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19 pages, 6460 KiB  
Article
Research on Numerical Simulation and Interpretation Method of Water Injection Well Temperature Field Based on DTS
by Shengzhe Shi, Junfeng Liu, Ming Li, Chao Sun and Tong Lei
Processes 2025, 13(1), 274; https://doi.org/10.3390/pr13010274 - 19 Jan 2025
Viewed by 406
Abstract
Traditional water injection profile monitoring primarily relies on methods such as isotope tracers and oxygen activation. Conventional resistive temperature instruments, which are drag-measured, are highly sensitive to production interference and can only capture the transient temperature response of the wellbore at a single [...] Read more.
Traditional water injection profile monitoring primarily relies on methods such as isotope tracers and oxygen activation. Conventional resistive temperature instruments, which are drag-measured, are highly sensitive to production interference and can only capture the transient temperature response of the wellbore at a single depth. As a result, the temperature data obtained from well temperature logging has certain limitations. Using DTS (Distributed Temperature Sensing) for pre-and post-well opening and shut-in water injection profile testing, along with quantitative analysis of water absorption, addresses the limitations of traditional well temperature logging, which typically offers only qualitative insights. However, the interpretation of DTS data still requires further refinement to improve its alignment with actual conditions. In this study, COMSOL software 6.1 was used to simulate the temperature distribution within the downhole temperature field, both spatially and temporally. The Sobol method was employed to analyze the influence of fluid flow rate and rock thermal conductivity on the temperature field. The results indicated that the fluid flow rate in the wellbore has a more significant impact and is the primary controlling factor of the downhole temperature field. Based on actual field conditions and the forward simulation results, the differential evolution algorithm was applied to invert and interpret the water injection profile. The inversion results showed minimal error, confirming the feasibility of this approach. It is helpful to interpret the well temperature profile measured by the distributed fiber optic temperature sensor, which is helpful to improve the ability of well temperature logging to identify the output profile, which has important academic value and practical significance for the development of water injection wells. Full article
(This article belongs to the Section Energy Systems)
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Figure 1

Figure 1
<p>Schematic diagram of the downhole geometry: (<b>a</b>) schematic diagram of the wellbore; (<b>b</b>) schematic diagram of fiber optic installation location and wellbore cross-section [<a href="#B2-processes-13-00274" class="html-bibr">2</a>].</p>
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<p>Temperature field model.</p>
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<p>Model meshing.</p>
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<p>Wellbore velocity field.</p>
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<p>The temperature field changes when the flow velocity is 0.026 m/s.</p>
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<p>The temperature field changes when the flow velocity is 0.04 m/s.</p>
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<p>The temperature field changes when the flow velocity is 0.07 m/s.</p>
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<p>Temperature at different flow velocities as a function of depth.</p>
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<p>Change in absorbent layer temperature over time.</p>
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<p>Diagram of the temperature field.</p>
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<p>Temperature field maps under different lithologies.</p>
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<p>Histogram of temperature variation difference at different thermal conductivity coefficients.</p>
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<p>Absorbent layer temperature with time for different thermal conductivities.</p>
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<p>Graph of sensitivity analysis results.</p>
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<p>Inversion interpretation flowchart.</p>
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<p>Temperature analysis diagram of the target layer.</p>
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<p>Comparison chart of the results of the inversion interpretation.</p>
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13 pages, 5235 KiB  
Article
Real-Time Determination of Total Suspended Solids in Activated Sludge’s Carousel Using a Single Emitter Ultrasonic Sensor
by Rafael Pessoa Santos Brochado, Thiago de Alencar Neves, Thiago Bressani-Ribeiro, Lariza dos Santos Azevedo, Carolina Gemelli Carneiro, R. Martijn Wagterveld, Doekle Yntema, Klaas Jan Agema and Luewton Lemos Felicio Agostinho
Water 2025, 17(1), 44; https://doi.org/10.3390/w17010044 - 27 Dec 2024
Viewed by 476
Abstract
Sludge management is a very relevant aspect in the operation of Wastewater Treatment Plants (WWTPs). In activated sludge systems, it is common to have daily (or continuous) monitoring of total suspended solids in the aeration tank (MLSS). If such control is not properly [...] Read more.
Sludge management is a very relevant aspect in the operation of Wastewater Treatment Plants (WWTPs). In activated sludge systems, it is common to have daily (or continuous) monitoring of total suspended solids in the aeration tank (MLSS). If such control is not properly performed, it can cause solids to wash out in the secondary sedimentation tank or significantly impact BOD (Biochemical Oxygen Demand) and nitrogen removal. There are many commercially available systems which can provide real-time monitoring of solids (mainly optical or ultrasound sensors). Even though commercially available (usually with a high cost), there are still issues related to the use of such sensors. The most important one is the progressive accumulation of solids, which cause measurement errors. In this work, the authors investigated the application of a low-cost US sensor for MLSS (mixed-liquor suspended solids) monitoring in two full-scale activated sludge WWTPs. The tested sensor was similar to a previously described device, which had been previously employed in a pilot-scale UASB reactor in Brazil. The main differences were related to an integrated treatment and acquisition system which allowed real-time treatment of the US wave as well as data acquisition at a predefined time. The values generated by the sensor were compared with a commercial optical sensor installed in the same WWTP and double-checked with periodic gravimetric tests. The results at a Leeuwarden WWTP showed that the measurements of the US sensor, the optical sensor, and gravimetric test did not present significant differences during the test period at a significance level of 5%. Absolute errors were on average 0.04% (US sensor) and 0.03% (optic sensor) of MLSS compared to the gravimetric test. Although the use of the tested US sensor for monitoring solids in WWTP is promising, there are still several improvements that need to be made to the sensor. These include implementing a more precise calibration frequency, establishing a cleaning routine, and preventing sensor fouling. Furthermore, the sensor still needs a more thorough cost–benefit analysis, which would help assess the practicality of implementing this technology in various WWTPs. Full article
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Figure 1
<p>Scheme of the US sensor instrumentation. “1” represents the data collection methodologies for Leeuwarden WWTP and “2” for the Grou WWTP.</p>
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<p>Grou WWTP’s carousel unit: 1—aerators, 2—optic and ultrasonic sensor position for MLSS measurements.</p>
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<p>Leeuwarden WWTP’s carousel unit: 1—optic sensor (MLSS), 2—US sensor (MLSS).</p>
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<p>Time series of the MLSS measured by the ultrasonic, optic sensor, gravimetric test, and the inflow rate at the Grou WWTP.</p>
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<p>MLSS estimation time series by the ultrasonic and optic sensors compared to the gravimetric test within a period of 34 days during spring season at the Leeuwarden WWTP. Gray shades refer to sampling campaigns with complete signal attenuation due to US sensor fouling.</p>
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<p>Box–whisker plot of the MLSS measurement by the ultrasonic sensor, optic sensor and gravimetric test from 18 May to 20 June 2022 at the Leeuwarden WWTP. The number of measurements is represented by “n”.</p>
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<p>MLSS estimation by the ultrasonic sensor and optic sensor from 24 March to 1 April 2022 at the Grou WWTP. The number of measurements is represented by “n”.</p>
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<p>Solids accumulation in the ultrasonic sensor after the period of one week at the Grou WWTP.</p>
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<p>Solids accumulation in the ultrasonic sensor after two days at the Leeuwarden WWTP.</p>
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27 pages, 4435 KiB  
Article
Remote Ischemic Post-Conditioning (RIC) Mediates Anti-Inflammatory Signaling via Myeloid AMPKα1 in Murine Traumatic Optic Neuropathy (TON)
by Naseem Akhter, Jessica Contreras, Mairaj A. Ansari, Andrew F. Ducruet, Md Nasrul Hoda, Abdullah S. Ahmad, Laxman D. Gangwani, Kanchan Bhatia and Saif Ahmad
Int. J. Mol. Sci. 2024, 25(24), 13626; https://doi.org/10.3390/ijms252413626 - 19 Dec 2024
Viewed by 795
Abstract
Traumatic optic neuropathy (TON) has been regarded a vision-threatening condition caused by either ocular or blunt/penetrating head trauma, which is characterized by direct or indirect TON. Injury happens during sports, vehicle accidents and mainly in military war and combat exposure. Earlier, we have [...] Read more.
