Changes in power generation performance of an undershot cross-flow-type hydraulic turbine in an irrigation channel due to snow masses passing through the rotor.

This study is focused on the development of a microhydraulic turbine that can stably and efficiently generate electricity even in channel where snow masses frequently flow down. A hydraulic turbine of an undershot cross-flow type was installed in an irrigation channel, and the change in the turbine performance was measured when spherical snowballs were released one by one from the upstream. The observation of the snowballs passing through the turbine was also conducted. Consequently, the variations in the power generated by the rotor were classified into three modes based on the motion of the snowballs, and could be organized by the ratio of the snowballs' cross-sectional area to the product of the rotor width and blade interval. Furthermore, the emergence of the power output overshoot phenomenon, in which the power output temporarily increases compared to clear water when the rotor restarts after stopping, was identified, and the relationship between the amount of loss when the rotor stops and that of electric energy gained during the overshoot was clarified. Certain guidelines for the installation of the undershot cross-flow type in irrigation channels of snowy regions was successfully obtained.

Inactivation characteristics of a 280 nm Deep-UV irradiation dose on aerosolized SARS-CoV-2.

A non-filter virus inactivation unit was developed that can control the irradiation dose of aerosolized viruses by controlling the lighting pattern of a 280 nm deep-UV (DUV)-LED and the air flowrate. In this study, the inactivation properties of aerosolized SARS-CoV-2 were quantitatively evaluated by controlling the irradiation dose to the virus inside the inactivation unit. The RNA concentration of SARS-CoV-2 remained constant when the total irradiation dose of DUV irradiation to the virus exceeded 16.5 mJ/cm2. This observation suggests that RNA damage may occur in regions below the detection threshold of RT-qPCR assay. However, when the total irradiation dose was less than 16.5 mJ/cm2, the RNA concentration monotonically increased with a decreasing LED irradiation dose. However, the nucleocapsid protein concentration of SARS-CoV-2 was not predominantly dependent on the LED irradiation dose. The plaque assay showed that 99.16% of the virus was inactivated at 8.1 mJ/cm2 of irradiation, and no virus was detected at 12.2 mJ/cm2 of irradiation, resulting in a 99.89% virus inactivation rate. Thus, an irradiation dose of 23% of the maximal irradiation capacity of the virus inactivation unit can activate more than 99% of SARS-CoV-2. These findings are expected to enhance versatility in various applications. The downsizing achieved in our study renders the technology apt for installation in narrow spaces, while the enhanced flowrates establish its viability for implementation in larger facilities.

Simultaneous Measurement of Volumetric Flowrates of Gas-Liquid Bubbly Flow Using a Turbine Flowmeter.

The flowrate measurement of the gas-liquid two-phase flow frequently observed in industrial equipment, such as in heat exchangers and reactors, is critical to enable the precise monitoring and operation of the equipment. Furthermore, certain applications, such as oil and natural gas processing plants, require the accurate measurements of the flowrates of each phase simultaneously. This study presents a method that can simultaneously measure the volumetric flowrates of each phase of gas and liquid two-phase mixtures, Qg and Ql, respectively, without separating the phases. The method employs a turbine flowmeter and two pressure sensors connected to the pipes upstream and downstream of the turbine flowmeter. By measuring the rotational speed of the rotor and the pressure loss across the flowmeter, the flowrate of the two-phase mixtures Qtp = (Qg + Ql) and the gas volumetric flowrate ratio ß = (Qg/Qtp) are determined. The values of Qg and Ql are calculated as ßQtp and (1 - ß)Qtp. This study also investigates the measurement accuracies for air-water two-phase flows at 0.67 × 10-3 ≤ Qtp ≤ 1.67 × 10-3 m3/s and ß ≤ 0.1, concluding that the full-scale accuracies of Qtp, ß, Qg, and Ql are 3.1%, 4.8%, 3.9%, and 3%, respectively. These accuracies either match or improve the accuracies of similar methods reported in the literature, indicating that the proposed method is a viable solution for the determination of phase-specific flowrates in gas-liquid two-phase mixtures.

