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Shinpei Shibata, Shota Kisaka Monthly Notices of the Royal Astronomical Society 507 (1), 1055-1063, 2021-08-02

...This means that the length of the lever arm of the angular momentum extracted by the photons, relativistic particles, and wind must be on average c/Ω*, which is known as the light cylinder radius....

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Damir D. Dzhafarov, Ludovic Patey Computability 10 (2), 111-121, 2021-04-16

...<jats:p>We prove the following result: there is a family R = ⟨ R 0 , R 1 , … ⟩ of subsets of ω such that for every stable coloring c : [ ω ] 2 → k hyperarithmetical in R and every finite collection of...

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Shuang-Lan Wu, Atsushi Nozu, Yosuke Nagasaka Bulletin of the Seismological Society of America 111 (1), 309-320, 2020-10-13

...For the imaginary part of the complex frequency, ωc=ω−λi, λ=ξπ/Tw with ξ≥2.0 can be recommended, with the understanding that the waveforms are effective only within the range of [0,Tw/ξ]....

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D. H. Ping, H. P. Xiang, H. Chen, L. L. Guo, K. Gao, X. Lu Scientific Reports 10 (1), 6081-, 2020-04-08

...In this study, a new metastable carbide formation mechanism was proposed as ω-Fe<jats:sub>3</jats:sub>C → ω′-Fe<jats:sub>3</jats:sub>C → θ′-Fe<jats:sub>3</jats:sub>C based on the transmission electron...

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Pawan Kumar, Željka Bošnjak Monthly Notices of the Royal Astronomical Society 494 (2), 2385-2395, 2020-03-20

...The counter-streaming pairs are subject to two-stream instability, which leads to formation of particle bunches of size of the order of c/ωp, where ωp is the plasma frequency....

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Ramandeep Gill, Jonathan Granot Monthly Notices of the Royal Astronomical Society 491 (4), 5815-5825, 2019-11-28

...Current 2D/3D particle-in-cell simulations are limited to short time-scales and box sizes ≲104(c/ωp) ≪ R/Γsh much smaller than the shocked region’s comoving width, and hence cannot probe the asymptotic...

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Hasegawa, Takemitsu, Sugiura, Hiroshi Journal of Computational and Applied Mathematics 358 327-342, 2019-10-01

...Interpolating f by a polynomial pn of degree n and expanding in terms of the Chebyshev polynomials with O(n log n) operations by the FFT, we obtain an approximation Q(pn;c,ω) ≅ Q(f;c,ω)....

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D. H. Ping, H. P. Xiang, X. Liu, X. Ji, S. J. Li, X. Lu Journal of Applied Physics 125 (17), 175112-, 2019-05-06

...2abcc, cω=3/2abcc)....

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D. H. Ping, H. P. Xiang Journal of Applied Physics 125 (4), 045105-, 2019-01-25

...The ω-Fe lattice parameters are dependent on their corresponding body centered cubic (BCC) phase (aω=2abcc,cω=3/2abcc)....

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Fuchiwaki, O., Tanaka, Y., Notsu, H., Hyakutake, T. Microfluidics and Nanofluidics 22 (8), 80-, 2018-08

...We define Reynolds number, R_e, as ar_cω/ν, where a is half of the oscillation's amplitude, r_c is the cylinder's radius, ω is the oscillation's angular frequency, and ν is the kinematic viscosity....

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Peter Kurzweil, Mikhail Shamonin Batteries 4 (3), 35-, 2018-08-01

...<jats:p>Frequency-dependent capacitance C(ω) is a rapid and reliable method for the determination of the state-of-charge (SoC) of electrochemical storage devices....

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Zhi-Gang Wang, Jun-Xia Zhang The European Physical Journal C 78 (6), 503-, 2018-06

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Glòria Montaña, Albert Feijoo, Àngels Ramos The European Physical Journal A 54 (4), 64-, 2018-04

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J. Nieves, R. Pavao, L. Tolos The European Physical Journal C 78 (2), 114-, 2018-02

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Garima Joshi, G. Ravi, S. Mukherjee Physics of Plasmas 24 (12), 2017-12-01

...., the skin depth (∼c/ωpe), rather than being oblique as predicted by theory and observed in other experiments. The wave shows a feeble resonance cone at an angle of ∼10° but no obliqueness....

