efficiency of both turbid materials and toxic metals, i.e. removal efficiency within a range 96.5–99.3%. The flocculants containing 0.025 M Na3PO4 showed optimal removal efficiency of turbidity, colour, toxic metals and natural organic compounds.

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23

Neuman, Magnus, and Per Edström. "Anisotropic reflectance from turbid media I Theory." Journal of the Optical Society of America A 27, no. 5 (April 13, 2010): 1032. http://dx.doi.org/10.1364/josaa.27.001032.

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24

Neuman, Magnus, and Per Edström. "Anisotropic reflectance from turbid media II Measurements." Journal of the Optical Society of America A 27, no. 5 (April 13, 2010): 1040. http://dx.doi.org/10.1364/josaa.27.001040.

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25

Ghosh, N., A. Banerjee, and J. Soni. "Turbid medium polarimetry in biomedical imaging and diagnosis." European Physical Journal Applied Physics 54, no. 3 (June 2011): 30001. http://dx.doi.org/10.1051/epjap/2011110017.

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26

Babaie, Jonathan, Mehrdad Abolbashari, Navid Farahi, Sun Myong Kim, and Faramarz Farahi. "Optical film thickness measurement of turbid materials using the fractional BiSpectrum noise-reduction technique." Optics Communications 440 (June 2019): 106–16. http://dx.doi.org/10.1016/j.optcom.2019.01.066.

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27

Svensson, Tomas, Erik Alerstam, Dmitry Khoptyar, Jonas Johansson, Staffan Folestad, and Stefan Andersson-Engels. "Near-infrared photon time-of-flight spectroscopy of turbid materials up to 1400 nm." Review of Scientific Instruments 80, no. 6 (June 2009): 063105. http://dx.doi.org/10.1063/1.3156047.

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28

He, Duo-Min, and Gerald G. L. Seet. "Divergent-beam Lidar imaging in turbid water." Optics and Lasers in Engineering 41, no. 1 (January 2004): 217–31. http://dx.doi.org/10.1016/s0143-8166(02)00138-0.

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29

Urban, Claus, Sara Romer, Frank Scheffold, and Peter Schurtenberger. "Static and dynamic light scattering in turbid suspensions." Macromolecular Symposia 162, no. 1 (December 2000): 235–48. http://dx.doi.org/10.1002/1521-3900(200012)162:1<235::aid-masy235>3.0.co;2-1.

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30

Silverman, M. P., and Wayne Strange. "Ellipsometric penetration of turbid media: depolarization and surface characterization." Thin Solid Films 313-314 (February 1998): 831–35. http://dx.doi.org/10.1016/s0040-6090(97)01004-3.

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31

Putra, Rudy Syah, Desi Nasriyanti, and Muhammad Sarkawi. "Coagulation activity of liquid extraction of Leucaena leucocephala and Sesbania grandiflora on the removal of turbidity." Open Chemistry 20, no. 1 (January 1, 2022): 1239–49. http://dx.doi.org/10.1515/chem-2022-0230.

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Abstract Turbidity is removed by adding a chemical coagulant, which produces a secondary toxic of alumina residues in the water. Therefore, the aim of study was to evaluate the coagulation activity of NaCl extract from Leucaena leucocephala and Sesbania grandiflora seeds on the removal of turbidity for water purification. The proximate composition of the seeds was determined. Fourier transform infrared spectroscopy was used to identify the functional groups of protein, and the surface morphology was observed by SEM-EDS. To obtain the optimized condition, all experiments were evaluated by artificial turbid water before being applied on the natural water (i.e., Selokan Mataram). The coagulation process was evaluated by concentration (M), dosage (mL/L), and pH in terms of turbidity, total dissolved solids, and transmittance of light. The results showed that both coagulant seeds contained 25.32 and 30.81% of protein. These coagulants could remove the turbidity by 99.7% for L. leucocephala and 94.24% for S. grandiflora from artificial turbid water at the optimized concentration of 1.0 M, and dosage of 5 and 10 mL/L, respectively. At pH 5 the removal of turbidity from Selokan Mataram was 99.4% for L. leucocephala and 97.23% for S. grandiflora.

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32

Xing Chong, 幸翀, 黄家寿 Huang Jiashou, and 罗硕 Luo Shuo. "Measurment of Turbid Media′s Backscattering Mueller Matrix." Chinese Journal of Lasers 36, no. 10 (2009): 2587–92. http://dx.doi.org/10.3788/cjl20093610.2587.

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33

Donner, Craig, and Henrik Wann Jensen. "Rapid simulation of steady-state spatially resolved reflectance and transmittance profiles of multilayered turbid materials." Journal of the Optical Society of America A 23, no. 6 (June 1, 2006): 1382. http://dx.doi.org/10.1364/josaa.23.001382.

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34

Qin, Jianwei, and Renfu Lu. "Hyperspectral diffuse reflectance imaging for rapid, noncontact measurement of the optical properties of turbid materials." Applied Optics 45, no. 32 (November 10, 2006): 8366. http://dx.doi.org/10.1364/ao.45.008366.

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35

Schmidt, Werner. "Novel single-beam optical spectrophotometer for fast luminescence, absorption, and reflection measurements of turbid materials." Optical Engineering 34, no. 2 (February 1, 1995): 589. http://dx.doi.org/10.1117/12.188591.

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36

Rogers, Geoffrey L. "Multiple path analysis of reflectance from turbid media." Journal of the Optical Society of America A 25, no. 11 (October 31, 2008): 2879. http://dx.doi.org/10.1364/josaa.25.002879.

