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Auswahl der wissenschaftlichen Literatur zum Thema „Macrofluidic model“
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Zeitschriftenartikel zum Thema "Macrofluidic model"
Gome, Gilad, Benyamin Chak, Shadi Tawil, Dafna Shpatz, Jonathan Giron, Ilan Brajzblat, Chen Weizman, Andrey Grishko, Sharon Schlesinger und Oded Shoseyov. „Cultivation of Bovine Mesenchymal Stem Cells on Plant-Based Scaffolds in a Macrofluidic Single-Use Bioreactor for Cultured Meat“. Foods 13, Nr. 9 (28.04.2024): 1361. http://dx.doi.org/10.3390/foods13091361.
Der volle Inhalt der QuelleÇakal, Gaye Ö., İnci Eroğlu und Saim Özkar. „Simulation of continuous boric acid slurry reactors in series by microfluid and macrofluid models“. Journal of Crystal Growth 306, Nr. 1 (August 2007): 240–47. http://dx.doi.org/10.1016/j.jcrysgro.2007.04.058.
Der volle Inhalt der QuelleHilfiker, Rolf, und Hans-Friedrich Eicke. „Self-consistency of the percolation model as applied to a macrofluid-like water-in-oil microemulsion“. Journal of the Chemical Society, Faraday Transactions 1: Physical Chemistry in Condensed Phases 83, Nr. 5 (1987): 1621. http://dx.doi.org/10.1039/f19878301621.
Der volle Inhalt der QuelleVass, Sz, T. Gilányi und S. Borbély. „SANS Study of the Structure of Sodium Alkyl Sulfate Micellar Solutions in Terms of the One-Component Macrofluid Model“. Journal of Physical Chemistry B 104, Nr. 9 (März 2000): 2073–81. http://dx.doi.org/10.1021/jp9934735.
Der volle Inhalt der QuelleTIAN, FEI, WEIDONG SHI und HUA JIANG. „INNER FLOW FIELD OF POOL MIXED BY THREE SUBMERSIBLE MIXERS“. Journal of Advanced Manufacturing Systems 11, Nr. 02 (Dezember 2012): 91–97. http://dx.doi.org/10.1142/s0219686712500072.
Der volle Inhalt der QuelleOsawa, Takahiro, Wenchu Wang, Jinlu Dai und Evan T. Keller. „Macrofluidic recirculating model of skeletal metastasis“. Scientific Reports 9, Nr. 1 (18.10.2019). http://dx.doi.org/10.1038/s41598-019-50577-3.
Der volle Inhalt der QuelleCui, Jingang, Wei Jiang, Jilei Su, Jiazhen Zhang, Yongliang Yu und Yongsheng Ding. „Microfluidic-to-macrofluidic: A simple in vitro model of atherosclerosis induced by fluidic stimulation“. Biomicrofluidics 17, Nr. 4 (01.07.2023). http://dx.doi.org/10.1063/5.0155267.
Der volle Inhalt der QuelleCho, Youngkyu, Kyuhwan Na, Yesl Jun, Jihee Won, Ji Hun Yang und Seok Chung. „Three-Dimensional In Vitro Lymphangiogenesis Model in Tumor Microenvironment“. Frontiers in Bioengineering and Biotechnology 9 (04.10.2021). http://dx.doi.org/10.3389/fbioe.2021.697657.
Der volle Inhalt der QuelleKern, Axelle Y., Yevgeniy Kreinin, Lise Charle, Mark Epshtein, Netanel Korin und Pierre H. Mangin. „A macrofluidic model to investigate the intrinsic thrombogenicity of clinically used stents and develop less thrombogenic stents“. Heliyon, Februar 2024, e26550. http://dx.doi.org/10.1016/j.heliyon.2024.e26550.
Der volle Inhalt der QuelleCherubini, Marta, Scott Erickson, Prasanna Padmanaban, Per Haberkant, Frank Stein, Violeta Beltran-Sastre und Kristina Haase. „Flow in fetoplacental-like microvessels in vitro enhances perfusion, barrier function, and matrix stability“. Science Advances 9, Nr. 51 (22.12.2023). http://dx.doi.org/10.1126/sciadv.adj8540.
Der volle Inhalt der QuelleDissertationen zum Thema "Macrofluidic model"
Kern, Axelle Y. „La thrombose de stent : évaluation de l’importance de la rhéologie dans la thrombogénicité des stents et d’un nouvel agent pharmacologique dirigé contre la GPVI pour prévenir la thrombose de stent“. Electronic Thesis or Diss., Strasbourg, 2024. http://www.theses.fr/2024STRAJ027.