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Neeraj Jain, A. Surjalal Sharma Physics of Plasmas 22 (10), 2015-10-01

...A numerical linear eigen value analysis of the EMHD tearing mode, valid for current sheet half-thicknesses ranging from ϵ&lt;de=c/ωpe (strong electron inertia) to ϵ&gt;de (weak electron inertia), is presented...

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Claudio Curti, Andrea Sartori, Lucia Battistini, Nicoletta Brindani, Gloria Rassu, Giorgio Pelosi, Alessio Lodola, Marco Mor, Giovanni Casiraghi, Franca Zanardi Chemistry – A European Journal 21 (17), 6433-6442, 2015-03-03

...Analysis of the <jats:sup>13</jats:sup>C NMR chemical shifts of the C‐ω remote site within homologous silyloxyindole donors enabled rationalization of the results and easy qualitative prediction of the...

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Madan Junghare, Bernhard Schink International Journal of Systematic and Evolutionary Microbiology 65 (Pt_1), 77-84, 2015-01-01

...The major fatty acids were C<jats:sub>16 : 0</jats:sub>, C<jats:sub>16 : 1</jats:sub>ω7c/ω6c and C<jats:sub>18 : 1</jats:sub>ω7c....

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Jürgen E. K. Schawe The Journal of Chemical Physics 141 (18), 184905-, 2014-11-14

...The relation between cooling rate, βc, and frequency, ω, is usually described by the Frenkel-Kobeko-Reiner-(FKR) hypothesis βc/ω = C, where C is a constant....

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S. V. Lebedev, L. Suttle, G. F. Swadling, M. Bennett, S. N. Bland, G. C. Burdiak, D. Burgess, J. P. Chittenden, A. Ciardi, A. Clemens, P. de Grouchy, G. N. Hall, J. D. Hare, N. Kalmoni, N. Niasse, S. Patankar, L. Sheng, R. A. Smith, F. Suzuki-Vidal, J. Yuan, A. Frank, E. G. Blackman, R. P. Drake Physics of Plasmas 21 (5), 2014-05-01

...ωpi from the obstacle....

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J. Jara-Almonte, W. Daughton, H. Ji Physics of Plasmas 21 (3), 032114-, 2014-03-01

...ωpe....

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M. Zhou, X. H. Deng, Y. Pang, S. Y. Huang, Z. G. Yuan, H. M. Li, X. J. Xu, Y. H. Wang, M. Yao, D. D. Wang Physics of Plasmas 19 (7), 072907-, 2012-07-01

...Approaching the neutral sheet, ion frozen-in condition is broken in a narrow region (∼c/ωpi) at the edge of a density cavity, while electrons are frozen-in to magnetic fields....

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H. S. Fu, Y. V. Khotyaintsev, A. Vaivads, M. André, S. Y. Huang Geophysical Research Letters 39 (6), 2012-03-27

...<jats:p>Using Cluster data, we investigate the electric structure of a dipolarization front (DF) – the ion inertial length (<jats:italic>c/ω</jats:italic><jats:sub><jats:italic>pi</jats:italic></jats:sub...

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J. S. Ross, S. H. Glenzer, P. Amendt, R. Berger, L. Divol, N. L. Kugland, O. L. Landen, C. Plechaty, B. Remington, D. Ryutov, W. Rozmus, D. H. Froula, G. Fiksel, C. Sorce, Y. Kuramitsu, T. Morita, Y. Sakawa, H. Takabe, R. P. Drake, M. Grosskopf, C. Kuranz, G. Gregori, J. Meinecke, C. D. Murphy, M. Koenig, A. Pelka, A. Ravasio, T. Vinci, E. Liang, R. Presura, A. Spitkovsky, F. Miniati, H.-S. Park Physics of Plasmas 19 (5), 056501-, 2012-03-21

...With c/ωpi≪ℓint≪λmfp, we are in a regime where collisionless shock formation is possible.</jats:p>...

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S. D. Baalrud, A. Bhattacharjee, Y.-M. Huang, K. Germaschewski Physics of Plasmas 18 (9), 092108-, 2011-09-01

...Plasmas 14, 100703 (2007)] arise when collisions are sufficiently weak that dη is shorter than the ion skin depth di ≡ c/ωpi....

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Edward A. Startsev, Ronald C. Davidson, Mikhail Dorf Physics of Plasmas 16 (9), 092101-1-8-, 2009-09-01

...ωpe is the collisionless skin depth and ωpe is the electron plasma frequency....