Traumatic optic neuropathy (TON) has been regarded a vision-threatening condition caused by either ocular or blunt/penetrating head trauma, which is characterized by direct or indirect TON. Injury happens during sports, vehicle accidents and mainly in military war and combat exposure. Earlier, we have demonstrated that remote ischemic post-conditioning (RIC) therapy is protective in TON, and here we report that AMPKα1 activation is crucial. AMPKα1 is the catalytic subunit of the heterotrimeric enzyme AMPK, the master regulator of cellular energetics and metabolism. The α1 isoform predominates in immune cells including macrophages (Mφs). Myeloid-specific AMPKα1 KO mice were generated by crossing AMPKα1Flox/Flox and LysMcre to carry out the study. We induced TON in mice by using a controlled impact system. Mice (mixed sex) were randomized in six experimental groups for Sham (mock); Sham (RIC); AMPKα1F/F (TON); AMPKα1F/F (TON+RIC); AMPKα1F/F LysMCre (TON); AMPKα1F/F LysMCre (TON+RIC). RIC therapy was given every day (5–7 days following TON). Data were generated by using Western blotting (pAMPKα1, ICAM1, Brn3 and GAP43), immunofluorescence (pAMPKα1, cd11b, TMEM119 and ICAM1), flow cytometry (CD11b, F4/80, CD68, CD206, IL-10 and LY6G), ELISA (TNF-α and IL-10) and transmission electron microscopy (TEM, for demyelination and axonal degeneration), and retinal oxygenation was measured by a Unisense sensor system. First, we observed retinal morphology with funduscopic images and found TON has vascular inflammation. H&E staining data suggested that TON increased retinal inflammation and RIC attenuates retinal ganglion cell death. Immunofluorescence and Western blot data showed increased microglial activation and decreased retinal ganglion cell (RGCs) marker Brn3 and axonal regeneration marker GAP43 expression in the TON [AMPKα1F/F] vs. Sham group, but TON+RIC [AMPKα1F/F] attenuated the expression level of these markers. Interestingly, higher microglia activation was observed in the myeloid AMPKα1F/F KO group following TON, and RIC therapy did not attenuate microglial expression. Flow cytometry, ELISA and retinal tissue oxygen data revealed that RIC therapy significantly reduced the pro-inflammatory signaling markers, increased anti-inflammatory macrophage polarization and improved oxygen level in the TON+RIC [AMPKα1F/F] group; however, RIC therapy did not reduce inflammatory signaling activation in the myeloid AMPKα1 KO mice. The transmission electron microscopy (TEM) data of the optic nerve showed increased demyelination and axonal degeneration in the TON [AMPKα1F/F] group, and RIC improved the myelination process in TON [AMPKα1F/F], but RIC had no significant effect in the AMPKα1 KO mice. The myeloid AMPKα1c deletion attenuated RIC induced anti-inflammatory macrophage polarization, and that suggests a molecular link between RIC and immune activation. Overall, these data suggest that RIC therapy provided protection against inflammation and neurodegeneration via myeloid AMPKα1 activation, but the deletion of myeloid AMPKα1 is not protective in TON. Further investigation of RIC and AMPKα1 signaling is warranted in TON. Full article
(This article belongs to the Special Issue New Therapeutic Targets for Neuroinflammation and Neurodegeneration)
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Figure 1

Figure 1
<p>(<b>A</b>) Representative in vivo funduscopic fluorescein image from C56BL/6 mice showing inflammation in blood vessels in TON as compared with control eye. Intravenous fluorescein angiography of the mouse retina shows poor perfusion through attenuated vasculature (due to progression of the retinal degeneration) following TON. (<b>B</b>) H&amp;E data showed increased neuronal cell death in ganglion cell layer in TON compared with control. However, the neuronal cell death is prevented with RIC treatment. Fluorescein angiography imaging (<b>A</b>) was captured within 5 mins of fluorescein dye injection through tail vein.</p>
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<p>(<b>A</b>,<b>B</b>) Immunofluorescence staining showed microglial marker TMEM119 expression in mouse retina. TON (with AMPK) increases microglial activation, and RIC downregulated significantly. Myeloid pAMPKα1 KO group showed heightened microglial activation; notably, RIC demonstrated no significant effects. Florescence color intensity was measured by Image J software (NIH, <a href="https://imagej.net/ij/" target="_blank">https://imagej.net/ij/</a>). White boxes show the TMEM119 expression in inner nuclear layer (INL) and GCL (ganglion cell layer) region of mouse eye. For Sham (mock) and Sham (RIC), both groups are regarded as AMPKα1<sup>F/F</sup>. (<b>C</b>–<b>I</b>) Representative pseudocolor and histograms of flow cytometry show the gating strategy for microglia/macrophages (CD11b+_F4/80+) and CD68+ and CD206+ expressing microglia in blood. Bar graph summarizing the cell counts of microglia (M1/M2) in the blood after 5 days of TON. Red, TMEM119 (activated microglial marker); Blue, DAPI. We used 6 experimental groups, Sham (mock); Sham (RIC); AMPKα1<sup>F/F</sup> (TON); AMPKα1<sup>F/F</sup> (TON+RIC); AMPKα1<sup>F/F</sup> LysMCre (TON); AMPKα1<sup>F/F</sup> LysMCre (TON+RIC). Differences among experimental groups were determined by analysis of variance (one-way ANOVA) followed by Newman–Keuls multiple comparison tests. The results represent the means ± SEM of fold changes (<span class="html-italic">n</span> = 5). * <span class="html-italic">p</span> &lt; 0.05, *** <span class="html-italic">p</span> &lt; 0.001, **** <span class="html-italic">p</span> &lt; 0.0001. ns, non-significant. For Sham (mock) and Sham (RIC), both groups are regarded as AMPKα1<sup>F/F</sup>.</p>
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<p>(<b>A</b>,<b>B</b>) Immunofluorescence staining showed microglial marker TMEM119 expression in mouse retina. TON (with AMPK) increases microglial activation, and RIC downregulated significantly. Myeloid pAMPKα1 KO group showed heightened microglial activation; notably, RIC demonstrated no significant effects. Florescence color intensity was measured by Image J software (NIH, <a href="https://imagej.net/ij/" target="_blank">https://imagej.net/ij/</a>). White boxes show the TMEM119 expression in inner nuclear layer (INL) and GCL (ganglion cell layer) region of mouse eye. For Sham (mock) and Sham (RIC), both groups are regarded as AMPKα1<sup>F/F</sup>. (<b>C</b>–<b>I</b>) Representative pseudocolor and histograms of flow cytometry show the gating strategy for microglia/macrophages (CD11b+_F4/80+) and CD68+ and CD206+ expressing microglia in blood. Bar graph summarizing the cell counts of microglia (M1/M2) in the blood after 5 days of TON. Red, TMEM119 (activated microglial marker); Blue, DAPI. We used 6 experimental groups, Sham (mock); Sham (RIC); AMPKα1<sup>F/F</sup> (TON); AMPKα1<sup>F/F</sup> (TON+RIC); AMPKα1<sup>F/F</sup> LysMCre (TON); AMPKα1<sup>F/F</sup> LysMCre (TON+RIC). Differences among experimental groups were determined by analysis of variance (one-way ANOVA) followed by Newman–Keuls multiple comparison tests. The results represent the means ± SEM of fold changes (<span class="html-italic">n</span> = 5). * <span class="html-italic">p</span> &lt; 0.05, *** <span class="html-italic">p</span> &lt; 0.001, **** <span class="html-italic">p</span> &lt; 0.0001. ns, non-significant. For Sham (mock) and Sham (RIC), both groups are regarded as AMPKα1<sup>F/F</sup>.</p>
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<p>Effect of RIC on IL10 and neutrophil expression following TON. (<b>A</b>,<b>B</b>,<b>D</b>,<b>F</b>) Representative pseudocolor and histograms of flow cytometry show the gating strategy for microglia/macrophages (CD11b+_IL10+, F4/80+_IL10+ and CD68+_IL10+) and CD68+_LY6G+-expressing neutrophils in blood. (<b>C</b>,<b>E</b>,<b>G</b>,<b>H</b>) Representative bar graph summarizing the cell counts of IL10+ and Ly6G+ in the blood after 5 days of TON. Six experimental groups included Sham (mock); Sham (RIC); AMPKα1<sup>F/F</sup> (TON); AMPKα1<sup>F/F</sup> (TON+RIC); AMPKα1<sup>F/F</sup> LysMCre (TON); AMPKα1<sup>F/F</sup> LysMCre (TON+RIC). Differences among experimental groups were determined by analysis of variance (one-way ANOVA) followed by Newman–Keuls multiple comparison tests. The results represent the means ± SEM of fold changes (<span class="html-italic">n</span> = 5). ** <span class="html-italic">p</span> &lt; 0.01.*** <span class="html-italic">p</span> &lt; 0.001, **** <span class="html-italic">p</span> &lt; 0.0001. ns, non-significant. For Sham (mock) and Sham (RIC), both groups are regarded as AMPKα1<sup>F/F</sup>.</p>
Full article ">Figure 3 Cont.
<p>Effect of RIC on IL10 and neutrophil expression following TON. (<b>A</b>,<b>B</b>,<b>D</b>,<b>F</b>) Representative pseudocolor and histograms of flow cytometry show the gating strategy for microglia/macrophages (CD11b+_IL10+, F4/80+_IL10+ and CD68+_IL10+) and CD68+_LY6G+-expressing neutrophils in blood. (<b>C</b>,<b>E</b>,<b>G</b>,<b>H</b>) Representative bar graph summarizing the cell counts of IL10+ and Ly6G+ in the blood after 5 days of TON. Six experimental groups included Sham (mock); Sham (RIC); AMPKα1<sup>F/F</sup> (TON); AMPKα1<sup>F/F</sup> (TON+RIC); AMPKα1<sup>F/F</sup> LysMCre (TON); AMPKα1<sup>F/F</sup> LysMCre (TON+RIC). Differences among experimental groups were determined by analysis of variance (one-way ANOVA) followed by Newman–Keuls multiple comparison tests. The results represent the means ± SEM of fold changes (<span class="html-italic">n</span> = 5). ** <span class="html-italic">p</span> &lt; 0.01.*** <span class="html-italic">p</span> &lt; 0.001, **** <span class="html-italic">p</span> &lt; 0.0001. ns, non-significant. For Sham (mock) and Sham (RIC), both groups are regarded as AMPKα1<sup>F/F</sup>.</p>
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<p>The effect of RIC on TON induced pro-inflammatory signaling. (<b>A</b>,<b>B</b>) ELISA results in blood plasma showing TNF and IL10 expression. Fluorescence color intensity was measured by Image J software. We used 6 experimental group, Sham (mock); Sham (RIC); AMPKα1<sup>F/F</sup> (TON); AMPKα1<sup>F/F</sup> (TON+RIC); AMPKα1<sup>F/F</sup> LysM<sup>Cre</sup> (TON); AMPKα1<sup>F/F</sup> LysM<sup>Cre</sup> (TON+RIC). Differences among experimental groups were determined by analysis of variance (one-way ANOVA) followed by Newman–Keuls multiple comparison tests. The results represent the means ± SEM of fold changes (<span class="html-italic">n</span> = 5). * <span class="html-italic">p</span> &lt; 0.05, ** <span class="html-italic">p</span> &lt; 0.01, *** <span class="html-italic">p</span> &lt; 0.001, **** <span class="html-italic">p</span> &lt; 0.0001. ns, non-significant. For Sham (mock) and Sham (RIC), both groups are regarded as AMPKα1<sup>F/F</sup>.</p>
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<p>Effect of RIC on TON induced pro-inflammatory signaling. (<b>A</b>,<b>B</b>) The effect of RIC on ICAM-1 expression assessed by immunofluorescence and (<b>C</b>,<b>D</b>) ICAM1 Protein expression was checked by Western blot. Fluorescence color intensity as well as western blot band intensity was measured by Image J software (NIH, <a href="https://imagej.net/ij/" target="_blank">https://imagej.net/ij/</a>). We used 6 experimental groups, Sham (mock); Sham (RIC); AMPKα1<sup>F/F</sup> (TON); AMPKα1<sup>F/F</sup> (TON+RIC); AMPKα1<sup>F/F</sup> LysM<sup>Cre</sup> (TON); AMPKα1<sup>F/F</sup> LysM<sup>Cre</sup> (TON+RIC). Differences among experimental groups were determined by analysis of variance (one-way ANOVA) followed by Newman–Keuls multiple comparison tests. The results represent the means ± SEM of fold changes (<span class="html-italic">n</span> = 5). * <span class="html-italic">p</span> &lt; 0.05, ** <span class="html-italic">p</span> &lt; 0.01, *** <span class="html-italic">p</span> &lt; 0.001, **** <span class="html-italic">p</span> &lt; 0.0001. ns, non-significant. Scale bar 50 μm. For Sham (mock) and Sham (RIC), both groups are regarded as AMPKα1<sup>F/F</sup>.</p>
Full article ">Figure 5 Cont.
