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Artigos de revistas sobre o tema "Self-flux"

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Autor: Grafiati

Publicado: 25 de maio de 2024

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1

Pistinner, S. L., e D. Eichler. "Self-inhibiting heat flux". Monthly Notices of the Royal Astronomical Society 301, n.º 1 (novembro de 1998): 49–58. http://dx.doi.org/10.1046/j.1365-8711.1998.01770.x.

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2

Castaño, Diego J., e Teresa M. Castaño. "Self-inductance and magnetic flux". American Journal of Physics 91, n.º 8 (1 de agosto de 2023): 622–28. http://dx.doi.org/10.1119/5.0098417.

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The canonical equation for self-inductance involving magnetic flux is examined, and a more general form is presented that can be applied to continuous current distributions. We attempt to clarify and extend the use of the standard equation by recasting it in its more versatile form.

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3

Morel, J. E., e J. M. McGhee. "A Self-Adjoint Angular Flux Equation". Nuclear Science and Engineering 132, n.º 3 (julho de 1999): 312–25. http://dx.doi.org/10.13182/nse132-312.

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4

Lukin, Vyacheslav S. "Self-organization in magnetic flux ropes". Plasma Physics and Controlled Fusion 56, n.º 6 (10 de março de 2014): 060301. http://dx.doi.org/10.1088/0741-3335/56/6/060301.

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5

Ga, E. M., D. Son, J. G. Bak e S. G. Lee. "Drift Self-compensating Type Flux-meter for Automatic Magnetic Flux Measurement". Journal of Magnetics 8, n.º 4 (1 de dezembro de 2003): 160–63. http://dx.doi.org/10.4283/jmag.2003.8.4.160.

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6

Mints, R. G., e Ilya Papiashvili. "Self-generated magnetic flux inYBa2Cu3O7−xgrain boundaries". Physical Review B 62, n.º 22 (1 de dezembro de 2000): 15214–20. http://dx.doi.org/10.1103/physrevb.62.15214.

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7

Cademartiri, Ludovico, Alessandra Sutti, Gianluca Calestani, Chiara Dionigi, Petr Nozar e Andrea Migliori. "Flux-Assisted Self-Assembly of Monodisperse Colloids". Langmuir 19, n.º 19 (setembro de 2003): 7944–47. http://dx.doi.org/10.1021/la034485r.

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8

Zhou, Pengbo, Guangtong Ma, Yuke Deng, Xingchao Nie, Yao Zhai, Kang Liu, Han Zhang e Yongjian Li. "A Contactless Self-Regulating HTS Flux Pump". IEEE Transactions on Applied Superconductivity 30, n.º 4 (junho de 2020): 1–6. http://dx.doi.org/10.1109/tasc.2020.2978787.

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9

Okada, Yohji, Masashi Kitagou, Toru Masuzawa e Masato Enokizono. "Development of Flux Concentrated type Self-Bearing Motor". IFAC Proceedings Volumes 43, n.º 18 (2010): 461–66. http://dx.doi.org/10.3182/20100913-3-us-2015.00010.

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10

Pla, Oscar, e Franco Nori. "Self-Organized Critical Behavior in Pinned Flux Lattices". Physical Review Letters 67, n.º 7 (12 de agosto de 1991): 919–22. http://dx.doi.org/10.1103/physrevlett.67.919.

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11

Setina, Emily. "Marianne Moore, Photography, and the Self-in-Flux". English Language Notes 44, n.º 2 (1 de setembro de 2006): 275–82. http://dx.doi.org/10.1215/00138282-44.2.275.

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12

Krasnyuk, I. B., e R. M. Taranets. "Self-similar distribution in “giant” magnetic flux creep". Technical Physics 52, n.º 10 (outubro de 2007): 1247–51. http://dx.doi.org/10.1134/s1063784207100015.

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13

Riedel, K. S. "Flux coordinates, self-consistent equilibria, and variational principle". Physics of Fluids 31, n.º 4 (1988): 890. http://dx.doi.org/10.1063/1.866771.

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14

Peets, D. C., Ruixing Liang, Mati Raudsepp, D. A. Bonn e W. N. Hardy. "Self-flux growth of single-crystalline Tl2Ba2CuO6+x". Physica C: Superconductivity 460-462 (setembro de 2007): 1335–36. http://dx.doi.org/10.1016/j.physc.2007.04.014.