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Shinji Saito, S. Peter Gary, Hui Li, Yasuhito Narita Physics of Plasmas 15 (10), 102305-, 2008-10-01

...The simulations represent decaying turbulence, in which an initial, narrowband spectrum of fluctuations at wavenumbers kc∕ωe≃0.1 cascades toward increased damping at kc∕ωe≃1.0, where c∕ωe is the electron...

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Eun-Hwa Kim, Iver H. Cairns, Peter A. Robinson Physics of Plasmas 15 (10), 2008-10-01

...Our results include: (1) both o- and x-mode waves are produced for Ω=(ωL∕c)1∕3(ωc∕ω)≲1, contrary to previous ideas. Only the o mode is produced for Ω≳1.5....

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Yang Ren, Masaaki Yamada, Hantao Ji, Seth Dorfman, Stefan P. Gerhardt, Russel Kulsrud Physics of Plasmas 15 (8), 082113-, 2008-08-01

...The width of the electron diffusion region scales with the electron skin depth (∼5.5–7.5c∕ωpe) and the peak electron outflow velocity scales with the electron Alfvén velocity (∼0.12–0.16VeA), independent...

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KAWAKAMI Tomohiro Bulletin of the Faculty of Education, Wakayama University. Natural science 58 9-18, 2008-02-29

...We prove that if M. admits the C^ω (resp. C^∞) cell decomposition or 0 ≤ r < ∞, then the orbit map π : G → G...

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C. Dames ASME 2008 First International Conference on Micro/Nanoscale Heat Transfer, Parts A and B 2008-01-01

...<jats:p>The thermal conductivity is modeled with a spectral form of kinetic theory k=13∫CωνLdω(1) where ω is the angular frequency, Cω is the specific heat per unit frequency, ν = ∂ω/∂q is the group velocity...

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Danchev Peter V. SUT Journal of Mathematics 44 (1), 33-37, 2008

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N. Bian, G. Vekstein Physics of Plasmas 14 (7), 072107-, 2007-07-01

...Here, β is a standard plasma thermal pressure parameter, while di≡c∕(ωpil) is the normalized ion inertial skin depth, with l being the shear length of the magnetic field....

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杉崎 竜哉, 田辺 誠, 出浦 智之, 奥田 広之 設計工学・システム部門講演会講演論文集 2007.17 (0), 234-237, 2007

...For a block structure the transfer matrix C(ω) at frequency co from the nodal velocity vector to acoustic pressure vector on the boundary surface is obtained by using BEM....

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宮崎 武文 日本生理学会大会発表要旨集 2007 (0), 152-152, 2007

...In order to get some more evidences on this hypothesis, I analyzed the effects of Calphostin C (1 μM), an inhibitor of protein kinase C, ω-Conotoxin GVIA (1 μM), a selective N-type Ca<SUP>2+</SUP> channel...

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G. Vekstein, N. H. Bian Physics of Plasmas 13 (12), 122105-, 2006-12-01

...Here, c∕ωpi is the ion inertial skin depth, a is the width of the plasma slab, and S≫1 is the Lundquist number of a highly conducting plasma....

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A. Bret, M. E. Dieckmann, C. Deutsch Physics of Plasmas 13 (8), 2006-08-01

...For high beam densities, highly unstable oblique modes dominate the spectrum of unstable waves as long as ωc∕ωp≲2γb3∕2, where ωc is the electron gyrofrequency, ωp is the electron plasma frequency, and...

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J. R. Wygant, C. A. Cattell, R. Lysak, Y. Song, J. Dombeck, J. McFadden, F. S. Mozer, C. W. Carlson, G. Parks, E. A. Lucek, A. Balogh, M. Andre, H. Reme, M. Hesse, C. Mouikis Journal of Geophysical Research: Space Physics 110 (A9), A09206-, 2005-09

...The thinnest current sheet observed during this interval was bifurcated into a pair of current sheets and the measured width of the individual current sheet was 60–100 km (3–5 c/ω<jats:sub>pe</jats:sub...

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Gavin Bierman, Erik Meijer, Wolfram Schulte ECOOP 2005 - Object-Oriented Programming 287-311, 2005

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Dwaipayan Chakrabarti, Biman Bagchi The Journal of Chemical Physics 122 (1), 014501-, 2004-12-13

...We here investigate a kinetic model of cooperative dynamics within the landscape paradigm for the dynamic heat capacity C(ω,T) behavior....