Characteristics of collection and inactivation of virus in air flowing inside a winding conduit equipped with 280 nm deep UV-LEDs.

A general-purpose virus inactivation unit that can inactivate viruses was developed using deep ultraviolet (DUV) LEDs that emit DUV rays with a wavelength of 280 nm. The inside of the virus inactivation unit is a rectangular conduit with a sharp turn of 180° (sharp-turned rectangular conduit). Virus inactivation is attempted by directly irradiating the air passing through the conduit with DUV rays. The flow characteristics of air and virus particles inside the virus inactivation unit were investigated using numerical simulations. The air was locally accelerated at the sharp turn parts and flowed along the partition plate in the sharp-turned rectangular conduit. The aerosol particles moving in the sharp-turned rectangular conduit were greatly bent in orbit at the sharp turn parts, and then rapidly approached the partition plate at the lower part of the conduit. Consequently, many particles collided with the partition plates behind the sharp-turn parts. SARS-CoV-2 virus was nebulized in the virus inactivation unit, and the RNA concentration and virus inactivation rate with and without the emission of DUV-LEDs were measured in the experiment. The concentration of SARS-CoV-2 RNA was reduced to 60% through DUV-LED irradiation. In addition, SARS-CoV-2 passing through the virus inactivation unit was inactivated below the detection limit by the emission of DUV-LEDs. The virus inactivation rate and the value of the detection limit corresponded to 99.38% and 35.36 TCID50/mL, respectively.

Oligopeptide Transport in Rat Lung Alveolar Epithelial Cells is Mediated by Pept2.

PURPOSE: Studies were conducted in primary cultured rat alveolar epithelial cell monolayers to characterize peptide transporter expression and function. METHODS: Freshly isolated rat lung alveolar epithelial cells were purified and cultured on permeable support with and without keratinocyte growth factor (KGF). Messenger RNA and protein expression of Pept1 and Pept2 in alveolar epithelial type I- and type II-like cell monolayers (±KGF, resp.) were examined by RT-PCR and Western blotting. 3H-Glycyl-sarcosine (3H-gly-sar) transmonolayer flux and intracellular accumulation were evaluated in both cell types. RESULTS: RT-PCR showed expression of Pept2, but not Pept1, mRNA in both cell types. Western blot analysis revealed presence of Pept2 protein in type II-like cells, and less in type I-like cells. Bi-directional transmonolayer 3H-gly-sar flux lacked asymmetry in transport in both types of cells. Uptake of 3H-gly-sar from apical fluid of type II-like cells was 7-fold greater than that from basolateral fluid, while no significant differences were observed from apical vs. basolateral fluid of type I-like cells. CONCLUSIONS: This study confirms the absence of Pept1 from rat lung alveolar epithelium in vitro. Functional Pept2 expression in type II-like cell monolayers suggests its involvement in oligopeptide lung disposition, and offers rationale for therapeutic development of di/tripeptides, peptidomimetics employing pulmonary drug delivery.

Numerical Simulation of Bubble Cluster Induced Flow by Three-Dimensional Vortex-in-Cell Method.

The behavior of air bubble clusters rising in water and the induced flow field are numerically studied using a three-dimensional two-way coupling algorithm based on a vortex-in-cell (VIC) method. In this method, vortex elements are convected in the Lagrangian frame and the liquid velocity field is solved from the Poisson equation of potential on the Eulerian grid. Two-way coupling is implemented by introducing a vorticity source term induced by the gradient of void fraction. Present simulation results are favorably compared with the measured results of bubble plume, which verifies the validity of the proposed VIC method. The rising of a single bubble cluster as well as two tandem bubble clusters are simulated. The mechanism of the aggregation effect in the rising process of bubble cluster is revealed and the transient processes of the generation, rising, strengthening, and separation of a vortex ring structure with bubble clusters are illustrated and analyzed in detail. Due to the aggregation, the average rising velocity increases with void fraction and is larger than the terminal rising velocity of single bubble. For the two tandem bubble cluster cases, the aggregation effect is stronger for smaller initial cluster distance, and both the strength of the induced vortex structure and the average bubble rising velocity are larger. For the 20 mm cluster distance case, the peak velocity of the lower cluster is about 2.7 times that of the terminal velocity of the single bubble and the peak average velocity of two clusters is about 2 times larger. While for the 30 mm cluster distance case, both the peak velocity of the lower cluster and two clusters are about 1.7 times that of the terminal velocity of the single bubble.