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15

Hashimoto, Shinobu, Kentaro Hattori, Koji Inoue, Ayuka Nakahashi, Sawao Honda e Yuji Iwamoto. "Self-flux synthesis and photoluminescent properties of LiAl5O8". Materials Research Bulletin 44, n.º 1 (janeiro de 2009): 70–73. http://dx.doi.org/10.1016/j.materresbull.2008.04.003.

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16

Ivić, Zoran, Nikos Lazarides e G. P. Tsironis. "Self-induced transparency in a flux-qubit chain". Chaos, Solitons & Fractals: X 1 (março de 2019): 100003. http://dx.doi.org/10.1016/j.csfx.2019.100003.

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17

Cao, Chongde, Wolfgang Löser, Günter Behr, Rüdiger Klingeler, Norman Leps, Hartmut Vinzelberg e Bernd Büchner. "Self-flux growth of large EuCu2Si2 single crystals". Journal of Crystal Growth 318, n.º 1 (março de 2011): 1043–47. http://dx.doi.org/10.1016/j.jcrysgro.2010.10.197.

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18

Naumov, N. D. "Self-consistent description of charged-particle flux catastrophes". Doklady Physics 49, n.º 9 (setembro de 2004): 508–11. http://dx.doi.org/10.1134/1.1810574.

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19

Wegrzyn, J. "Self‐shielding, non‐fluoride containing, flux‐cored wires". Welding International 10, n.º 5 (janeiro de 1996): 341–45. http://dx.doi.org/10.1080/09507119609549007.

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20

Kumar, Ravi, S. K. Malik, S. P. Pai, P. R. Apte, R. Pinto, R. Vijayaraghavan e Dhanajay Kumar. "Self-field-induced flux creep inYBa2Cu3O7−ythin films". Physical Review B 46, n.º 9 (1 de setembro de 1992): 5766–68. http://dx.doi.org/10.1103/physrevb.46.5766.

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21

Tripp, Steven L., Rafal E. Dunin-Borkowski e Alexander Wei. "Flux Closure in Self-Assembled Cobalt Nanoparticle Rings". Angewandte Chemie International Edition 42, n.º 45 (24 de novembro de 2003): 5591–93. http://dx.doi.org/10.1002/anie.200352825.

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22

Tripp, Steven L., Rafal E. Dunin-Borkowski e Alexander Wei. "Flux Closure in Self-Assembled Cobalt Nanoparticle Rings". Angewandte Chemie 115, n.º 45 (24 de novembro de 2003): 5749–51. http://dx.doi.org/10.1002/ange.200352825.

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23

KIM, KYUN TAK, e YEONG SIK KIM. "EFFECTS OF COUNTERPART MATERIALS ON WEAR BEHAVIOR OF THERMALLY SPRAYED Ni-BASED SELF-FLUX ALLOY COATINGS". International Journal of Modern Physics B 24, n.º 15n16 (30 de junho de 2010): 3023–28. http://dx.doi.org/10.1142/s0217979210066021.

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This study aims at investigating the wear behavior of thermally sprayed Ni -based self-flux alloy coatings against different counterparts. Ni -based self-flux alloy powders were flame-sprayed onto a carbon steel substrate and then heat-treated at temperature of 1000 °C. Dry sliding wear tests were performed using the sliding speeds of 0.2 and 0.8 m/s and the applied loads of 5 and 20 N. AISI 52100, Al 2 O 3, Si 3 N 4 and ZrO 2 balls were used as counterpart materials. Wear behavior of Ni -based self-flux alloy coatings against different counterparts were studied using a scanning electron microscope(SEM) and energy dispersive X-ray spectroscopy (EDX). It was revealed that wear behavior of Ni -based self-flux alloy coatings were much influenced by counterpart materials.

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24

Kim, Yeong Sik, e Kyun Tak Kim. "Effect of Sliding Speed and Applied Load on the Wear Behavior of Thermally Sprayed Ni-Based Self-Flux Alloy Coating". Key Engineering Materials 353-358 (setembro de 2007): 840–43. http://dx.doi.org/10.4028/www.scientific.net/kem.353-358.840.