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S. N. Walker, H. St. C. K. Alleyne, M. A. Balikhin, M. André, T. S. Horbury Annales Geophysicae 22 (7), 2291-2300, 2004-07-14

...It is shown that the scale size of these short-lived electric field structures is of the order of a few c/ωpe....

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A. Ishizawa, R. Horiuchi, H. Ohtani Physics of Plasmas 11 (7), 3579-3585, 2004-07-01

...Although the ion frozen-in constraint is broken within a distance of the ion skin depth c/ωpi, the violation due to the ion inertia is weak compared to the strong violation caused by the ion-meandering...

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M. A. Shay, J. F. Drake, M. Swisdak, B. N. Rogers Physics of Plasmas 11 (5), 2199-2213, 2004-05-01

...This wide equilibrium current sheet is contrasted with the very thin equilibrium current sheets of width c/ωpi used in previous simulations to establish the importance of the Hall term in Ohm’s law in...

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J. D. Huba, L. I. Rudakov Physics of Plasmas 9 (11), 4435-4438, 2002-11-01

...<jats:p>New numerical results of three-dimensional magnetic reconnection in the Hall limit (L&lt;c/ωpi where c/ωpi is the ion inertial length) are presented....

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Uri Zwick Journal of the ACM 49 (3), 289-317, 2002-05

...Our algorithm improves on the <jats:italic>Õ</jats:italic> ( <jats:italic>n</jats:italic> <jats:sup>(3c+ω)/2</jats:sup> ) time algorithm, where...

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David A. Hostutler, Haiyang Li, Dennis J. Clouthier, Ghassan Wannous The Journal of Chemical Physics 116 (10), 4135-4141, 2002-03-08

...We have assigned the band system as a Hund’s case (c) Ω′=1−Ω″=1 transition from the ground Σg−3 state to a Σu−3 excited state....

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Haruhiko Saitoh, Zensho Yoshida, Chihiro Nakashima Review of Scientific Instruments 73 (1), 87-90, 2002-01-01

...For sufficiently large ωc/ωp (ωc: cyclotron frequency; ωp: plasma frequency), the flow can be approximated by the E×B drift velocity....

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Bruce I. Cohen, Andris M. Dimits, William M. Nevins, Yang Chen, Scott Parker Physics of Plasmas 9 (1), 251-262, 2002-01-01

...The hybrid schemes have the desirable properties that they do not require that the mesh size perpendicular to the applied magnetic field be smaller than the collisionless skin depth c/ωpe and naturally...

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S. Vincena, W. Gekelman, J. Maggs Physics of Plasmas 8 (9), 3884-3896, 2001-09-01

...The waves are excited by modulating a field-aligned electron current drawn to a disk antenna with a radius on the order of the electron skin-depth, δ=c/ωpe....

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M. R. Brown Physics of Plasmas 6 (5), 1717-1724, 1999-05-01

...Observations included a very thin current sheet (on the order of c/ωpe), accelerated electrons, and whistler waves. The argon ions were unmagnetized in these experiments....

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S. Peter Gary Journal of Geophysical Research: Space Physics 104 (A4), 6759-6762, 1999-04

...Theory yields <jats:italic>k<jats:sub>d</jats:sub></jats:italic>c/ω<jats:italic>p</jats:italic> = <jats:italic>S<jats:sub>k</jats:sub></jats:italic>/β<jats:sub><jats:italic>p</jats:italic></jats:sub><jats...

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C. C. Chaston, C. W. Carlson, W. J. Peria, R. E. Ergun, J. P. McFadden Geophysical Research Letters 26 (6), 647-650, 1999-03-15

...The wave period is usually less than 0.25s with ‘perpendicular wavelengths’ which average to 7.1 electron skin depths (c/ω<jats:sub>pe</jats:sub>∼80m)....

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Robert G. Kleva, Parvez N. Guzdar Physics of Plasmas 6 (1), 116-121, 1999-01-01

...The effect of the electron mass is characterized by the collisionless electron skin depth de=c/ωpe, where ωpe=4πne2/me is the electron plasma frequency....