Raman spectroscopic detection of the T-Hg II-T base pair and the ionic characteristics of mercury.

Developing applications for metal-mediated base pairs (metallo-base-pair) has recently become a high-priority area in nucleic acid research, and physicochemical analyses are important for designing and fine-tuning molecular devices using metallo-base-pairs. In this study, we characterized the Hg(II)-mediated T-T (T-Hg(II)-T) base pair by Raman spectroscopy, which revealed the unique physical and chemical properties of Hg(II). A characteristic Raman marker band at 1586 cm(-1) was observed and assigned to the C4=O4 stretching mode. We confirmed the assignment by the isotopic shift ((18)O-labeling at O4) and density functional theory (DFT) calculations. The unusually low wavenumber of the C4=O4 stretching suggested that the bond order of the C4=O4 bond reduced from its canonical value. This reduction of the bond order can be explained if the enolate-like structure (N3=C4-O4(-)) is involved as a resonance contributor in the thymine ring of the T-Hg(II)-T pair. This resonance includes the N-Hg(II)-bonded state (Hg(II)-N3-C4=O4) and the N-Hg(II)-dissociated state (Hg(II+) N3=C4-O4(-)), and the latter contributor reduced the bond order of N-Hg(II). Consequently, the Hg(II) nucleus in the T-Hg(II)-T pair exhibited a cationic character. Natural bond orbital (NBO) analysis supports the interpretations of the Raman experiments.

Resveratrol inhibits angiogenic response of cultured endothelial F-2 cells to vascular endothelial growth factor, but not to basic fibroblast growth factor.

Resveratrol, a natural polyphenol in grapes, is known to prevent the cardiovascular diseases and to exert the antiangiogenic effect in in vivo models with vascular endothelial growth factor (VEGF) or basic fibroblast growth factor (bFGF). We examined the effect of resveratrol on tubule formation of cultured endothelial F-2 cells. In collagen gel matrix, F-2 cells formed an extended network of tubular structures in response to VEGF or bFGF. Resveratrol dose-dependently prevented the VEGF-induced tubule formation, but failed to inhibit the angiogenic response to bFGF. We next examined whether the inhibition of nitric oxide (NO) production is linked to the antiangiogenic effect of resveratrol on VEGF-stimulated F-2 cells, because NO plays a crucial role in VEGF-induced tubular network formation. NO production was increased by VEGF, but not by bFGF, and resveratrol inhibited VEGF-stimulated NO production. N(G)-nitro-L-arginine methyl ester (L-NAME) potently inhibited NO production under all conditions, including VEGF stimulation, and abrogated VEGF-induced tubule formation. However, L-NAME did not inhibit bFGF-induced tubule formation. To investigate the bFGF-induced in vivo antiangiogenic effect of resveratrol, we examined the effect of resveratrol on prostaglandin E(2) (PGE(2)) production and cyclooxygenase (COX) expression in NRK-F fibroblasts. COX-2 and its derived PGE(2) are important factors for bFGF-induced in vivo angiogenesis. Resveratrol dose-dependently prevented both COX-2 induction and PGE(2) production in bFGF-stimulated fibroblasts. These results suggest that resveratrol exerts the inhibitory effects on VEGF- and bFGF-induced angiogenesis through different mechanisms including inhibition of NO production in VEGF-stimulated endothelial cells and inhibition of COX-2 induction in bFGF-stimulated fibroblasts.

Differential effect of resveratrol on nitric oxide production in endothelial f-2 cells.