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This study aims at investigating the effect of the sliding speed and the applied load on the dry sliding wear behavior of thermally sprayed Ni-based self-flux alloy coating. Ni-based self-flux alloy powders were flame-sprayed onto a carbon steel substrate and then these coatings were heat-treated at temperature of 1000 oC. Dry sliding wear tests were performed using the sliding speeds of 0.2, 0.4, 0.6 and 0.8 m/s and the applied loads of 5, 10, 15 and 20 N. AISI 52100 ball (diameter 8 mm) was used as counterpart material. Wear behavior of Ni-based self-flux alloy coatings was studied using a scanning electron microscope (SEM) and energy dispersive X-ray spectroscopy (EDX). It was revealed that microstructure and wear behavior of the Ni-based self-flux alloy coatings were much influenced by the sliding speed and the applied load.

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25

Yamazaki, Masato, Takashi Kasashima, Katsuya Yamagiwa, Takeshi Mitsuoka e Kazushige Ohbayashi. "Characteristic Design of Microwave Dielectric Materials by Using Self-Flux Compositions". Key Engineering Materials 301 (janeiro de 2006): 109–12. http://dx.doi.org/10.4028/www.scientific.net/kem.301.109.

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In order to improve the sinterability and controllability of dielectric properties, we focused on self-flux composition. In the case of Ba(Mg1/3Nb2/3)O3, we selected Ba(1-b)NbbOd as self-flux system and investigated correlations between Q-factor and the b value. Interestingly, high Q-value was obtained only at the b=0.45. Moreover, the dielectric constant and tf change linearly by the quantity of Ba0.55Nb0.45Od under keeping up high-Q value. As a result, it was indicated that the dielectric properties could be controlled by the assumption of stoichiometric composition and liquid phase consisted by self-flux.

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26

Zhang, Shulong, Mingtao Li, Yilun Yang, Chengchun Zhao, Mingzhu He, Yin Hang e Yifei Fang. "Effects of the initial flux ratio on CeSb2 crystal growth by a self-flux method". CrystEngComm 23, n.º 29 (2021): 5045–52. http://dx.doi.org/10.1039/d1ce00557j.

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Self-flux growth of the single crystal CeSb₂ was studied in detail, and the most suitable growth parameters of CeSb₂ were obtained. The unusual magnetoresistance properties of CeSb₂ were observed and discussed.

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27

Chen, Jia, Jiafan Ye, Guoqing Gou e Wei Gao. "Rare earth elements in self-shielded flux-cored wires and their effect on the weld toughing of U75V rail steel". International Journal of Modern Physics B 34, n.º 01n03 (30 de dezembro de 2019): 2040054. http://dx.doi.org/10.1142/s0217979220400548.

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Self-shielded flux-cored wire is a new type of welding material that has the advantages of outdoor and high-efficiency application, and it has been used widely for rail repair. A self-shielded flux-cored wire with high alkalinity and rare earth elements was taken for research, and the microstructure, inclusions, hardness and the impact toughness were studied. Rare earth elements could eliminate the oxygen and sulfur when they were added into the molten pool. The addition amount has been optimized to the range of 4% in the self-shielded flux-cored wire when used for rail repairing.

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28

Zhai, Yao, Pengbo Zhou, Jing Li, Chenzhen Sun, Yuxiao Li, Ling Xiao, Yuke Deng e Guangtong Ma. "Performance Investigation of Contactless Self-Regulating HTS Flux Pump". IEEE Transactions on Applied Superconductivity 31, n.º 5 (agosto de 2021): 1–5. http://dx.doi.org/10.1109/tasc.2021.3073531.

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29

XU ZHENG, ZHAO XIAO-RU, WU WEN-BIN, SUN XUE-FENG, ZHOU GUI-EN, LI XIAO-GUANG e ZHANG YU-HENG. "GROWTH CHARACTERISTICS OF Bi2Sr2CaCu2Oy SINGLE CRYSTALS USING SELF-FLUX". Acta Physica Sinica 45, n.º 9 (1996): 1562. http://dx.doi.org/10.7498/aps.45.1562.