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Naganori Hayashi, Tsuguhiko Tashiro, Hideo Yamamori, Kazuya Takagi, Yuichi Morishima, Yoshihisa Otsubo, Toshiyuki Sugiura, Katsunori Furukawa, Hiroshi Nitta, Nobuyuki Nakajima, Nobuo Suzuki, Isao Ito Journal of Parenteral and Enteral Nutrition 22 (6), 363-367, 1998-11

...Cell‐mediated immunity was thus significantly decreased in burned groups (groups C, ω6, and ω3; p <.01)....

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T. Lho, N. Hershkowitz, J. Miller, W. Steer, G. H. Kim Physics of Plasmas 5 (9), 3135-3142, 1998-09-01

...Wave propagation mode changes, from pseudosurface to helicon waves and from helicon to pseudosurface waves, were observed at critical conditions, ωc/ω&gt;3.0 and n∼2.2×1011 cm−3.</jats:p>...

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Alexander A. Nevzorov, Michael F. Brown The Journal of Chemical Physics 107 (23), 10288-10310, 1997-12-15

...ωH)/2π=938.7 MHz....

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J. F. Drake, D. Biskamp, A. Zeiler Geophysical Research Letters 24 (22), 2921-2924, 1997-11-15

...The current layer thins down below the electron skin depth <jats:italic>c/ω<jats:sub>pe</jats:sub></jats:italic> and then breaks up into a fully turbulent distribution of swirling vortices, The turbulence...

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Bernhard Jaun, Masakazu Tanaka, Paul Seiler, Florian N. M. Kühnle, Christine Braun, Dieter Seebach Liebigs Annalen 1997 (8), 1697-1710, 1997-08

...This structure is stabilized by hydrogen bonds between the NH(1) of the (<jats:italic>M</jats:italic>)‐helix and the OC(ω‐1) of the (<jats:italic>P</jats:italic>)‐helix and the NH(2) (<jats:italic>M...

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D. Biskamp, E. Schwarz, J. F. Drake Physics of Plasmas 4 (4), 1002-1009, 1997-04-01

...In the high-β case (β≳1) reconnection is controlled by the whistler mode, leading to decoupling of ions from electrons on scales &lt;c/ωpi....

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William F. Jackson, James M. Huebner, Nancy J. Rusch Microcirculation 4 (1), 35-50, 1997-03

..., <jats:italic>n</jats:italic> = 36 for rat cells: 8 ± 0.6 Cω, <jats:italic>n</jats:italic> = 21 for hamster cells: <jats:italic>p</jats:italic> < 0.05)....

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Shinohara Shunjiro, Kawai Yoshinobu Japanese Journal of Applied Physics 35 (6A), L725-L728, 1996

...For most evanescent waves, δ is expressed as f c / ω<SUB> pe</SUB> for ω<SUB> pe</SUB> >> ω, ν (f: collision term, ν : collision frequency, c : velocity of light, ω<SUB> pe</SUB> : electron plasma angular...

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P. L. Pritchett Physics of Plasmas 2 (7), 2664-2673, 1995-07-01

...In the parameter regime accessible to the simulations [flux bundle size L/(c/ωpi)≳3 and mass ratio Mi/me≤36], there is no indication of any significant change in the reconnection rate that could be associated...

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B. W. Church, R. N. Sudan Physics of Plasmas 2 (6), 1837-1845, 1995-06-01

...While other work on electron vortices considered a regime where the vortex radius is much smaller than the collisionless skin depth λ=c/ωp, this equilibrium is valid for large-radius, diamagnetic vortices...

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T. C. Chiou, T. Katsouleas, C. Decker, W. B. Mori, J. S. Wurtele, G. Shvets, J. J. Su Physics of Plasmas 2 (1), 310-318, 1995-01-01

...The accelerating gradients on the axis of a channel of radius c/ωp are of order of one-half of the gradients in a uniform plasma. For present high-power lasers, multi-GeV/m gradients are predicted....

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T. Achibat, A. Boukenter, E. Duval The Journal of Chemical Physics 99 (3), 2046-2051, 1993-08-01

...It was found that C(ω)∝ω2 at very low frequency ω&lt;20 cm−1 in inorganic glasses (SiO2,B2O3) and that C(ω)∝ω at low frequency in polymer glasses and in inorganic glasses for ω≳20 cm−1....

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E. Duval, N. Garcia, A. Boukenter, J. Serughetti The Journal of Chemical Physics 99 (3), 2040-2045, 1993-08-01

...The expressions of C(ω) are determined for other mechanisms of susceptibility fluctuations, depending on an interaction propagating in the fractal.</jats:p>...