We examined the rapid effect of resveratrol on nitric oxide (NO) production in endothelial F-2 cells. During an incubation period of 10 min, resveratrol at low concentrations (<20 microM) had no effect on NO production, whereas it significantly increased NO production at high concentrations (>50 microM). In contrast, pretreatment with resveratrol at low concentrations caused a significant decrease in vascular endothelial growth factor (VEGF)-stimulated NO production. Resveratrol failed to induce phosphorylation of endothelial NO synthase (eNOS) and VEGF receptor and did not affect autophosphorylation of the VEGF receptor. However, resveratrol markedly suppressed VEGF-induced eNOS phosphorylation. Resveratrol at high concentrations reduced the viability of F-2 cells as determined by 3-(4,5-dimethyl-2-thiazoyl)-2,5-diphenyl-2H-tetrazolium bromide (MTT) and dye exclusion methods. Resveratrol-stimulated NO production was completely abolished by the depletion of extracellular Ca2+. These results indicate that resveratrol stimulates NO production by a Ca(2+)-dependent mechanism and reduces VEGF-stimulated NO production by impairing a Ca(2+)-independent mechanism in endothelial F-2 cells. However, the stimulatory effect of resveratrol may be partly attributed to its cytotoxicity.

Palladium(0)-catalyzed direct cross-coupling reaction of allylic alcohols with aryl- and alkenylboronic acids.

Allylic alcohols can be used directly for the palladium(0)-catalyzed allylation of aryl- and alkenylboronic acids with a wide variety of functional groups. A triphenylphosphine-ligated palladium catalyst turns out to be most effective for the cross-coupling reaction and its low loading (less than 1 mol%) leads to formation of the coupling product in high yield. The Lewis acidity of the organoboron reagents and poor leaving ability (high basicity) of the hydroxyl group are essential for the cross-coupling reaction. The reaction process is atom-economical and environmentally benign, because it needs neither preparation of allyl halides and esters nor addition of stoichiometric amounts of a base. Furthermore, allylic alcohols containing another unsaturated carbon-carbon bond undergo arylative cyclization reactions leading to cyclopentane formation.

Functional characterization and cloning of amino acid transporter B(0,+) (ATB(0,+)) in primary cultured rat pneumocytes.

Cationic amino acid transport in primary cultured rat pneumocytes exhibiting characteristics of alveolar epithelial type I-like cells are described. Asymmetry and activator ion dependency of (3)H-L-arginine uptake were characterized from the apical or basolateral fluid of pneumocytes grown on permeable support. Substrate specificity of transport was evaluated as a function of (3)H-L-arginine uptake inhibition in the presence of other amino acids. Transepithelial transport studies estimated (3)H-L-arginine flux in the apical-to-basolateral and basolateral-to-apical directions. Full length cDNA of rat amino acid transporter B(0,+) (rATB(0,+)) was cloned and its relative expression level studied. Results indicate that uptake of (3)H-L-arginine from apical fluid is dependent on Na(+) and Cl(-). Zwitterionic and cationic amino acids (excluding L-proline and anionic amino acids) inhibited uptake of (3)H-L-arginine from apical, but not basolateral incubation fluid. Apical-to-basolateral transepithelial flux of (3)H-L-arginine was 20x higher than basolateral-to-apical transport. Kinetic studies of (3)H-L-arginine uptake from apical fluid revealed maximal velocity (V(max)) and Michaelis-Menten constants (K(t)) of 33.32 +/- 2.12 pmol/mg protein/15 min and 0.50 +/- 0.11 mM, respectively, in a cooperative process having a coupling ratio of 1.18 +/- 0.16 with Na(+) and 1.11 +/- 0.13 with Cl(-). Expression of rATB(0,+) mRNA was identified by RT-PCR and Northern analysis. Corresponding cloned 3.2 kb rATB(0,+) cDNA sequence exhibits pronounced homology in deduced amino acid sequence to mouse (95% identity and 97% similarity) and human (89% identity and 95% similarity) ATB(0,+) homologues. We conclude that rat pneumocytes express ATB(0,+), which may partly contribute towards recovering cationic and neutral amino acids from alveolar luminal fluid.