<p>Effect of RIC on TON induced pro-inflammatory signaling. (<b>A</b>,<b>B</b>) The effect of RIC on ICAM-1 expression assessed by immunofluorescence and (<b>C</b>,<b>D</b>) ICAM1 Protein expression was checked by Western blot. Fluorescence color intensity as well as western blot band intensity was measured by Image J software (NIH, <a href="https://imagej.net/ij/" target="_blank">https://imagej.net/ij/</a>). We used 6 experimental groups, Sham (mock); Sham (RIC); AMPKα1<sup>F/F</sup> (TON); AMPKα1<sup>F/F</sup> (TON+RIC); AMPKα1<sup>F/F</sup> LysM<sup>Cre</sup> (TON); AMPKα1<sup>F/F</sup> LysM<sup>Cre</sup> (TON+RIC). Differences among experimental groups were determined by analysis of variance (one-way ANOVA) followed by Newman–Keuls multiple comparison tests. The results represent the means ± SEM of fold changes (<span class="html-italic">n</span> = 5). * <span class="html-italic">p</span> &lt; 0.05, ** <span class="html-italic">p</span> &lt; 0.01, *** <span class="html-italic">p</span> &lt; 0.001, **** <span class="html-italic">p</span> &lt; 0.0001. ns, non-significant. Scale bar 50 μm. For Sham (mock) and Sham (RIC), both groups are regarded as AMPKα1<sup>F/F</sup>.</p>
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<p>(<b>A</b>–<b>D</b>) Effect of RIC therapy on retinal oxygenation in TON. Oxygen levels were analyzed with UniSense sensor system (Sweden). We used 6 experimental groups, Sham (mock); Sham (RIC); AMPKα1F/F (TON); AMPKα1F/F (TON+RIC); AMPKα1F/F LysM<sup>Cre</sup> (TON); AMPKα1F/F LysM<sup>Cre</sup> (TON+RIC). Differences among experimental groups were determined by analysis of variance (one-way ANOVA) followed by Newman–Keuls multiple comparison tests. The results represent the means ± SEM of fold changes (<span class="html-italic">n</span> = 5). * <span class="html-italic">p</span> &lt; 0.05, ** <span class="html-italic">p</span> &lt; 0.01, *** <span class="html-italic">p</span> &lt; 0.001, **** <span class="html-italic">p</span> &lt; 0.0001. ns, non-significant. For Sham (mock) and Sham (RIC), both groups are regarded as AMPKα1<sup>F/F</sup>.</p>
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<p>(<b>A</b>–<b>D</b>) Effect of RIC therapy on TON retina. Western blot analysis demonstrated significant changes in protein expression level of Brn3a and GAP43 between TON+RIC and TON group. Densitometry analysis was carried out by Image J software (NIH, <a href="https://imagej.net/ij/" target="_blank">https://imagej.net/ij/</a>). We used 4 experimental groups, AMPKα1F/F (TON); AMPKα1F/F (TON+RIC); AMPKα1F/F LysM<sup>Cre</sup> (TON); AMPKα1F/F LysM<sup>Cre</sup> (TON+RIC). Differences among experimental groups were determined by analysis of variance (one-way ANOVA) followed by Newman–Keuls multiple comparison tests. The results represent the means ± SEM of fold changes (<span class="html-italic">n</span> = 5). * <span class="html-italic">p</span> &lt; 0.05, ** <span class="html-italic">p</span> &lt; 0.01. ns, non-significant.</p>
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<p>Representative ultrastructural features of axonal injury in traumatic optic neuropathy. Electron micrographs are taken across the longitudinal plane through the injury front and show a range of axoplasmic, axolemmal and myelin sheath abnormalities. RIC therapy attenuated this degenerating process in TON. We used 6 experimental groups, Sham (mock); Sham (RIC); AMPKα1F/F (TON); AMPKα1F/F (TON+RIC); AMPKα1F/F LysM<sup>Cre</sup> (TON); AMPKα1F/F LysM<sup>Cre</sup> (TON+RIC). Scale bar 4 μm. For Sham (mock) and Sham (RIC), both groups are regarded as AMPKα1<sup>F/F</sup>.</p>
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<p>Schematic representation demonstrating increased M1-type macrophages causing inflammation and demyelination of optic nerve (ON) in TON. Our hypothesis demonstrates that RIC therapy activates AMPKα1 to modulate macrophage polarization toward M2-type anti-inflammatory macrophages that protect demyelination of downregulated ON.</p>
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7 pages, 1202 KiB  
Proceeding Paper
Optimizing Germanium-Selective Functionalization on Patterned SiGe Substrates with Thiol-Based Molecules: The Critical Role of Oxygen-Free Conditions
by Alessia Arrigoni, Federico Turco, Benedetta Maria Squeo, Sonia Freddi, Monica Bollani, Tersilla Virgili, Andrea Chiappini, Laura Pasquardini and Mariacecilia Pasini
Chem. Proc. 2024, 16(1), 21; https://doi.org/10.3390/ecsoc-28-20193 - 9 Dec 2024
Cited by 1 | Viewed by 392
Abstract
Germanium offers attractive optical properties despite being an indirect bandgap semiconductor, and new Ge-based devices are being optimized for sensing and photonics applications. In particular, considering the use of Ge as a sensor, improving its selectivity via organic grafting offers new alternatives that [...] Read more.
Germanium offers attractive optical properties despite being an indirect bandgap semiconductor, and new Ge-based devices are being optimized for sensing and photonics applications. In particular, considering the use of Ge as a sensor, improving its selectivity via organic grafting offers new alternatives that are still under investigation. In this work, we focus on the selective functionalization of germanium in SiGe-patterned alloys using a custom thiol-based luminescent molecule, namely 6-[2,7-bis[5-(5-hexyl-2-thienyl)-2-thienyl]-9-(6-sulfanylhexyl)fluoren-9-yl]hexane-1-thiol. The process selectively targets regions with Ge, while leaving Si-rich areas uncovered. Moreover, this study emphasizes the importance of an oxygen-free environment, as performing the functionalization in an inert atmosphere significantly improves surface coverage. Full article
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Figure 1

Figure 1
<p>Chemical structure of the grafted molecule.</p>
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<p>Fluorescence microscopy images of SiGe samples functionalized in (<b>1</b>) air, two different sample regions (<b>a</b>,<b>b</b>) and (<b>2</b>) under inert conditions, two different sample regions (<b>c</b>,<b>d</b>). Samples are irradiated by UV light.</p>
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<p>Reaction scheme for the synthesis of Bis-TTF.</p>
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12 pages, 4007 KiB  
Article
Fabrication of Flexible SWCNTs/Polyurethane Coatings for Efficient Electric and Thermal Management of Space Optical Remote Sensors
by Huiqiao Yang, Yueting Wang, Bo Yang, Fulong Ji, Haitong Jiang and Lei Li
Processes 2024, 12(12), 2650; https://doi.org/10.3390/pr12122650 - 25 Nov 2024
Viewed by 596
Abstract
Given the requirement of high-efficiency thermal dissipation for large-aperture space optical remote sensors, a radiator based on single-walled carbon nanotubes (SWCNTs) filled with waterborne polyurethane (SWCNTs/WPU) coatings was proposed in this work. In situ polymerized SWCNTs/WPU coatings allowed for the uniform distribution of [...] Read more.
Given the requirement of high-efficiency thermal dissipation for large-aperture space optical remote sensors, a radiator based on single-walled carbon nanotubes (SWCNTs) filled with waterborne polyurethane (SWCNTs/WPU) coatings was proposed in this work. In situ polymerized SWCNTs/WPU coatings allowed for the uniform distribution of acid-purified SWCNTs in WPU matrix. Modified oxygen-containing groups on purified SWCNTs enhanced the interfacial compatibility of SWCNTs/WPU and enabled an improved tensile strength 9 (26.3 MPa) compared to raw-SWCNTs/WPU. A high electrical conductivity of 5.16 W/mK and thermal conductivity of 10.9 S/cm were achieved by adding 49.1 wt.% of SWCNTs. Only 2.85% and 4.2% of declined ratios for electric and thermal conductivities were presented after 1000 bending cycles, demonstrating excellent durability and flexibility. The designed radiator was composed of a heat pipe, SWCNTs/WPU coatings and an aluminum honeycomb core, allowing for −1.6~0.3 °C of temperature difference for the in-orbit temperature and thermal balance experimental temperature of the collector pipe. Moreover, the close temperature difference for the in-orbit and ground temperatures of the radiator indicated that the designed radiator with high heat dissipation met the mechanical environment requirements of a rocket launch. SWCNTs/WPU would be promising electric/thermal interface materials in the application of space optical remote sensors. Full article
(This article belongs to the Section Materials Processes)
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<p>Schematic illustration for fabricating SWCNTs/WPU.</p>
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<p>SEM images of SWCNTs (<b>a</b>,<b>b</b>), SWCNTs/WPU-1 (<b>c</b>,<b>d</b>), SWCNTs/WPU-2 (<b>e</b>,<b>f</b>), SWCNTs/WPU-3 (<b>g</b>,<b>h</b>), SWCNTs/WPU-4 (<b>i</b>,<b>j</b>), and WPU (<b>k</b>,<b>l</b>).</p>
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<p>Raman spectra of SWCNTs before and after acid treatment (<b>a</b>). XRD patterns of SWCNTs/WPU (<b>b</b>). FTIR spectra of SWCNTs (<b>c</b>) and SWCNTs/WPU (<b>d</b>). TGA (<b>e</b>) and DTG (<b>f</b>) curves of SWCNTs/WPU.</p>
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<p>Effect of SWCNT content on the electrical conductivity (<b>a</b>) and thermal conductivity (<b>b</b>) of r-SWCNTs/WPU and p-SWCNTs/WPU.</p>
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<p>Stress–strain curves of p-SWCNTs/WPU (<b>a</b>). Tensile strength of r-SWCNTs/WPU and p-SWCNTs/WPU (<b>b</b>). Stability of electrical and thermal conductivities of p-SWCNTs/WPU-4 with bending experiment of 0–1000 cycles (<b>c</b>).</p>
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<p>Schematic illustration for heat dissipation solution.</p>
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<p>Heat transformation diagram (<b>a</b>), structural diagram (<b>b</b>), and cross-sectional photograph (<b>c</b>) of thermal radiator.</p>
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<p>Temperature variation of various components and positions of the radiator during the in-orbit flight.</p>
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13 pages, 3048 KiB  
Article
Thermal Quenching of Intrinsic Photoluminescence in Amorphous and Monoclinic HfO2 Nanotubes
by Artem Shilov, Sergey Savchenko, Alexander Vokhmintsev, Kanat Zhusupov and Ilya Weinstein
Materials 2024, 17(22), 5587; https://doi.org/10.3390/ma17225587 - 15 Nov 2024
Viewed by 544
Abstract
Nanotubular hafnia arrays hold significant promise for advanced opto- and nanoelectronic applications. However, the known studies concern mostly the luminescent properties of doped HfO2-based nanostructures, while the optical properties of nominally pure hafnia with optically active centers of intrinsic origin are [...] Read more.