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T. Tajima, S. Cable, R. M. Kulsrud Physics of Fluids B: Plasma Physics 4 (7), 2338-2345, 1992-07-01

...The size of the fluctuations is λ ∼ (c/ωp)(η/ω)1/2, where η and ω are the collision frequency and the (nearly zero) frequency of magnetic fields oscillations....

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A. Ting, E. Esarey, P. Sprangle Physics of Fluids B: Plasma Physics 2 (6), 1390-1394, 1990-06-01

...Relativistic focusing with the self-consistent plasma response shows that laser pulse fronts and laser pulses shorter than a plasma wavelength, 2πc/ωp, are not relativistically guided and will continuously...

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和田, 幸一, 守谷, 幸男, 川口, 喜三男, 森下, 正浩 全国大会講演論文集 第39回 (情報理論及び基礎技術), 65-66, 1989-10-16

...Ω(max(n,min(fn<logf>/<logn>,n^2)))かつT=Ω(n)であることを示す.サイズ既知モデルに対しては,C=O(e_f+nlogf),T=O(n)である分散アルゴリズムを示し,C=Ω(e_f)かつT=Ω(n)であることを示す.更に,故障をより一般化し,計算機の故障も許す場合には,各計算機が如何なる情報を保持していても連結性判定問題を解く分散アルゴリズムは存在しないことを示す...

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東海林, 直美, 加賀屋, 弘子, 相馬, 俊信 物性研究 51 (3), 283-292, 1988-12-20

...SiとGeに関する比熱C_Ωと線熱膨張係数αの温度依存性が,擬ポテンシャルに基づく格子振動の方法を用いて第一原理から理論的に研究される。調和近似におけるC^h_Ωとα^hの得られた結果は,低温部でこれらの結晶の実験値と首尾一貫している。高温部で,比熱への非調和項の寄与C^<ah>_Ω=C^h_Ω(1+AT)が,Trivedi達による表式を用いて計算される。...

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W. Horton, B. G. Hong, W. M. Tang The Physics of Fluids 31 (10), 2971-2983, 1988-10-01

...The small scale electrostatic component of the turbulence produces a small, of order (me/mi)1/2, drift wave anomalous transport of both the trapped and passing electrons while the c/ωpe scale turbulence...

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Yoshiro Nakagawa, Tamotsu Enomoto Journal of Applied Physics 61 (2), 470-475, 1987-01-15

...The observed large beam radius, compared with the radius expected from the model, could be attributed mainly to field penetration into the beam radius since the skin depth of the ion beam (c/ωp ∼0.4 cm...

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J. S. Brooks, O. G. Symko, T. G. Castner Japanese Journal of Applied Physics 26 (S3-1), 721-, 1987-01-01

...As T→0 C(ω,T) shows very little dispersion from hopping and one obtains the dielectric response <jats:italic>ε</jats:italic>'(N)-<jats:italic>ε</jats:italic> <jats:sub>h</jats:sub>=4π...

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P. L. Pritchett The Physics of Fluids 29 (9), 2919-2930, 1986-09-01

...Solution of the linear dispersion relation reveals that when the plasma frequency–gyrofrequency ratio ωpe/Ωe&lt;vte/c, the instability is localized just below k⊥c/Ωe=1....

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V. A. Thomas, Stephen H. Brecht The Physics of Fluids 29 (8), 2444-2454, 1986-08-01

...<jats:p>In this paper a hybrid particle–fluid simulation code is used to examine the large-scale (λ∼c/ωpi) low-frequency (ω∼ωci) formation and evolution of a collisonless shock in two dimensions where...

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I. Zhelyazkov, E. Benova, V. Atanassov Journal of Applied Physics 59 (5), 1466-1472, 1986-03-01

...For a given regime the axial plasma density profile is specified by two quantities: a numerical parameter σ=ωR/c (ω being the wave frequency, R the tube radius, and c denoting the speed of light) and the...

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A. Nishiguchi, T. Yabe, M. G. Haines The Physics of Fluids 28 (12), 3683-3690, 1985-12-01

...In laser-driven ablation the convection is toward the overdense region and B can be amplified by 10–100 times because ∇ ⋅ VT&lt;0, making B/ni almost constant for λmfp&gt;c/ωpe.</jats:p>...