Molecular and functional expression of multidrug resistance-associated protein-1 in primary cultured rat alveolar epithelial cells.

Multidrug resistance-associated protein-1 (MRP1) is an integral membrane efflux protein that is implicated in multidrug resistance in cancer, but it is also expressed in normal tissues. The objective of this study was to determine the expression, localization and functional activity of MRP1 in primary cultured rat alveolar epithelial cells of types I- and II cell-like phenotypes. RT-PCR data showed 550-base pair fragments in both types I- and II-like pneumocytes that exhibited 99% identity to the rat MRP1 isoform. Significant levels of MRP1 protein were detected by western analysis of immunoprecipitates in both cell types, and immunofluorescence combined with confocal laser scanning microscopy indicated basolateral localization of MRP1. Indomethacin (0-100 microM) increased fluorescein basolateral-to-apical transport, and accumulation of fluorescein in the cells, in a dose-dependent manner. We therefore conclude that the MRP1 gene is present in primary cultured rat epithelial cells of both types I- and II-like phenotypes and its corresponding protein (MRP1) is localized in the basolateral membrane of these cells. Primary cultured monolayers of rat type II-like pneumocytes appear to be a useful tool for screening MRP1 substrates designed for pulmonary delivery/targeting.

Structural and physicochemical features on the metal-mediated base pairs.

The chemical structure of the mercury-mediated T-T pair (T-Hg(I)I-T) was determined with (15)N NMR spectroscopy. In order to determine the chemical structure of the T-Hg(I)I-T pair, (15)N-(15)N J-coupling across a metal center (2JNN) was employed. Notably, this is the first observation of (2)J(NN) in a biological macromolecule (DNA duplex). This pairing mode was found to be a irregular metal ion-binding mode for DNA and RNA molecules, in which imino proton-metal exchange processes are included. Accordingly, (2)J(NN) is highly important for the determination of the chemical structures of metal-mediated base pairs.

Functional regulation of Na+-dependent neutral amino acid transporter ASCT2 by S-nitrosothiols and nitric oxide in Caco-2 cells.

We describe the regulation mechanisms of the Na(+)-dependent neutral amino acid transporter ASCT2 via nitric oxide (NO) in the human intestinal cell line, Caco-2. Exposure of Caco-2 cells to S-nitrosothiol, such as S-nitroso-N-acetyl-DL-penicillamine (SNAP) and S-nitrosoglutathione, and the NO-donor, NOC12, concentration- and time-dependently increased Na(+)-dependent alanine uptake. Kinetic analyses indicated that SNAP increases the maximal velocity (V(max)) of Na(+)-dependent alanine uptake in Caco-2 cells without affecting the Michaelis-Menten constant (K(t)). The stimulatory effect was partially eliminated by actinomycin D and cycloheximide. Increased Na(+)-dependent alanine uptake by SNAP was partially abolished by the NO scavengers, 2-(4-carboxyphenyl)-4,4,5,5-tetramethylimidazoline-1-oxyl 3-oxide sodium salt (carboxy-PTIO) and N-(dithiocarboxy)sarcosine disodium salts (DTCS), as well as the NADPH oxidase inhibitor, diphenyleneiodonium. RT-PCR revealed that Caco-2 cells expressed the Na(+)-dependent neutral amino acid transporter ASCT2, but not the other Na(+)-dependent neutral amino acid transporters ATB(0,+) and B(0)AT1. These results suggested that functional up-regulation of ASCT2 by SNAP might be partially associated with an increase in the density of transporter protein via de novo synthesis.

Analysis of transmembrane segment 7 of the dipeptide transporter hPepT1 by cysteine-scanning mutagenesis.