Nanotubular hafnia arrays hold significant promise for advanced opto- and nanoelectronic applications. However, the known studies concern mostly the luminescent properties of doped HfO2-based nanostructures, while the optical properties of nominally pure hafnia with optically active centers of intrinsic origin are far from being sufficiently investigated. In this work, for the first time we have conducted research on the wide-range temperature effects in the photoluminescence processes of anion-defective hafnia nanotubes with an amorphous and monoclinic structure, synthesized by the electrochemical oxidation method. It is shown that the spectral parameters, such as the position of the maximum and half-width of the band, remain almost unchanged in the range of 7–296 K. The experimental data obtained for the photoluminescence temperature quenching are quantitatively analyzed under the assumption made for two independent channels of non-radiative relaxation of excitations with calculating the appropriate energies of activation barriers—9 and 39 meV for amorphous hafnia nanotubes, 15 and 141 meV for monoclinic ones. The similar temperature behavior of photoluminescence spectra indicates close values of short-range order parameters in the local atomic surrounding of the active emission centers in hafnium dioxide with amorphous and monoclinic structure. Anion vacancies VO and VO2 appeared in the positions of three-coordinated oxygen and could be the main contributors to the spectral features of emission response and observed thermally stimulated processes. The recognized and clarified mechanisms occurring during thermal quenching of photoluminescence could be useful for the development of light-emitting devices and thermo-optical sensors with functional media based on oxygen-deficient hafnia nanotubes. Full article
(This article belongs to the Special Issue Advances in Luminescent Materials)
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<p>Scanning electron microscope (SEM) (<b>a</b>,<b>b</b>) and transmission electron microscope (TEM) (<b>c</b>,<b>d</b>) images obtained for the monoclinic HfO<sub>2</sub> nanotubes under study. The value marked in (<b>d</b>) corresponds to the interplanar distance <math display="inline"><semantics> <mrow> <mover accent="true"> <mn>1</mn> <mo>¯</mo> </mover> <mn>11</mn> </mrow> </semantics></math>.</p>
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<p>Photoluminescence (PL) spectra of amorphous (<b>top</b>) and monoclinic (<b>bottom</b>) hafnia nanotubes measured at different temperatures.</p>
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<p>Temperature dependencies of the experimental values of the maximum position E<sub>max</sub> (blue color) and half-width FWHM (green color) of the measured PL bands. The circles indicate data for amorphous NTs, triangles—for monoclinic NTs. The dashed lines show the averaged values of E<sub>max</sub> and FWHM in the temperature range of 7–296 K.</p>
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<p>PL spectra of amorphous (<b>left</b>, circles) and monoclinic (<b>right</b>, triangles) nanotubes measured at a temperature of 10 K, with decomposition into Gaussian components (red lines).</p>
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<p>Dependence <span class="html-italic">I</span>(<span class="html-italic">T</span>) for amorphous (<b>top</b>) and monoclinic (<b>bottom</b>) NTs. The red and blue lines, see insets, are linear approximations.</p>
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13 pages, 1808 KiB  
Article
Prediction of Thrombus Formation within an Oxygenator via Bioimpedance Analysis
by Jan Korte, Tobias Lauwigi, Lisa Herzog, Alexander Theißen, Kai Suchorski, Lasse J. Strudthoff, Jannis Focke, Sebastian V. Jansen, Thomas Gries, Rolf Rossaint, Christian Bleilevens and Patrick Winnersbach
Biosensors 2024, 14(10), 511; https://doi.org/10.3390/bios14100511 - 18 Oct 2024
Viewed by 1302
Abstract
Blood clot formation inside the membrane oxygenator (MO) remains a risk in extracorporeal membrane oxygenation (ECMO). It is associated with thromboembolic complications and normally detectable only at an advanced stage. Established clinical monitoring techniques lack predictive capabilities, emphasizing the need for refinement in [...] Read more.
Blood clot formation inside the membrane oxygenator (MO) remains a risk in extracorporeal membrane oxygenation (ECMO). It is associated with thromboembolic complications and normally detectable only at an advanced stage. Established clinical monitoring techniques lack predictive capabilities, emphasizing the need for refinement in MO monitoring towards an early warning system. In this study, an MO was modified by integrating four sensor fibers in the middle of the hollow fiber mat bundle, allowing for bioimpedance measurement within the MO. The modified MO was perfused with human blood in an in vitro test circuit until fulminant clot formation. The optical analysis of clot residues on the extracted hollow fibers showed a clot deposition area of 51.88% ± 14.25%. This was detectable via an increased bioimpedance signal with a significant increase 5 min in advance to fulminant clot formation inside the MO, which was monitored by the clinical gold standard (pressure difference across the MO (dp-MO)). This study demonstrates the feasibility of detecting clot growth early and effectively by measuring bioimpedance within an MO using integrated sensor fibers. Thus, bioimpedance may even outperform the clinical gold standard of dp-MO as a monitoring method by providing earlier clot detection. Full article
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<p>View of modified RatOx: (<b>A</b>) Top view. (<b>B</b>) Lateral view. (<b>C</b>) Axial Micro-CT scan. Hollow fiber mat bundle (+) with integrated sensor fibers (*).</p>
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<p>Schematic illustration of the experimental setup. dp-MO: pressure difference across the oxygenator. The syringe indicates the location of blood sampling; created with BioRender.com.</p>
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<p>Exemplary images of stamped-out hollow fiber mats of the RatOx after flushing with sodium chloride solution. (<b>Left image</b>) Blood clot formation adherent to sensor fibers; (<b>right image</b>) no visible blood clot formation. View from inflow direction (1) until the last hollow fiber mat at the outflow region (11); one remaining hollow fiber mat (6) inside the bundle next to the sensor fibers.</p>
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<p>(<b>A</b>) The bar chart represents the share of hollow fiber mat area covered with blood clot residues for the clotting and control groups; the color contrast ranges from white (no/barely covered with blood clot deposits) to dark red (heavily covered with blood clot deposits) shown within the bars. Mean clot deposit on the hollow fiber mats surface is significantly higher in the clotting vs. control group and within the control group on hollow fiber mat No. 1 and 6 vs. every other hollow fiber mat in the control group. ANOVA: ** <span class="html-italic">p</span> &lt; 0.002 vs. hollow fiber mat No. 2 to 5 and 7 to 11; *** <span class="html-italic">p</span> &lt; 0.001 vs. control. (<b>B</b>) Exemplary scans of the hollow fiber mat layers 1–11, representative of the values shown in (<b>A</b>).</p>
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<p>Significant increase of impedance signal 5 min prior to fulminant clot formation (green area * <span class="html-italic">p</span> &lt; 0.05) in the clotting group (dots, 0.25 IU/mL heparin, <span class="html-italic">n</span> = 7), in contrast to the control group (squares, 5 IU/mL heparin, <span class="html-italic">n</span> = 5) showing no increase. First indicators for clot formation in hemodynamic parameters (increase in dp-MO) were detectable 3 min later (yellow area). Fulminant clot formation was indicated by an increase in dp-MO in conjunction with doubling of the pump’s speed (&gt;60 RPM) resulting in the termination of the experiments (red area). Mean ± SD, ANOVA; * <span class="html-italic">p</span> &lt; 0.05 vs. baseline (BL).</p>
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<p>Platelet count (PLTs) and Activated Clotting Time (ACT) over the relative duration of the experiments. (<b>A</b>) PLTs in the clotting group (0.25 IU/mL; <span class="html-italic">n</span> = 7) decreased significantly compared to the those in the control group (5 IU/mL; <span class="html-italic">n</span> = 5). (<b>B</b>) In the control group, ACT increased significantly after initial heparinization, in comparison to the control group. All values within the respective quarter were cumulated and averaged. Mean ± SEM, ANOVA; * <span class="html-italic">p</span> &lt; 0.05, ; ** <span class="html-italic">p</span> &lt; 0.002; *** <span class="html-italic">p</span> &lt; 0.001.</p>
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18 pages, 4465 KiB  
Article
Development of a Microbioreactor for Bacillus subtilis Biofilm Cultivation
by Mojca Seručnik, Iztok Dogsa, Lan Julij Zadravec, Ines Mandic-Mulec and Polona Žnidaršič-Plazl
Micromachines 2024, 15(8), 1037; https://doi.org/10.3390/mi15081037 - 15 Aug 2024
Viewed by 1228
Abstract
To improve our understanding of Bacillus subtilis growth and biofilm formation under different environmental conditions, two versions of a microfluidic reactor with two channels separated by a polydimethylsiloxane (PDMS) membrane were developed. The gas phase was introduced into the channel above the membrane, [...] Read more.