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Kawamura Kimitaka, Ishiwatari Ryoshi ＧＥＯＣＨＥＭＩＣＡＬ　ＪＯＵＲＮＡＬ 19 (3), 113-126, 1985

...Some organic compounds decompose after reaching maximum concentrations at different temperatures: β-hydroxy acids (154°C), ω-hydroxy acids (179°C), (ω-1)-hydroxy acids (179°C), n-alcohols (229°C), phytanic...

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Scott Robertson The Physics of Fluids 26 (4), 1129-1138, 1983-04-01

...ωpe exceeds half the beam radius....

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I. Fidone, G. Granata, R. L. Meyer The Physics of Fluids 25 (12), 2249-2263, 1982-12-01

...It is first shown that the validity of the nonrelastivistic linear dispersion relation for a Maxwellian plasma is restricted by the conditions N2∥≫Te/mc2 and N2∥≫‖1−ω2c/ω2‖....

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D. B. Melrose, K. G. Rönnmark, R. G. Hewitt Journal of Geophysical Research: Space Physics 87 (A7), 5140-5150, 1982-07

...We find that for ∂f/∂v<jats:sub>⊥</jats:sub> > 0 at small v<jats:sub>⊥</jats:sub> there always exist rapidly growing waves with k<jats:sub>∥</jats:sub>²c²/ω² = n²cos²θ ≪ 1....

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岡本 加世子, 渡辺 正純, 川田 満, 後藤 義一, 芦田 康子, 小田 克明, 矢島 明子, 今田 伊助, 森本 浩 ＣＨＥＭＩＣＡＬ　＆　ＰＨＡＲＭＡＣＥＵＴＩＣＡＬ　ＢＵＬＬＥＴＩＮ 30 (8), 2797-2819, 1982

..., α-tocopherol and phylloquinone (Ia, b, c, IIa, b, c), 3-carboxy-2-butenyl (IIIa, b, c), 6-hydroxy-3-methyl-2-hexenyl (IVa, b, c), 4-hydroxy-3-methylbutyl (Va, b), 4-hydroxy-3-methyl-2-butenyl (VIb, c)...

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叶 篤正, Li Mai-tsun 気象集誌. 第2輯 60 (1), 16-23, 1982

...大規模運動において.L₀=c/ƒを特性的長さとするスケール効果があるのに類似してメソスケールの運動に対してはL₀'=C/Ωという特性的長さが存在することを示す。ここにcは重力波の速さ,ƒはコリオリ•パラメーター,Ωは風速場のもつ絶対渦度の代表値である。...

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ヒラシタ, ユキオ, HIRASHITA, Yukio 中京大学教養論叢 22 (1), 1-10-, 1981-05-31

...A W(1) Weierstrass point is a Weierstrass point in the ordinary sense, and a M(1/δ) Weierstrass point corresponds to a D Weierstrass point defined by means of H^0(C, (Ω^1)^<〓r(r-1)/2> (rD) in the algebraic...

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平下 幸男, Yukio HIRASHITA 中京大学教養論叢 = Chukyo University bulletin of the Faculty of Liberal Arts 22 (1), 1-10, 1981-05-31

...A W(1) Weierstrass point is a Weierstrass point in the ordinary sense, and a M(1/δ) Weierstrass point corresponds to a D Weierstrass point defined by means of H^0(C, (Ω^1)^<〓r(r-1)/2> (rD) in the algebraic...

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D. A. D’Ippolito, Y. C. Lee, J. F. Drake The Physics of Fluids 23 (4), 771-782, 1980-04-01

...ω....

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天下井 清, 川島 利兵衛 The Journal of Japan Institute of Navigation 62 (0), 113-124, 1980

...またC_ωでは揚網時の復原力を必要とする旋網漁船が最も大きい。船の重量が増すにつれて必然的にC_b,C_ωの値を大きくしている。2)総トン数当りの主機関馬力数は増加しているが船型の肥大化のために従来の船速を維持するにとどまっている。3)延繩釣漁船50トン以上100トン未満階層の代表であるイカ釣漁船において発電機出力は異常に増大し,集魚灯における過当競争を反映している。...

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C. Y. Yang, K. H. Johnson, J. A. Horsley The Journal of Chemical Physics 68 (3), 1001-1005, 1978-02-01

...An interpretation of the optical spectrum of the uranyl ion in terms of a Hund’s case (c) (ω, ω) coupling scheme is given.</jats:p>...