To investigate the involvement of transmembrane segment 7 (TMS7) of hPepT1 in forming the putative central aqueous channel through which the substrate traverses, we individually mutated each of the 21 amino acids in TMS7 to a cysteine and analyzed the mutated transporters using the scanning cysteine accessibility method. Y287C- and M292C-hPepT1 did not express at the plasma membrane. Out of the remaining 19 transporters, three (F293C-, L296C-, and F297C-hPepT1) showed negligible glycyl-sarcosine (gly-sar) uptake activity and may play an important role in defining the overall hPepT1 structure. K278C-hPepT1 showed approximately 40% activity and the 15 other transporters exhibited more than 50% gly-sar uptake when compared with wild type (WT)-hPepT1. Gly-sar uptake for the 16 active transporters containing cysteine mutations was then measured in the presence of 2.5 mM 2-aminoethyl methanethiosulfonate hydrobromide (MTSEA) or 1 mM [2-(trimethylammonium) ethyl] methanethiosulfonate bromide (MTSET). Gly-sar uptake was significantly inhibited for each of the 16 single cysteine mutants in the presence of 2.5 mM MTSEA. In contrast, significant inhibition of uptake was only observed for K278C-, M279C-, V280C-, T281C-, M284C-, L286C-, P291C-, and D298C-hPepT1 in the presence of 1 mM MTSET. MTSET modification of R282C-hPepT1 resulted in a significant increase in gly-sar uptake. To investigate this further, we mutated WT-hPepT1 to R282A-, R282E-, and R282K-hPepT1. R282E-hPepT1 showed a 43% reduction in uptake activity, whereas R282A- and R282K-hPepT1 had activities comparable with WT-hPepT1, suggesting a role for the Arg-282 positive charge in substrate translocation. Most of the amino acids that were MTSET-sensitive upon cysteine mutation, including R282C, are located toward the intracellular end of TMS7. Hence, our results suggest that TMS7 of hPepT1 is relatively solvent-accessible along most of its length but that the intracellular end of the transmembrane domain is particularly so. From a structure-function perspective, we speculate that the extracellular end of TMS7 may shift following substrate binding, providing the basis for channel opening and substrate translocation.

Biophysical evidence for His57 as a proton-binding site in the mammalian intestinal transporter hPepT1.

PURPOSE: The objective of this study was to provide direct evidence of the relative importance of the His57 residue present in transmembrane domain 2 (TMD 2) and the His121 residue in TMD 4 as proton-binding sites in human PepT1 (hPepT1) by using a novel mutagenesis approach. METHODS: His57 and His121 in hPepT1 were each mutated to alanine, arginine, or lysine individually to obtain H57A-, H57R-, H57K-, H121A-, H121R-, and H121K-hPepT1. H7A-hPepT1 was used as a negative control. [3H]Glycylsarcosine (Gly-Sar) uptake was measured 72 h posttransfection using HEK293 cells individually transfected with these mutated proteins. Steady-state I/V curves (-150 mV to +50 mV, holding potential -70 mV) were obtained by measuring 5 mM Gly-Sar-induced currents in oocytes expressing H-57R- and H57K-hPepT1. Noninjected oocytes and wild-type hPepT1 (WT-hPepT1)-injected oocytes served as negative and positive controls, respectively. RESULTS: At pH 6.0, H57K-, H57R-, H121K-, and H121R-hPepT1 led to a 97%, 90%, 45%, and 75% decrease in [3H]Gly-Sar uptake into HEK293 cells, respectively. At pH 7.4, uptake in cells transfected with H57K- and H57R-hPepT1 was not significantly different from that at pH 6.0, whereas cells expressing H121R- and H121K-hPepT1 showed 56% and 65% decrease, respectively, compared to that at pH 6.0. In oocytes expressing H57R-hPepT1, steady-state currents induced by 5 mM Gly-Sar increased with increasing pH (I(max) = 300 nA at pH 8.5), suggesting the binding of protons to H57R. No such trend was observed in oocytes injected with H57K, H121R, and H121K cRNA. CONCLUSIONS: H57R-hPepT1 is able to bind protons at a relatively basic pH, resulting in facilitation of transport of Gly-Sar by hPepT1 at higher pH. Our novel approach provides direct evidence that His57 is a principal proton-binding site in hPepT1.