To improve our understanding of Bacillus subtilis growth and biofilm formation under different environmental conditions, two versions of a microfluidic reactor with two channels separated by a polydimethylsiloxane (PDMS) membrane were developed. The gas phase was introduced into the channel above the membrane, and oxygen transfer from the gas phase through the membrane was assessed by measuring the dissolved oxygen concentration in the liquid phase using a miniaturized optical sensor and oxygen-sensitive nanoparticles. B. subtilis biofilm formation was monitored in the growth channels of the microbioreactors, which were designed in two shapes: one with circular extensions and one without. The volumes of these microbioreactors were (17 ± 4) μL for the reactors without extensions and (28 ± 4) μL for those with extensions. The effect of microbioreactor geometry and aeration on B. subtilis biofilm growth was evaluated by digital image analysis. In both microbioreactor geometries, stable B. subtilis biofilm formation was achieved after 72 h of incubation at a growth medium flow rate of 1 μL/min. The amount of oxygen significantly influenced biofilm formation. When the culture was cultivated with a continuous air supply, biofilm surface coverage and biomass concentration were higher than in cultivations without aeration or with a 100% oxygen supply. The channel geometry with circular extensions did not lead to a higher total biomass in the microbioreactor compared to the geometry without extensions. Full article
(This article belongs to the Special Issue Feature Papers of Micromachines in Biology and Biomedicine 2024)
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<p>Structure of the microbioreactor, consisting of 1—PMMA plate with holes for the liquid and gas supply, 2—double-sided adhesive polypropylene foil with a carved channel for the gas supply, thickness 143 μm, 3—PDMS membrane, thickness 108.5 ± 0.9 μm, 4—double-sided adhesive polypropylene foil with a carved channel for the bacterial culture, thickness 143 μm, 5—glass coverslip. (<b>a</b>) Schematic presentation of a microbioreactor with a rectangular growth channel; (<b>b</b>) photos of the components of the microbioreactor with circular extensions of the rectangular growth channel.</p>
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<p>Removal of the transparent PDMS membrane from the Teflon foil after incubation in the oven. The membrane was used to transfer oxygen from the gas to the liquid phase within the microbioreactor. To facilitate detachment from the support, the front edge of the membrane was placed on adhesive tape. The scale bar corresponds to 10 mm.</p>
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<p>Concentration of dissolved oxygen in a liquid solution containing an indicator in the form of nanoparticles. The flow rate of the gas (starting with nitrogen, and further changes are indicated on the graph) was 2 mL/min, while liquid flow rates were (<b>a</b>) 5 µL/min and (<b>b</b>) 10 µL/min. Only one of the three replicates is shown, while their standard deviations are listed in <a href="#micromachines-15-01037-t001" class="html-table">Table 1</a>.</p>
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<p>Cultivation of <span class="html-italic">B. subtilis</span> biofilm in a microreactor with a rectangular growth channel in CGM at 36 °C, an air flow rate of 1 mL/min, and a growth medium flow rate of 1 μL/min. (<b>a</b>) Growth channel filled with CGM; (<b>b</b>) biofilm after 18 h, (<b>c</b>) after 24 h, (<b>d</b>) after 48 h, and (<b>e</b>) after 72 h; (<b>f</b>) time dependence of two replicates (rep 1 and rep 2) of the surface coverage of the rectangular growth channel by the <span class="html-italic">B. subtilis</span> biofilm (orange) and time dependence of the optical density (<span class="html-italic">OD</span>) within the growth channel (blue) as a quantitative measure of biofilm coverage and biomass accumulation. Note that the white spots in figures (<b>a</b>–<b>e</b>) outside the channel are due to the adhesive between the film and the PDMS membrane.</p>
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<p>Time dependence of <span class="html-italic">B. subtillis</span> biofilm coverage of the rectangular growth channel surface (orange) and time dependence of optical density (OD) within the growth channel (blue) as a quantitative measure of biofilm coverage and biomass accumulation in a complete growth medium (<b>a</b>) at a flow rate of 1 μL/min and (<b>b</b>) at a flow rate of 0.3 μL/min at 36 °C. The flow rate of 100% oxygen was 1 mL/min in both cases. The replicate experiments are referred to as rep 1, rep 2, and rep 3.</p>
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<p>Time dependence of <span class="html-italic">B. subtillis</span> biofilm coverage of the rectangular growth channel surface (orange) and time dependence of optical density (OD) within the growth channel (blue) as a quantitative measure of biofilm coverage and biomass accumulation in a complete growth medium (<b>a</b>) at a flow rate of 1 μL/min and (<b>b</b>) at a flow rate of 0.3 μL/min at 36 °C. The flow rate of 100% oxygen was 1 mL/min in both cases. The replicate experiments are referred to as rep 1, rep 2, and rep 3.</p>
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<p>Cultivation of <span class="html-italic">B. subtilis</span> biofilm in a microreactor with a rectangular growth channel with circular extensions at 36 °C and with a complete growth medium (CGM) flow rate of 1 μL/min and an air flow rate of 1 mL/min: (<b>a</b>) growth channel filled with CGM; (<b>b</b>) biofilm after 19 h, (<b>c</b>) after 24 h, (<b>d</b>) after 48 h, (<b>e</b>) after 72 h, and (<b>f</b>) after 144 h; (<b>g</b>) time dependence of <span class="html-italic">B. subtillis</span> biofilm surface coverage of the growth channel (orange) and time dependence of the optical density (<span class="html-italic">OD</span>) within the growth channel (blue) as quantitative measure of the biofilm coverage and biomass accumulation. The replicate experiments are referred to as rep 1 and rep 2.</p>
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<p>Cultivation of <span class="html-italic">B. subtilis</span> biofilm in a microreactor with a rectangular growth channel with circular extensions at 36 °C and in a complete growth medium (CGM) introduced at a flow rate of 1 μL/min and 100% O<sub>2</sub> supplied with a flow rate of 1 mL/min. (<b>a</b>) Growth channel filled with CGM; (<b>b</b>) biofilm after 17 h, (<b>c</b>) 24 h, (<b>d</b>) 48 h, (<b>e</b>) 72 h, and (<b>f</b>) 144 h; (<b>g</b>) time dependence of <span class="html-italic">B. subtillis</span> biofilm surface coverage of the growth channel (orange) and time dependence of the optical density (<span class="html-italic">OD</span>) within the growth channel (blue) as quantitative measure of the biofilm coverage and biomass accumulation. The replicate experiments are referred to as rep 1 and rep 2.</p>
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<p>Cultivation of <span class="html-italic">B. subtilis</span> biofilm in a microreactor with a rectangular growth channel with circular extensions in CGM at 36 °C and without aeration: (<b>a</b>) growth channel filled with CGM; (<b>b</b>) biofilm after 19 h, (<b>c</b>) 24 h, (<b>d</b>) 48 h, (<b>e</b>) 72 h, and (<b>f</b>) 144 h; (<b>g</b>) time dependence of <span class="html-italic">B. subtillis</span> biofilm surface coverage of the growth channel (orange) and time dependence of the optical density (OD) within the growth channel (blue) as quantitative measure of the biofilm coverage and biomass accumulation. The replicate experiments are referred to as rep 1 and rep 2.</p>
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<p>Phenotypic heterogeneity of <span class="html-italic">B. subtilis</span> cells in biofilm: long settler cells and short explorer cells after 72 h cultivation in a microbioreactor with circular expansions in complete growth medium introduced at a flow rate of 1 μL/min and an air flow rate of 2 mL/min. The scale bar represents 50 µm.</p>
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<p>Representative images of <span class="html-italic">B. subtilis</span> biofilms in a microbioreactor with circular extensions taken by light microscopy after 24 h of cultivation at 36 °C in complete growth medium supplied at a flow rate of 1 μL/min and providing (<b>a</b>) 100% oxygen at a flow rate of 2 mL/min, (<b>b</b>) air at a flow rate of 2 mL/min, or (<b>c</b>) no aeration. The scale bars represent 50 µm.</p>
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19 pages, 5276 KiB  
Article
Design and Implementation of a Low-Power Device for Non-Invasive Blood Glucose
by Luis Miguel Pires and José Martins
Designs 2024, 8(4), 63; https://doi.org/10.3390/designs8040063 - 24 Jun 2024
Cited by 1 | Viewed by 1964
Abstract
Glucose is a simple sugar molecule. The chemical formula of this sugar molecule is C6H12O6. This means that the glucose molecule contains six carbon atoms (C), twelve hydrogen atoms (H), and six oxygen atoms (O). In human [...] Read more.
Glucose is a simple sugar molecule. The chemical formula of this sugar molecule is C6H12O6. This means that the glucose molecule contains six carbon atoms (C), twelve hydrogen atoms (H), and six oxygen atoms (O). In human blood, the molecule glucose circulates as blood sugar. Normally, after eating or drinking, our bodies break down the sugars in food and use them to obtain energy for our cells. To execute this process, our pancreas produces insulin. Insulin “pulls” sugar from the blood and puts it into the cells for use. If someone has diabetes, their pancreas cannot produce enough insulin. As a result, the level of glucose in their blood rises. This can lead to many potential complications, including blindness, disease, nerve damage, amputation, stroke, heart attack, damage to blood vessels, etc. In this study, a non-invasive and therefore easily usable method for monitoring blood glucose was developed. With the experiment carried out, it was possible to measure glucose levels continuously, thus eliminating the disadvantages of invasive systems. Near-IR sensors (optical sensors) were used to estimate the concentration of glucose in blood; these sensors have a wavelength of 940 nm. The sensor was placed on a small black parallelepiped-shaped box on the tip of the finger and the output of the optical sensor was then connected to a microcontroller at the analogue input. Another sensor used, but only to provide more medical information, was the heartbeat sensor, inserted into an armband (along with the microprocessor). After processing and linear regression analysis, the glucose level was predicted, and data were sent via the Bluetooth network to a developed APP. The results of the implemented device were compared with available invasive methods (commercial products). The hardware consisted of a microcontroller, a near-IR optical sensor, a heartbeat sensor, and a Bluetooth module. Another objective of this experiment using low-cost and low-power hardware was to not carry out complex processing of data from the sensors. Our practical laboratory experiment resulted in an error of 2.86 per cent when compared to a commercial product, with a hardware cost of EUR 8 and a consumption of 50 mA. Full article
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<p>Light spectrum [<a href="#B23-designs-08-00063" class="html-bibr">23</a>].</p>
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<p>System architecture.</p>
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<p>NIR emitter LED (<b>left</b>) and optical receiver (<b>right</b>).</p>
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<p>MAX30102 board (5-pin version).</p>
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<p>MAX30102 board (7-pin version).</p>
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<p>MAX30102 block diagram.</p>
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<p>Blood circulation example: arteries (<b>a</b>) and veins (<b>b</b>).</p>
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<p>Electrical scheme of experiment.</p>
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<p>Firmware flowchart.</p>
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<p>Influence of light propagation in glucose molecules.</p>
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<p>Experimental diagram of the glucose meter.</p>
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<p>Point cloud and linear regression to expression in (1).</p>
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<p>Visual design of the experimental prototype.</p>
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<p>Appearance of the app.</p>
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9 pages, 3671 KiB  
Article
Chromogenic Approach for Oxygen Sensing Using Tapered Coreless Optical Fibre Coated with Methylene Blue
by Rahul Kumar and Neil Wight
Metrology 2024, 4(2), 295-303; https://doi.org/10.3390/metrology4020018 - 12 Jun 2024
Viewed by 1164
Abstract
In this paper, a Methylene Blue (MB)-coated tapered coreless (TCL) optical fibre sensor is proposed and experimentally investigated for oxygen sensing in the near-infrared (NIR) wavelength range of 993.5 nm. The effect of TCL diameter and MB sol–gel coating thickness on the sensitivity [...] Read more.
In this paper, a Methylene Blue (MB)-coated tapered coreless (TCL) optical fibre sensor is proposed and experimentally investigated for oxygen sensing in the near-infrared (NIR) wavelength range of 993.5 nm. The effect of TCL diameter and MB sol–gel coating thickness on the sensitivity of the sensor was also investigated. A maximum sensitivity of 0.19 dB/O2% in the oxygen concentration range of 0–37.5% was achieved for a TCL fibre sensor with a 2 µm taper waist diameter and a 0.86 µm MB sol–gel coating thickness, with a response time of 4 min. The sensor provides reproducible results even after 7 days and is shown to be highly selective to oxygen compared to argon and ethanol at the same concentration. Full article
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<p>(<b>a</b>) Schematic diagram of functionalised tapered coreless (TCL) fibre optic sensor showing original 125 µm diameter and fabricated waist region created using the heat and pull technique, and (<b>b</b>) SEM images of fabricated MB sol–gel-coated TCL fibre structure, with LHS image showing the coating thickness and RHS image showing the waist diameter and uniformity of the MB sol–gel coating. (<b>c</b>) SEM image showing the lengths of transition and waist regions for a TCL fibre structure with a 4 µm waist diameter.</p>
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<p>Schematic diagram of the experimental apparatus showing the sealed gas chamber, carrier and test gas flow inlets, and chamber gas outlet, alongside the broadband optical source and optical spectrum analyser used to provide and detect NIR light.</p>
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<p>Intensity variation for different concentrations of oxygen using a fabricated TCL fibre optic sensor with a 2 µm tapering diameter and a 0.86 µm MB sol–gel coating thickness: (<b>a</b>) with respect to time, and (<b>b</b>) spectral response. A reduction in intensity as oxygen concentration increases is clearly shown, as well as the response time of the sensor to changes in the oxygen concentration.</p>
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<p>Change in intensity as a function of changing oxygen concentrations, for fabricated 2 and 4 µm tapered-waist-diameter TCL fibre optic sensors, coated with 0.39, 0.69, and 0.89 µm thicknesses of MB sol–gel. Intensity changes for an un-tapered 125 µm coreless fibre optic sensor with a 0.86 µm MB sol–gel coating thickness are also shown for reference.</p>
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<p>Effect of coating thickness and diameter of TCL optical fibre sensor on its sensitivity, revealing sensitivity to oxygen concentration for increasing MB sol–gel coating thickness.</p>
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<p>Selectivity of MB sol–gel-coated TCL fibre optic sensor with 2 µm tapering diameter and coating thickness of 0.86 µm for oxygen versus argon and ethanol.</p>
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<p>Repeatability for TCL fibre optic sensor with 2 µm tapering diameter and coating thickness of 0.86 µm after exposure to ambient conditions for 7 days.</p>
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28 pages, 3237 KiB  
Review
Recent Technologies for Transcutaneous Oxygen and Carbon Dioxide Monitoring
by Sara Bernasconi, Alessandra Angelucci, Anastasia De Cesari, Aurora Masotti, Maurizio Pandocchi, Francesca Vacca, Xin Zhao, Chiara Paganelli and Andrea Aliverti
Diagnostics 2024, 14(8), 785; https://doi.org/10.3390/diagnostics14080785 - 9 Apr 2024
Cited by 3 | Viewed by 3654
Abstract
The measurement of partial pressures of oxygen (O2) and carbon dioxide (CO2) is fundamental for evaluating a patient’s conditions in clinical practice. There are many ways to retrieve O2/CO2 partial pressures and concentrations. Arterial blood gas [...] Read more.