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30

Rudner, Mark S., e Justin C. W. Song. "Self-induced Berry flux and spontaneous non-equilibrium magnetism". Nature Physics 15, n.º 10 (8 de julho de 2019): 1017–21. http://dx.doi.org/10.1038/s41567-019-0578-5.

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31

Krasnyuk, I. B. "Self-similar magnetic structures and magnetic flux “Giant” creep". Technical Physics 52, n.º 5 (maio de 2007): 565–70. http://dx.doi.org/10.1134/s1063784207050052.

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32

Komatsu-Hidaka, Chiharu, e Takeo Takizawa. "Single crystal growth of SrGa2S4by the self-flux method". Japanese Journal of Applied Physics 39, S1 (1 de janeiro de 2000): 67. http://dx.doi.org/10.7567/jjaps.39s1.67.

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33

Szyndler, Megan W., e Robert M. Corn. "Self-Assembly of Flux-Closure Polygons from Magnetite Nanocubes". Journal of Physical Chemistry Letters 3, n.º 17 (10 de agosto de 2012): 2320–25. http://dx.doi.org/10.1021/jz300931s.

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34

Wen, L. C., H. Y. Hsieh, S. C. Chang, M. Y. Lin, Y. H. Lee, W. P. Su, H. C. I. Kao et al. "Compact Li-doped Gd2Ti2O7 prepared with LiO0.5 self-flux". Materials Research Bulletin 50 (fevereiro de 2014): 297–302. http://dx.doi.org/10.1016/j.materresbull.2013.10.050.

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35

Bilal, Adel, Jean-Pierre Derendinger e Konstadinos Sfetsos. "(Weak) G2 holonomy from self-duality, flux and supersymmetry". Nuclear Physics B 628, n.º 1-2 (abril de 2002): 112–32. http://dx.doi.org/10.1016/s0550-3213(02)00042-1.

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36

Kannan, C. V., S. Ganesamoorthy, D. Rajesh, R. Jayavel e H. Kimura. "Anisotropic properties of self-flux grown LiB3O5 single crystals". Solid State Communications 136, n.º 4 (janeiro de 2005): 215–19. http://dx.doi.org/10.1016/j.ssc.2005.07.028.

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37

Machida, Akio, Naomi Nagasawa, Takaaki Ami e Masayuki Suzuki. "Ferroelectricity ofBi2SrTa2O9Single Crystals Grown by the Self-Flux Method". Japanese Journal of Applied Physics 36, Part 1, No. 12A (15 de dezembro de 1997): 7267–71. http://dx.doi.org/10.1143/jjap.36.7267.

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38

Burtsev, V. A., e N. V. Kalinin. "Self-pressed radiating theta discharge with trapped magnetic flux". Plasma Devices and Operations 15, n.º 2 (junho de 2007): 147–58. http://dx.doi.org/10.1080/10519990701322807.

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39

Zhang, Haowei, e Haisheng Fang. "Flux synthesis of LiNi0.5Co0.2Mn0.3O2 via in situ self-oxygenation". Ionics 26, n.º 6 (24 de abril de 2020): 3185–92. http://dx.doi.org/10.1007/s11581-020-03576-8.

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40

Kannan, C. V., S. Ganesamoorthy, C. Subramanian e P. Ramasamy. "Dielectric properties of self-flux-grown RbTiOPO4 single crystals". physica status solidi (a) 196, n.º 2 (abril de 2003): 465–70. http://dx.doi.org/10.1002/pssa.200305941.

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41

Kliem, B., e N. Seehafer. "Helicity shedding by flux rope ejection". Astronomy & Astrophysics 659 (março de 2022): A49. http://dx.doi.org/10.1051/0004-6361/202142422.