Der volle Inhalt der QuelleA major complication of stenting in a diseased artery is stent thrombosis, which has a particularly high mortality rate. Dual antiplatelet therapy, indicated to prevent this complication, possesses a high risk of bleeding and is not always effective. The aim of my PhD was to identify the mechanisms of stent thrombosis and to evaluate the interest of a new class of antiplatelet agents to efficiently prevent it with a low bleeding risk. The development of an original macrofluidic model has enabled us to show that the carotid stents used in clinical practice present an intrinsic thrombogenicity evidenced both at the bifurcation of a vessel where the stent meshes lie in the lumen, and around some specific places of the stent struts which are in contact with the vessel wall. The device also helped to identify a protective effect of the stent mesh, which reduces stent thrombosis. Finally, the model showed that glenzocimab, an anti-GPVI agent, is effective in preventing stent thrombosis to a similar extent than reference treatments, but with no bleeding risk
Yucel, Cakal Gaye O. „Dynamic Behavior Of Continuous Flow Stirred Slurry Reactors In Boric Acid Production“. Phd thesis, METU, 2005. http://etd.lib.metu.edu.tr/upload/12605047/index.pdf.
Der volle Inhalt der Quelles) in series system. In this reaction system there are at least three phases, one liquid and two solid phases (colemanite and gypsum). In a batch reactor all the phases have the same operating time (residence time), whereas in a continuous reactor all the phases may have different residence time distributions. The residence time of both the reactant and the product solids are very important because they affect the dissolution conversion of colemanite and the growth of gypsum crystals. The main aim of this study was to investigate the dynamic behavior of continuous flow stirred slurry reactors. By obtaining the residence time distribution of the solid and liquid components, the non-idealities in the reactors can be found. The experiments performed in the continuous flow stirred slurry reactors showed that the reactors to be used during the boric acid production experiments approached an ideal CSTR in the range of the stirring rate (500-750 rpm) studied. The steady state performance of the continuous flow stirred slurry reactors (CFSSR&rsquo
s) in series was also studied. During the studies, two colemanites having the same origin but different compositions and particle sizes were used. The boric acid production reaction consists of two simultaneous reactions, dissolution of colemanite and crystallization of gypsum. The dissolution of colemanite and the gypsum formation was followed from the boric acid and calcium ion concentrations, respectively. The effect of initial CaO/ SO42- molar ratio (1.00, 1.37 and 2.17) on the boric acid and calcium ion concentrations were searched. Also, at these initial molar ratios the colemanite feed rate was varied (5, 7.5, 10 and 15 g/min) to change the residence time of the slurry. Purity of the boric acid solution was examined in terms of the selected impurities, which were the magnesium and sulfate ion concentrations. The concentrations of them were compared at the initial molar ratios of 1.00 and 1.37 with varying colemanite feed rates. It was seen that at high initial CaO/ SO42- molar ratios the sulfate and magnesium ion concentrations decreased but the calcium ion concentration increased. The gypsum crystals formed in the reaction are in the shape of thin needles. These crystals, mixed with the insolubles coming from the mineral, are removed from the boric acid slurry by filtration. Filtration of gypsum crystals has an important role in boric acid production reaction because it affects the efficiency, purity and crystallization of boric acid. These crystals must grow to an appropriate size in the reactor. The growth process of gypsum crystals should be synchronized with the dissolution reaction. The effect of solid hold-up (0.04&ndash
0.09), defined as the volume of solid to the total volume, on the residence time of gypsum crystals was investigated and the change of the residence time (17-60 min) on the growth of the gypsum was searched. The residence time at each reactor was kept constant in each experiment as the volumes of the reactors were equal. The growth of gypsum was examined by a laser diffraction particle size analyzer and the volume weighted mean diameters of the gypsum crystals were obtained. The views of the crystals were taken under a light microscope. It was observed that the high residence time had a positive effect on the growth of gypsum crystals. The crystals had volume weighted mean diameters of even 240 µ
m. The gypsum crystal growth model was obtained by using the second order crystallization reaction rate equation. The residence time of the continuous reactors are used together with the gypsum growth model to simulate the continuous boric acid reactors with macrofluid and microfluid models. The selected residence times (20-240 min) were modeled for different number of CSTR&rsquo
s (1-8) and the PFR. The simulated models were, then verified with the experimental data. The experimentally found calcium ion concentrations checked with the concentrations found from the microfluid model. It was also calculated that the experimental data fitted the microfluid model with a deviation of 4-7%.