The measurement of partial pressures of oxygen (O2) and carbon dioxide (CO2) is fundamental for evaluating a patient’s conditions in clinical practice. There are many ways to retrieve O2/CO2 partial pressures and concentrations. Arterial blood gas (ABG) analysis is the gold standard technique for such a purpose, but it is invasive, intermittent, and potentially painful. Among all the alternative methods for gas monitoring, non-invasive transcutaneous O2 and CO2 monitoring has been emerging since the 1970s, being able to overcome the main drawbacks of ABG analysis. Clark and Severinghaus electrodes enabled the breakthrough for transcutaneous O2 and CO2 monitoring, respectively, and in the last twenty years, many innovations have been introduced as alternatives to overcome their limitations. This review reports the most recent solutions for transcutaneous O2 and CO2 monitoring, with a particular consideration for wearable measurement systems. Luminescence-based electronic paramagnetic resonance and photoacoustic sensors are investigated. Optical sensors appear to be the most promising, giving fast and accurate measurements without the need for frequent calibrations and being suitable for integration into wearable measurement systems. Full article
(This article belongs to the Special Issue Technologies in the Diagnosis of Lung Diseases)
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<p>Representation of the non-pulsatile and pulsatile blood components determining the plethysmography pulse range measurement.</p>
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<p>Timeline of oxygen and carbon dioxide sensors for transcutaneous gas monitoring.</p>
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<p>Transcutaneous sensors for oxygen detection. (<b>a</b>) Electrochemical sensor for transcutaneous oxygen detection positioned at ear lobe; (<b>b</b>) optical thin film sensor (adapted from [<a href="#B64-diagnostics-14-00785" class="html-bibr">64</a>]); and (<b>c</b>) SPOT chip, exploiting electronic paramagnetic resonance (adapted from [<a href="#B7-diagnostics-14-00785" class="html-bibr">7</a>]).</p>
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<p>Time domain representation of dual lifetime referencing signal for different values of carbon dioxide. A<sub>1</sub> is the signal obtained from CO<sub>2</sub>-insensitive luminophore, while A<sub>2</sub> and A<sub>4</sub> are the signals of the fluorophore. A<sub>3</sub> represents the total luminescence during the period in which the LED is off (Adapted from [<a href="#B65-diagnostics-14-00785" class="html-bibr">65</a>]).</p>
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<p>Conceptual design of a rate-based monitor, including all the components: valve, fan (or pump), sensor, and sampler chamber [<a href="#B1-diagnostics-14-00785" class="html-bibr">1</a>].</p>
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17 pages, 5313 KiB  
Article
Monitoring Water Quality Parameters in Small Rivers Using SuperDove Imagery
by Katerina Vatitsi, Sofia Siachalou, Dionissis Latinopoulos, Ifigenia Kagalou, Christos S. Akratos and Giorgos Mallinis
Water 2024, 16(5), 758; https://doi.org/10.3390/w16050758 - 2 Mar 2024
Cited by 1 | Viewed by 2364
Abstract
Freshwater ecosystems provide an array of provisioning, regulating/maintenance, and cultural ecosystem services. Despite their crucial role, freshwater ecosystems are exceptionally vulnerable due to changes driven by both natural and human factors. Water quality is essential for assessing the condition and ecological health of [...] Read more.
Freshwater ecosystems provide an array of provisioning, regulating/maintenance, and cultural ecosystem services. Despite their crucial role, freshwater ecosystems are exceptionally vulnerable due to changes driven by both natural and human factors. Water quality is essential for assessing the condition and ecological health of freshwater ecosystems, and its evaluation involves various water quality parameters. Remote sensing has become an efficient approach for retrieving and mapping these parameters, even in optically complex waters such as small rivers. This study specifically focuses on modelling two non-optically active water quality parameters, dissolved oxygen (DO) and electrical conductivity (EC), by integrating 3 m PlanetScope satellite imagery with data from real-time in situ remote monitoring sensors across two small rivers in Thrace, Northeast Greece. We employed three different experimental setups using a support vector regression (SVR) algorithm: ‘Multi-seasonal by Individual Sensor’ (M-I-S) for individual sensor analysis across two seasons, ‘Multi-seasonal—All Sensors’ (M-A-S) integrating data across all seasons and sensors, and ‘Seasonal—All Sensors’ (S-A-S) focusing on per-season sensor data. The models incorporating multiple seasons and all in situ sensors resulted in R2 values of 0.549 and 0.657 for DO and EC, respectively. A multi-seasonal approach per in situ sensor resulted in R2 values of 0.885 for DO and 0.849 for EC. Meanwhile, the seasonal approach, using all in situ sensors, achieved R2 values of 0.805 for DO and 0.911 for EC. These results underscore the significant potential of combining PlanetScope data and machine learning to model these parameters and monitor the condition of ecosystems over small river surfaces. Full article
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<p>Laspias River and Lissos River basins, and locations of the four real-time remote monitoring in situ sensors.</p>
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<p>Taylor diagrams of DO (<b>a</b>) and EC (<b>b</b>) of ‘Multi-seasonal by Individual Sensor’ (M-I-S) models. Distance between model and reference point is a measure of how realistically each model reproduces observations. The azimuthal angle represents the correlation between predicted and observed values, and RMSE is shown by the blue contours. The radial distance from the origin (black contours) refers to the standard deviation.</p>
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<p>Scatter plots (<b>a</b>,<b>c</b>) and Taylor diagrams (<b>b</b>,<b>d</b>) of M-A-S DO and EC models, respectively. The red dashed line is the 1:1 reference line, and the blue dotted line is the trend line considering the relationship between predicted and observed values.</p>
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<p>Scatter plots of S-A-S DO (<b>a</b>,<b>b</b>) and EC models (<b>c</b>,<b>d</b>). Plots (<b>a</b>,<b>c</b>) refer to the spring period, and plots (<b>b</b>,<b>d</b>) refer to the summer period. The red dashed line is the 1:1 reference line, and the blue dotted line is the trend line considering the relationship between predicted and observed values.</p>
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<p>Electrical conductivity distribution maps around the Lis-1 (<b>a</b>,<b>d</b>,<b>g</b>), Lis-2 (<b>b</b>,<b>e</b>,<b>h</b>), and Lis-3 (<b>c</b>,<b>f</b>,<b>i</b>) sites in the Lissos River on 25 March 2022 (<b>a</b>–<b>c</b>), 22 June 2022 (<b>d</b>–<b>f</b>), and 29 October 2022 (<b>g</b>–<b>i</b>) based on the M-A-S models.</p>
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<p>Dissolved oxygen distribution maps around the Lis-1 (<b>a</b>,<b>d</b>,<b>g</b>), Lis-2 (<b>b</b>,<b>e</b>,<b>h</b>), and Lis-3 (<b>c</b>,<b>f</b>,<b>i</b>) sites in the Lissos River on 25 March 2022 (<b>a</b>–<b>c</b>), 22 June 2022 (<b>d</b>–<b>f</b>), and 29 October 2022 (<b>g</b>–<b>i</b>) based on the M-A-S models.</p>
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<p>Electrical conductivity distribution maps around the Las-1 site in the Laspias River on 25 March 2022 (<b>a</b>), 27 June 2022 (<b>b</b>), and 28 October 2022 (<b>c</b>) based on the M-I-S models.</p>
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<p>Dissolved oxygen distribution maps around the Las-1 site in the Laspias River on 25 March 2022 (<b>a</b>), 27 June 2022 (<b>b</b>), and 28 October 2022 (<b>c</b>) based on the M-I-S models.</p>
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47 pages, 8839 KiB  
Review
The Art of Fluorescence Imaging with Chemical Sensors: The Next Decade 2012–2022
by Michael Schäferling and Vladimir Ondrus
Chemosensors 2024, 12(3), 31; https://doi.org/10.3390/chemosensors12030031 - 23 Feb 2024
Cited by 1 | Viewed by 2600
Abstract
Imaging methods by the means of optical sensors are applied in diverse scientific areas such as medical research and diagnostics, aerodynamics, environmental analysis, or marine research. After a general introduction to the field, this review is focused on works published between 2012 and [...] Read more.