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37

Kokhanovsky, Alexander A. "Radiative properties of optically thick fluorescent turbid media." Journal of the Optical Society of America A 26, no. 8 (July 30, 2009): 1896. http://dx.doi.org/10.1364/josaa.26.001896.

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38

Gan, X. S., S. P. Schilders, and Min Gu. "Image formation in turbid media under a microscope." Journal of the Optical Society of America A 15, no. 8 (August 1, 1998): 2052. http://dx.doi.org/10.1364/josaa.15.002052.

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39

Kokhanovsky, Alexander A. "Reflection of light from semi-infinite turbid media." Journal of the Optical Society of America A 15, no. 11 (November 1, 1998): 2877. http://dx.doi.org/10.1364/josaa.15.002877.

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40

Rogers, Geoffrey. "Transmission point spread function of a turbid slab." Journal of the Optical Society of America A 36, no. 10 (September 4, 2019): 1617. http://dx.doi.org/10.1364/josaa.36.001617.

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41

Bonner, R. F., R. Nossal, S. Havlin, and G. H. Weiss. "Model for photon migration in turbid biological media." Journal of the Optical Society of America A 4, no. 3 (March 1, 1987): 423. http://dx.doi.org/10.1364/josaa.4.000423.

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42

Schröer, W., J. Köser, and F. Kuhnen. "Light–scattering in turbid fluids: The single-scattering intensity." Journal of Molecular Liquids 134, no. 1-3 (May 2007): 40–48. http://dx.doi.org/10.1016/j.molliq.2006.12.001.

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43

Ulcickas, James R. W., and Garth J. Simpson. "Mueller Tensor Nonlinear Optical Polarization Analysis in Turbid Media." Journal of Physical Chemistry B 123, no. 30 (July 10, 2019): 6643–50. http://dx.doi.org/10.1021/acs.jpcb.9b04961.

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44

Yang, Hong Ying, Jin Li Zhou, Zhi Wen Que, and Xiao Dan Ma. "The Influence of Dye Concentration on Kubelka-Munk Fundamental Optical Parameters of Fabric." Advanced Materials Research 332-334 (September 2011): 481–84. http://dx.doi.org/10.4028/www.scientific.net/amr.332-334.481.

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Kubelka-Munk theory and a functional hypothesis on the relationship between colored turbid materials and colorant concentration (the so called additivity color-mixing law) work together and play an important role in color science and technology. This paper is to investigate the relations between the dye concentration and the Kubelka-Munk fundamental optical parameters through a series of systematical experiments, data processing and analyzing on fabrics dyed by disperse dyes. The experimental results question the hypothesis.

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45

Gan, Xiaosong, and Min Gu. "Microscopic image reconstruction through tissue-like turbid media." Optics Communications 207, no. 1-6 (June 2002): 149–54. http://dx.doi.org/10.1016/s0030-4018(02)01425-6.

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46

Gopal, Venkatesh, Sushil Mujumdar, Hema Ramachandran, and A. K. Sood. "Imaging in turbid media using quasi-ballistic photons." Optics Communications 170, no. 4-6 (November 1999): 331–45. http://dx.doi.org/10.1016/s0030-4018(99)00468-x.

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47

Jin, Peng Kang, Yong Ning Feng, Jie Xu, and Xian Bao Wang. "The Effect of Polyacrylamide on Floc Structure of Typical Systems." Applied Mechanics and Materials 260-261 (December 2012): 887–90. http://dx.doi.org/10.4028/www.scientific.net/amm.260-261.887.

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Based on that floc structure is an important factor that influencing the coagulation effect and the post-treatment load, the effect of PAM on floc structure of typical system is analyzed and evaluated in this paper. The results show that PAM has a notable influence on floc morphological structure characteristics. For inorganic turbid system, the fractal dimension and diameter of kaolin flocs adding PAM are bigger than that formed by adding aluminum sulfate merely, and the shear-resistant ability of flocs is stronger. With regard to dissolved organic system, adding PAM under two typical pH conditions, the floc morphological characteristic has the same variation with that in inorganic turbid system. PAM could improve the floc morphological structure. However, the improving effect will be relatively weaker under slightly acidic condition, which indicates that the chemical effect of PAM is restrained under this condition. While for the coexisting system, PAM shows an obvious improvement on floc structure under two pH conditions, the floc is compact, bigger and with a higher strength. The chemical effect of PAM is not restrained under slightly acidic condition, which may owe to the interaction between PAM and inorganic suspended materials and dissolved organics in coexisting system.

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48

Goto, Shogo, Kentaro Yasui, Kaito Kassai, Mitsuhiro Sezaki, Yoshimi Okamura, and Hiroyuki Kinoshita. "Application of ceramics made by mixing waste GFRP with clay to filtration materials for turbid water." Proceedings of Conference of Kyushu Branch 2017.70 (2017): 509. http://dx.doi.org/10.1299/jsmekyushu.2017.70.509.

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49

Schmidt, Werner. "A novel single beam optical spectrophotometer for fast luminescence, absorption, and reflection measurements of turbid materials." TrAC Trends in Analytical Chemistry 12, no. 2 (February 1993): 74–82. http://dx.doi.org/10.1016/0165-9936(93)87054-2.

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50

Oelkrug, Dieter, Barbara Boldrini, and Karsten Rebner. "Comparative Raman study of transparent and turbid materials: models and experiments in the remote sensing mode." Analytical and Bioanalytical Chemistry 409, no. 3 (April 30, 2016): 673–81. http://dx.doi.org/10.1007/s00216-016-9582-0.

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