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Context. We quantitatively address the conjecture that magnetic helicity must be shed from the Sun by eruptions launching coronal mass ejections in order to limit its accumulation in each hemisphere. Aims. By varying the ratio of guide and strapping field and the flux rope twist in a parametric simulation study of flux rope ejection from approximately marginally stable force-free equilibria, different ratios of self- and mutual helicity are set and the onset of the torus or helical kink instability is obtained. Methods. The helicity shed is found to vary over a broad range from a minor to a major part of the initial helicity, with self helicity being largely or completely shed and mutual helicity, which makes up the larger part of the initial helicity, being shed only partly. Torus-unstable configurations with subcritical twist and without a guide field shed up to about two-thirds of the initial helicity, while a highly twisted, kink-unstable configuration sheds only about one-quarter. The parametric study also yields stable force-free flux rope equilibria up to a total flux-normalized helicity of 0.25, with a ratio of self- to total helicity of 0.32 and a ratio of flux rope to external poloidal flux of 0.94. Results. These results numerically demonstrate the conjecture of helicity shedding by coronal mass ejections and provide a first account of its parametric dependence. Both self- and mutual helicity are shed significantly; this reduces the total initial helicity by a fraction of ∼0.4 − 0.65 for typical source region parameters.

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42

Ramírez, J., e J. R. Sanmartín. "Self-similar expansion of laser plasmas with nonlocal heat flux". Laser and Particle Beams 12, n.º 1 (março de 1994): 55–64. http://dx.doi.org/10.1017/s0263034600007229.

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A previous hydrodynamic model of the expansion of a laser-produced plasma, using classical (Spitzer) heat flux, is reconsidered with a nonlocal heat flux model. The nonlocal law is shown to be valid beyond the range of validity of the classical law, breaking down ultimately, however, in agreement with recent predictions.

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43

Groza, A. D. "p-polarized nonlinear surface polaritons near the surface of an epsilon-near-zero metamaterial with saturable permittivity". Journal of Nonlinear Optical Physics & Materials 24, n.º 02 (junho de 2015): 1550015. http://dx.doi.org/10.1142/s0218863515500150.

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We study p-polarized nonlinear surface polaritons (NLSP) propagating along the interface of an epsilon-near-zero metamaterial with saturable nonlinearity, very small negative linear permittivity and an optically linear medium. On the basis of the exact solution of Maxwell's equations, we investigate the relationship between the NLSP propagation constant and the NLSP energy flux for self-focusing and self-defocusing cases. In both cases, for the chosen value of propagation constant, calculations due to Kerr model lead to the lowest NLSP energy flux compared with the energy flux for metamaterial with saturable permittivity.

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44

Yang, Shuhong, Jun Zhang, Ting Li e Yang Liu. "Self-cancellation of solar ephemeral regions observed by SDO". Proceedings of the International Astronomical Union 8, S294 (agosto de 2012): 159–60. http://dx.doi.org/10.1017/s1743921313002433.

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AbstractWe study the ephemeral regions (ERs) in the quiet Sun observed by the Solar Dynamics Observatory, and find that they can be classified into two types: normal ERs (NERs) and self-cancelled ERs (SERs). We identify 2988 ERs among which there are 190 SERs, about 6.4% of the ERs. The total self-cancelled flux is 9.8% of the total ER flux. We suggest that the self-cancellation of SERs is caused by the submergence of magnetic loops connecting the dipolar patches, without magnetic energy release.

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45

Lancia, L., C. Fourment, J. Fuchs, J. L. Feugeas, Ph Nicolai, S. Bastiani-Ceccotti, M. Gauthier et al. "Simultaneous measurement of self-generated magnetic fields and electron heat transport in dense plasma". Laser and Particle Beams 31, n.º 4 (4 de setembro de 2013): 653–61. http://dx.doi.org/10.1017/s0263034613000451.

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AbstractThe role of self generated magnetic fields in the transport of a heat wave following a nanosecond laser irradiation of a solid target is investigated. Magnetic fields are expected to localize the electron carrying the heat flux but at the same time are affected in their evolution by the heat flux itself. We performed simultaneous measurements of heat wave propagation velocity within the target and magnetic fields developing on the target surface. These were compared to results obtained by numerical magneto-hydrodynamic modeling, including self-generated B fields. The comparison shows that longitudinal heat flow is overestimated in the simulations. Similarly, but most notably, the radial expansion of the magnetic fields is underestimated by the modeling. The two are likely linked, the more pronounced radial drift of B-fields induces a rotation of heat flux in the radial direction, and corresponding longitudinal heat flux inhibition. This suggests the need for improving present modeling of self-generated magnetic fields evolution in high power laser-matter interaction.