Imaging methods by the means of optical sensors are applied in diverse scientific areas such as medical research and diagnostics, aerodynamics, environmental analysis, or marine research. After a general introduction to the field, this review is focused on works published between 2012 and 2022. The covered topics include planar sensors (optrodes), nanoprobes, and sensitive coatings. Advanced sensor materials combined with imaging technologies enable the visualization of parameters which exhibit no intrinsic color or fluorescence, such as oxygen, pH, CO2, H2O2, Ca2+, or temperature. The progress on the development of multiple sensors and methods for referenced signal read out is also highlighted, as is the recent progress in device design and application formats using model systems in the lab or methods for measurements’ in the field. Full article
(This article belongs to the Special Issue Fluorescent Probe for Sensing and Bioimaging)
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<p>Synthesis route and chemical structures of new oxygen-sensitive europium and gadolinium complexes. Reprinted from Borisov et al. Adv. Funct. Mat. 2014, 24, 6548, Copyright 2014 John Wiley and Sons [<a href="#B30-chemosensors-12-00031" class="html-bibr">30</a>].</p>
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<p>(<b>A</b>) Experimental set up to determine skin oxygenation using the LLI-based imaging technology. The LLI-device excites the sensor foils with a pulsable LED array (blue light). Subsequent to the pulse of excitation light, the oxygen-dependent decay of the red light emitted from the sensor foil will be recorded by the LLI-device with the use of a time-gated CCD camera. The transparent sensor foil consists of a sensor layer, which comprises an oxygen-dependent probe immobilized in a highly oxygen-permeable polymer matrix. (<b>B</b>) Calibration of the LLI-sensor foil. (<b>C</b>) LLI-sensor foil (green) on the footpad (white edging) of a hind leg of a restrained mouse that is positioned on a heating foil (black). (<b>D</b>) Representative black and white intensity image of the sensor (<b>left</b>) and the corresponding referenced pseudocolour image (<b>right</b>) of the calculated skin tissue oxygen distribution. Reprinted from Hofmann et al. Methods Appl. Fluoresc. 2013, [<a href="#B32-chemosensors-12-00031" class="html-bibr">32</a>]. © IOP Publishing. Reproduced with permission. All rights reserved.</p>
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<p>Perfused bioreactor experimental set up. The culture medium in reservoir 1 flows through gas-permeable tubes to the culture chamber and to reservoir 2. The culture chamber may hold 3 scaffolds. At the outlet of the culture chamber, a bypass circuit composed of a 3-way valve and a gas-impermeable tubing with an optically accessible miniaturized bioreactor allows the oxygen concentration in the culture medium to be measured. The exhausted culture medium in reservoir 2 was reversed and collected in a waste reservoir to assess glucose and lactate content. Reprinted from Eghbali et al. Int. J. Artif. Organs. 2017, 40, 185. Copyright 2017 Springer [<a href="#B38-chemosensors-12-00031" class="html-bibr">38</a>].</p>
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<p>Chemical structure of pHsensitive diazaoxatriangulenium dyes and PET sensing mechanism. Adapted with permission from Dalfen et al. Anal. Chem. 2019, 91, 808. Copyright 2019 American Chemical Society [<a href="#B43-chemosensors-12-00031" class="html-bibr">43</a>].</p>
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<p>(<b>a</b>) Diagram of a pH-sensing film integrated into a paper-based culture platform. A single sheet of paper, wax-patterned with three identical channels, was seeded with cells, sandwiched between a PET film and pH sensor, and placed in a custom-made acrylic holder. (<b>b</b>) Representative micrographs of a (<b>top</b>) single channel seeded with mCherry-expressing MDA-MB-231 cells, (<b>middle</b>) the pH-sensitive fluorescein particles, and (<b>bottom</b>) the pH-insensitive DPA reference particles. The wax lines were used to limit cellular movement during the experiment and are visible through the sensing film. (<b>c</b>) Schematic of the pH sensor (not to scale). Reprinted with permission from Kenney et al. Anal. Chem. <b>2018</b> [<a href="#B47-chemosensors-12-00031" class="html-bibr">47</a>]. Copyright 2018 American Chemical Society.</p>
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<p>Chemical structures and reaction mechanisms of DPP-based fluorescent pH indicators. (<b>a</b>) Photoinduced electron transfer induced by deprotonation of the phenol group, and (<b>b</b>) shift in fluorescence emission maximum induced by deprotonation of nitrogen. Reproduced from Ref. [<a href="#B51-chemosensors-12-00031" class="html-bibr">51</a>] with permission from the Royal Society of Chemistry.</p>
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<p>Clinical case of a 51-year-old male, three years after laryngectomy and radiochemotherapy, who suffered from severe wound healing disorder after treatment of a voice fistula insufficency. (<b>a</b>) Photo documentation. (<b>b</b>) pO<sub>2</sub> sensor response. (<b>c</b>) pH sensor response. Sensor foils have a size of 2 × 2 cm. Copyright © 2019, Springer Nature, Auerswald et al., Radiat. Oncol. 2019, 14, 199 [<a href="#B59-chemosensors-12-00031" class="html-bibr">59</a>]. <a href="https://creativecommons.org/licenses/by/4.0/" target="_blank">https://creativecommons.org/licenses/by/4.0/</a> (accessed on 2 February 2024).</p>
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<p>(<b>a</b>) Chemical structures of cyclometalated iridium(III) complexes and sensing mechanism for peroxynitrite ONOO<sup>−</sup>. (<b>b</b>) Scheme of the synthetis route to phosphorescent mesoporous silica nanoprobe (MSN-ONOO) for peroxynitrite determination. Reprinted from Chen et al. Adv. Healthcare Mater. 2018, 7, 1800309, Copyright 2018 John Wiley and Sons [<a href="#B69-chemosensors-12-00031" class="html-bibr">69</a>].</p>
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<p>Synthesis and structure of molecular probes and nanosensor particles based on pH-sensitive perylene-bisimide dyes. Insert: Turn on fluorescence mechanism by interruption of PET due to the protonation of amino groups. Used with permission of Royal Society of Chemistry, Aigner et al. J. Mater. Chem. B, 2014, 2, 6792–6801, permission conveyed through Copyright Clearance Center, Inc. [<a href="#B74-chemosensors-12-00031" class="html-bibr">74</a>].</p>
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<p>Scheme of a ratiometric pH nanosensors consisting of hyperbranched polylactide nanoparticles, a score that is functionalized with the naphthalimide-based fluorophores N2 (green) as the pH-sensitive probe and N1 (blue) as the reference. Protonation of the naphthalimide leads to interruption of intramolecular PET. Reprinted with permission from Bao et al. Chem. Mater. 2015, 27, 3450–3455 [<a href="#B79-chemosensors-12-00031" class="html-bibr">79</a>]. Copyright 2015 American Chemical Society.</p>
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<p>Scheme and spectral properties of K<sup>+</sup>-sensitive Bodipy dye encapsulated in cationic methacrylate copolymer nanoparticles RL100. Reprinted from Müller et al. Adv. Funct. Mater. 2018, 28, 1704598 [<a href="#B80-chemosensors-12-00031" class="html-bibr">80</a>]. Copyright 2018 John Wiley and Sons.</p>
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<p>Preparation of dual-labeled carbon nanodots (DLCDs) with FITC as pH-sensitive dye and RBITC as reference. Reprinted from Shi et al. Angew. Chem. Int. Ed. 2012, 51, 6432–6435 [<a href="#B98-chemosensors-12-00031" class="html-bibr">98</a>]. Copyright 2018 John Wiley and Sons.</p>
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<p>(<b>a</b>) Scheme of the structure of a dopamine nanosensor and the resulting fluorescence emission enhancement of (GT)<sub>15</sub>DNA-wrapped SWNTs after binding of dopamine. Dopamine increases the fluorescence emission intensity of using both 1PE (<b>b</b>) and 2PE (<b>c</b>). The dashed line indicates the original signal, while solid the line indicates signal after dopamine addition. Reprinted from Del Bonis-O’Donnell et al., Adv. Funct. Mater. 2017, 27, 1702112 [<a href="#B103-chemosensors-12-00031" class="html-bibr">103</a>]. Copyright 2018 John Wiley and Sons.</p>
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<p>Top: Scheme of a ratiometric core–shell UC nanoprobe for intracellular pH sensing. The fluorescence of the pH-sensitive dye pHrodo Red is sensitized by the red upconversion luminescence (LRET), the green emission acts as reference. Bottom: Ratiometric imaging of pH probes reveals their localization in three types of microenvironment. Panel A shows localization of UCNPs by means of its green emission (550 nm) using 980 nm excitation, panel B sensitized UC-RET emission from pHrodo Red, panel C shows outlines of the cell in transmitted light, and panel D shows an overlaid ratiometric image of pH nanoprobes with different ratio depending on the localization. Different intensity ratios indicate localization of the nanoprobes in extracellular medium (ctrl), small endosomes, large endosomes, and lysosomes. Scale bar 10 μm [<a href="#B113-chemosensors-12-00031" class="html-bibr">113</a>].</p>
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<p>Normalized absorption and emission spectra showing the spectral overlap of the emission of NaYF<sub>4</sub>:Yb/Tm nanoparticles with the absorption of the oxygen-sensitive probe [Ru(dpp)<sub>3</sub>]<sup>2+</sup>Cl<sub>2</sub>. Black line: emission spectrum of the nanoparticles under photoexcitation at 980 nm. Red and blue line: absorbance and emission spectrum of [Ru(dpp)<sub>3</sub>]<sup>2+</sup>Cl<sub>2</sub>, respectively [<a href="#B117-chemosensors-12-00031" class="html-bibr">117</a>]. Reprinted with permission from Liu et al., J. Amer. Chem. Soc. 2015, Copyright 2015 American Chemical Society.</p>
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<p>(<b>a</b>) General design and synthetic route of silica coated upconversion nanoprobe functionalized with a merocyanaine dye (MC) UCNPs@SiO<sub>2</sub>-MC. (<b>b</b>) Sensing mechanism for HS<sup>−</sup> detection and energy transfer (LRET) process of UCNPs@SiO<sub>2</sub>-MC [<a href="#B122-chemosensors-12-00031" class="html-bibr">122</a>]. Reprinted with permission from Liu et al., ACS Appl. Mater. Interfaces 2014, 6, 14, 11013. Copyright 2014 American Chemical Society.</p>
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<p>Experimental set up of the soil incubation box. Excitation filter: 470 nm short-pass filter; emission filter: 530 nm long-pass filter. (<b>a</b>) Filter membrane, ~10 μm thick, (<b>b</b>) DGT gel, ~100 μm thick, and (<b>c</b>) planar oxygen optode, ~30 μm thick. Copyright © 2016 Wibke et al. [<a href="#B129-chemosensors-12-00031" class="html-bibr">129</a>]. Published by Elsevier Ltd.</p>
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<p>pH distribution obtained by RGB imaging of a planar pH-sensitive optrode patterns in the rhizopshere of <span class="html-italic">Vallisneria spiralsv</span>. (<b>A</b>) Photo of roots of <span class="html-italic">Vallisneria spiralsv</span> through the side of a rhizobox. The three white dashed lines (a,b,c) represent the positions of the extracted profiles, presented in (<b>C</b>,<b>D</b>). (<b>B</b>) Two-dimensional pH distribution around the roots from <span class="html-italic">Vallisneria spiralsv</span> taken after 4 h in the light. The images size is 20 mm × 56 mm. (<b>C</b>) Two profiles (<b>a</b>,<b>b</b>) of pH distribution across the sediment and water interface represented by the horizontal dashed line (<b>D</b>) pH distribution across two single roots from one profile (<b>c</b>), with the rhizosphere zones indicated as shade areas [<a href="#B135-chemosensors-12-00031" class="html-bibr">135</a>]. Copyright © 2018, Springer Nature, Han et al., Sci. Rep. 2016, 6, 26417. <a href="https://creativecommons.org/licenses/by/4.0/" target="_blank">https://creativecommons.org/licenses/by/4.0/</a> (accessed on 2 February 2024).</p>
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<p>(<b>A</b>) Composition of a planar NH<sub>3</sub> optrode and the chemical reaction with ammonia that leads to a changed emission of the indicator dye Oxazoline 170 perchlorate due to deprotonation. Makrolex yellow is added as reference. (<b>B</b>) Ratiometric calibration curve of the NH<sub>3</sub> and a close up of the linear range. Copyright © 2020 Merl et al. [<a href="#B140-chemosensors-12-00031" class="html-bibr">140</a>]. Published by Elsevier Ltd.</p>
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<p>Experimental set up for combined NH<sub>3</sub>, pH, and O<sub>2</sub> visualization. Two transparent glass plates form a soil sandwich. Optrodes (one O<sub>2</sub>, one pH, and two NH<sub>3</sub>) were attached to the insides as shown. Soil is filled in between the slides and the optrodes leave a headspace. Two single-lens reflex cameras as well as a blue LED and a UV LED are positioned at the respective sides of the soil sandwich. This enables simultaneous imaging of the three parameters. Copyright © 2020 Merl et al. [<a href="#B140-chemosensors-12-00031" class="html-bibr">140</a>]. Published by Elsevier Ltd.</p>
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<p>(<b>A</b>) False color images showing the ratio between the red and green channel from RGB images of a spray-painted coral skeleton at various defined O<sub>2</sub> levels in the surrounding seawater. (<b>B</b>) Calibration curve calculated by fitting an exponential decay function to the red-to-green ratio values vs. O<sub>2</sub> concentration data. Copyright © 2016 Koren et al. [<a href="#B143-chemosensors-12-00031" class="html-bibr">143</a>]. Published by Elsevier Ltd.</p>
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<p>Left: PSP coating composed of PtTFPP as a sensor dye and PTMSP as binder on the lower side of a wing. Right: Pressure distribution on the upper side of wing model at test conditions <span class="html-italic">Re</span> = 25 × 10<sup>6</sup> (Reynolds number), <span class="html-italic">T</span> = 296 K, angle of attack = 1°. Luminescence lifetime data were converted to pressure coefficients and displayed [<a href="#B176-chemosensors-12-00031" class="html-bibr">176</a>]. Copyright © 2018 by the American Institute of Aeronautics and Astronautics, Inc.</p>
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<p>(<b>a</b>) Normalized intensity change, (<b>b</b>) relative temperature sensitivity of ruthenium complexes with different terpyridine ligands, and (<b>c</b>) description of the complexes [<a href="#B225-chemosensors-12-00031" class="html-bibr">225</a>]. Copyright © 2016 by the American Institute of Aeronautics and Astronautics, Inc.</p>
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<p>Boundary layer transition on a swept wing using the 2C-cryoTSP at <span class="html-italic">T</span> = 278 K, <span class="html-italic">Ma</span> = 0.5, and <span class="html-italic">Re</span> = 1.7 million in DNW-KRG and with a different surface roughness [<a href="#B226-chemosensors-12-00031" class="html-bibr">226</a>]. Copyright © 2018 by the American Institute of Aeronautics and Astronautics, Inc.</p>
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<p>Top: Picture of a PSP/TSP-coated propeller model in the test section of a low-speed wind tunnel. Bottom: Test results showing the pressure distribution at different rotational speeds n from 3000 to 24,550 at the suction side of the propeller blade [<a href="#B230-chemosensors-12-00031" class="html-bibr">230</a>]. © 2018 by Claucherty et al. <a href="http://creativecommons.org/licenses/by/4.0/" target="_blank">http://creativecommons.org/licenses/by/4.0/</a> (accessed on 2 February 2024).</p>
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28 pages, 4379 KiB  
Article
Estimation of the Biogeochemical and Physical Properties of Lakes Based on Remote Sensing and Artificial Intelligence Applications
by Kaire Toming, Hui Liu, Tuuli Soomets, Evelyn Uuemaa, Tiina Nõges and Tiit Kutser
Remote Sens. 2024, 16(3), 464; https://doi.org/10.3390/rs16030464 - 25 Jan 2024
Cited by 8 | Viewed by 2015
Abstract
Lakes play a crucial role in the global biogeochemical cycles through the transport, storage, and transformation of different biogeochemical compounds. Their regulatory service appears to be disproportionately important relative to their small areal extent, necessitating continuous monitoring. This study leverages the potential of [...] Read more.
Lakes play a crucial role in the global biogeochemical cycles through the transport, storage, and transformation of different biogeochemical compounds. Their regulatory service appears to be disproportionately important relative to their small areal extent, necessitating continuous monitoring. This study leverages the potential of optical remote sensing sensors, specifically Sentinel-2 Multispectral Imagery (MSI), to monitor and predict water quality parameters in lakes. Optically active parameters, such as chlorophyll a (CHL), total suspended matter (TSM), and colored dissolved matter (CDOM), can be directly detected using optical remote sensing sensors. However, the challenge lies in detecting non-optically active substances, which lack direct spectral characteristics. The capabilities of artificial intelligence applications can be used in the identification of optically non-active compounds from remote sensing data. This study aims to employ a machine learning approach (combining the Genetic Algorithm (GA) and Extreme Gradient Boost (XGBoost)) and in situ and Sentinel-2 Multispectral Imagery data to construct inversion models for 16 physical and biogeochemical water quality parameters including CHL, CDOM, TSM, total nitrogen (TN), total phosphorus (TP), phosphate (PO4), sulphate, ammonium nitrogen, 5-day biochemical oxygen demand (BOD5), chemical oxygen demand (COD), and the biomasses of phytoplankton and cyanobacteria, pH, dissolved oxygen (O2), water temperature (WT) and transparency (SD). GA_XGBoost exhibited strong predictive capabilities and it was able to accurately predict 10 biogeochemical and 2 physical water quality parameters. Additionally, this study provides a practical demonstration of the developed inversion models, illustrating their applicability in estimating various water quality parameters simultaneously across multiple lakes on five different dates. The study highlights the need for ongoing research and refinement of machine learning methodologies in environmental monitoring, particularly in remote sensing applications for water quality assessment. Results emphasize the need for broader temporal scopes, longer-term datasets, and enhanced model selection strategies to improve the robustness and generalizability of these models. In general, the outcomes of this study provide the basis for a better understanding of the role of lakes in the biogeochemical cycle and will allow the formulation of reliable recommendations for various applications used in the studies of ecology, water quality, the climate, and the carbon cycle. Full article
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<p>Study area, 45 lakes of the input data for the GA_XGBoost model (Lakes (In situ), blue dots); and 180 Estonian lakes (&gt;0.1 km<sup>2</sup>), whose biogeochemical and physical water quality parameters were retrieved using the GA_XGBoost models and Sentinel-2 data (Lakes (Sentinel-2), red dots).</p>
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<p>Heatmap of Pearson correlations between biogeochemical and physical water quality parameters. Statistically significant correlations (<span class="html-italic">p</span>-value &lt; 0.05) are colored either red (positive) or blue (negative), while correlations that were not significant (<span class="html-italic">p</span> &gt; 0.05) are marked as grey.</p>
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<p>The mean Sentinel-2 MSI atmospherically corrected reflectance spectra sorted by the trophic state of study lakes. Sentinel-2 data are derived from each match-up point. Thick lines show the mean value, and the semitransparent area shows the standard error (±) of the mean.</p>
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<p>Scatter plots of training, test, and validation datasets produced using the best GA_XGB_model for deriving biogeochemical and physical water quality parameters from Sentinel-2 data along with the ideal model (1:1 line). The figure starts on the previous page.</p>
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<p>Scatter plots of training, test, and validation datasets produced using the best GA_XGB_model for deriving biogeochemical and physical water quality parameters from Sentinel-2 data along with the ideal model (1:1 line). The figure starts on the previous page.</p>
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<p>The boxplots of the mean values of chlorophyll a (CHL, µg/L), colored dissolved organic matter (CDOM, mg/L), total suspended matter (TSM, mg/L), total nitrogen (TN, mg/L), total phosphorus (TP, mg/L), PO<sub>4</sub> (mg/L), TN:TP ratio, BOD<sub>5</sub> (mg O<sub>2</sub>/L), COD (mg O<sub>2</sub>/L), pH, Secchi depth (SD, m), water temperature (WT, C°), and O<sub>2</sub> (mg/L) in 180 Estonian lakes &gt; 0.1 km<sup>2</sup> on five different dates using Sentinel-2 data. On the plots the line indicates the median, the circle is the mean, the box shows the interquartile range, and the upper and lower whiskers are the maximum and minimum, respectively.</p>
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14 pages, 3216 KiB  
Article
UV Absorption Spectrum for Dissolved Oxygen Monitoring: A Low-Cost Proposal for Water Quality Monitoring
by Aika Miura, Lorena Parra, Jaime Lloret and Mónica Catalá-Icardo
Photonics 2023, 10(12), 1336; https://doi.org/10.3390/photonics10121336 - 1 Dec 2023
Cited by 2 | Viewed by 3306
Abstract
One of the key indicators of water quality is dissolved oxygen. Even though oxygen is important in environmental monitoring, the sensors for dissolved oxygen are expensive and require periodic maintenance due to the use of membranes. In this paper, we propose using ultraviolet [...] Read more.
One of the key indicators of water quality is dissolved oxygen. Even though oxygen is important in environmental monitoring, the sensors for dissolved oxygen are expensive and require periodic maintenance due to the use of membranes. In this paper, we propose using ultraviolet light absorption to estimate dissolved oxygen saturation in water samples. The absorption spectrum of dissolved oxygen in the ultraviolet range is investigated over a water matrix with different levels of complexity. First, the difference between different water matrixes is studied. The results indicate similar variations between river water and tap water matrices for comparative purposes. Both samples present much higher absorbance signals than distilled water. Thus, the rest of the tests were performed with only three water matrixes (ultrapure, distilled, and river water). By aerating, water samples were completely saturated. Then, nitrogen gas was used to remove dissolved oxygen from samples to obtain saturations of 75, 50, 25, and 3%. The absorption was measured from 190 to 380 nm, using LLG-uniSPEC 2. The obtained data were used to generate regression models for selected wavelengths (190, 210, 240, and 250 nm). The differences beyond 260 nm for the studied dissolved oxygen saturations were null. The generated models had correlation coefficients from 0.99 to 0.97 for ultrapure water, 0.98 to 0.95 for distilled water, and 0.90 to 0.83 for river water. The maximum differences were found between samples with 75 and 100% of saturation. Full article
(This article belongs to the Special Issue Editorial Board Members’ Collection Series: Photonics Sensors)
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Figure 1
<p>Sample preparation schematic. (<b>A1</b>) River in which RW samples are collected. (<b>A2</b>) Distilled water for DW samples. (<b>A3</b>) Barnstead Smart2Pure purification system for UW samples. (<b>B</b>) DO8500 Portable Optical DO sensor used to verify DO saturations. (<b>C</b>) The nitrogen gas system with pressure gauge. (<b>D</b>) The method used for nitrogen introduction into sample cuvette measurements.</p>
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<p>Detection scheme, using a spectrophotometer and UC wavelength range.</p>
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<p>Plot of the absorbance signal with respect to the wavelength for DW, TW, and RW samples.</p>
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<p>Absorbance signals for UW samples in the UVC range.</p>
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<p>Absorbance signals for DW samples in the UVC range.</p>
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<p>Absorbance signals for RW samples in the UVC range.</p>
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<p>Plot of absorbance signals and DO saturation with UW results. Calibration at 210 nm (Squared Root-Y Squared-X Model).</p>
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<p>Plot of absorbance signals and DO saturation with UW results. Calibration at 210 nm (Squared-X Model).</p>
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<p>Plot of absorbance signals and DO saturation with DW results. Model calibration at 210 nm (Squared-X Model).</p>
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<p>Plot of absorbance signals and DO saturation with RW results. Model calibration at 210 nm (Squared-X Model).</p>
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