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46

Yashiro, Nobuyoshi, Kazuhiko Kusunoki, Kazuhito Kamei, Mitsuhiro Hasebe, Toru Ujihara e Kazuo Nakajima. "Growth of SiC Single Crystal from Si-C-(Co, Fe) Ternary Solution". Materials Science Forum 527-529 (outubro de 2006): 115–18. http://dx.doi.org/10.4028/www.scientific.net/msf.527-529.115.

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We carried out the growth of single crystalline silicon carbide (SiC) from Si-C-X (X= Co, Fe) ternary solutions. These ternary solutions are expected to show large carbon solubility compared with Si solvent (self-flux) by means of CALPHAD (CALculation of PHAse Diagrams) method. We investigated the growth rate and the polytype of the grown crystal from the ternary solutions. Then we found that the growth rate from the ternary solutions is much larger than that from the self-flux. The growth rate from Si-C-Co (Si-C-Fe) system was about 6mm/hr (12mm/hr) while that from the self-flux was only 2mm/hr. The grown crystal from the ternary solutions is classified into 6H that takes over the seed polytype.

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47

Baggio, Bruno, Giovanni Marzaro, Giovanni Gambaro, Francesco Marchini, Hibbard E. Williams e Arturo Borsatti. "Glycosaminoglycan Content, Oxalate Self-Exchange and Protein Phosphorylation in Erythrocytes of Patients with ‘Idiopathic’ Calcium Oxalate Nephrolithiasis". Clinical Science 79, n.º 2 (1 de agosto de 1990): 113–16. http://dx.doi.org/10.1042/cs0790113.

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1. This study was performed to test the hypothesis that glycosaminoglycans may play an important role in the observed abnormalities in oxalate flux seen in patients with calcium oxalate nephrolithiasis. 2. Oxalate flux rate, erythrocyte membrane glycosaminoglycan content, membrane protein phosphorylation and effect of heparan sulphate on erythrocyte oxalate flux in vitro were studied in control subjects and patients with calcium oxalate nephrolithiasis. 3. In comparison with control subjects, renal stone-formers showed a significantly higher oxalate self-exchange, a lower erythrocyte membrane glycosaminoglycan content and a higher membrane phosphorylation rate. In stone-formers, erythrocyte glycosaminoglycan content correlated inversely with both oxalate flux rate and protein phosphorylation. In vitro, heparan sulphate promoted a significant fall in the rate of oxalate self-exchange. 4. These findings support the hypothesis that a lower erythrocyte membrane content of glycosaminoglycans enhances membrane protein phosphorylation, leading to an increased rate of transmembrane oxalate flux.

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48

Kotelchuk, A. S. "Influence of thermophysical properties of cores of self-shielding flux-cored wires on welding and technological properties". Paton Welding Journal 2016, n.º 1 (28 de janeiro de 2016): 30–34. http://dx.doi.org/10.15407/tpwj2016.01.04.

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49

Strutynska, N. Yu. "Interaction in self-flux of systems MI2O-P2O5-TiO2-MIIO (MI - Rb, Rb/K, MII - Cu, Zn)". Functional materials 22, n.º 2 (30 de junho de 2015): 269–73. http://dx.doi.org/10.15407/fm22.02.269.

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50

Zhang, Ming Liang, Yong Lu e Dong Gao. "Study on Flux-Pinned Interaction between High-Temperature Superconductor and Permanent Magnet and Flux-Pinning’s Self-Stability". Advanced Materials Research 291-294 (julho de 2011): 1251–54. http://dx.doi.org/10.4028/www.scientific.net/amr.291-294.1251.

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Resumo:

Flux pinned effect (FPE) takes place in high-temperature superconductors (HTSC) when being cooled below critical temperature in magnetic field and appears the self-stable with resisting the disturbing and recovering the initial equilibrium position , even in the failure of control, which is ideal for the activities of spacecraft. In order to investigate the special phenomenon, the image-dipole model (IDM) for interaction and spring-damper model (SDM) for system are adopted in this paper. IDM are based on two assumed images and SDM linked with flux-pinned interface is based on virtual spring and damper. Two models effectively deal with the flux-pinning and give some clear expressions. When moving along single orient, this paper demonstrates the pairs’ self-stability based on two models.

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