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Juan Francisco Lam, Bernard Lippmann, Frederick Tappert The Physics of Fluids 20 (7), 1176-1179, 1977-07-01

...The results differ quantitatively from those obtained form the paraxial ray theory but do agree qualitatively in that there is a minimum beam radius of order c/ωp, a threshold ’’critical’’ power, no upper...

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R. J. Commisso, Hans R. Griem The Physics of Fluids 20 (1), 44-50, 1977-01-01

...The results show that ΔLs≲ 3c/ωpi≫c/ωpe, ηeff≈100 η⊥, and the effective collision frequency, ν′eff, ω1h≲ν′eff≪ωpi, where η⊥ is the classical, Spitzer–Härm resistivity, and ω1h is the lower hybrid frequency...

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Miklos Porkolab, Martin V. Goldman The Physics of Fluids 19 (6), 872-881, 1976-06-01

...For low β, when L&lt;c/ωpe, stationary envelope and hole solitons are found, whereas in the limit L≳c/ωpi the super-Alvénic solitons described magnetohydromagnetically by Kaufman and Stenflo are obtained...

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R. C. Davidson, Joan M. Ogden The Physics of Fluids 18 (8), 1045-1050, 1975-08-01

...The characteristic maximum growth rate for Ti⊥≫Ti∥ is γM≈(βi⊥/2)1/2ωci, where βi⊥=8πniTi⊥/B20, and the wavelengths corresponding to instability are of order c/ωpi, where ωpi is the ion plasma frequency...

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José Canosa, Hideo Okuda The Physics of Fluids 18 (3), 335-345, 1975-03-01

...For strong magnetic fields (ωc ≳ ωp), the simulations verify the theoretical prediction that energy transport by plasma waves increases slowly with the magnetic field, and that in the limit of large field...

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瓜生 道也 気象集誌. 第2輯 53 (1), 45-54, 1975

...<br>まず,そのような波束は伝播過程で角運動量Ecosθ/ω(Eは,波のエネルギー,ωは波の東西方向のdrift角速度,θは緯度)を保存することが示される.そしてこの波束によって誘導される2次の平均帯状流Uは,ρUcosθ=E/ωで与えられることがわかる(ρは流体の密度).これらの結果は,ベータ平面上では,波束が運動量.E/C(Cは東西位相速度.C=ωcosθ)を保存し,平均帯状流はρU=E/Cで...

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Y. K. Levine, N. J. M. Birdsall, A. G. Lee, J. C. Metcalfe, P. Partington, G. C. K. Roberts The Journal of Chemical Physics 60 (7), 2890-2899, 1974-04-01

...Two cases have been considered in which the motion about the long axis of the ellipsoid is fast [(ωC + ωH)2 / 6DZ2 ≪ 1] or slow [(ωC + ωH)2 / 6DZ2 &gt; 1] compared to the highest relevant Larmor frequency...

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内田 勝, 稲津 博 Radiologic Imaging Reserch 4 (2), 69-74, 1974

...The MTF C(ω) of clean-up effect of scattered radiations by collimator is to be obtained by the Vol.4 No.2 1974 69following Equation. C(ω)=X(ω)/Y(ω)<BR>Where C(ω) is changed by radiation fields....

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稲津 博 日本放射線技術学会雑誌 30 (3), 266-268, 1974

...The MTF C(ω) of clean-up effect of scatterted radiations by collimator is to be obtained by the following Equation. [numerical formula] Where C(ω) is changed by radiation fields....

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Michael E. Mcintyre Journal of Fluid Mechanics 60 (4), 801-811, 1973-10-09

.... \]</jats:disp-formula>Here [Mscr ] is the so-called ‘wave momentum’, defined as wave energy divided by horizontal phase velocity c ≡ ω/<jats:italic>k</jats:italic>, and<jats:italic>c</jats:italic><jats...

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大須賀 昭夫, 楠本 正一, 小竹 無二雄 日本化学会誌（化学と工業化学） 1973 (3), 590-594, 1973-03-10

...すなわち[3]から誘導されるジオール[5]とそのC位の水酸基が天然型と逆の配位をとっている7エピジオール[11]のNMRスペクトルでC(7)位の水素のシグルの半値幅はそれぞれ 9H zと モ23 H:zであり,かつ溶媒をCC1,からピリジンに変えたときのC(5)およびつω位のメチル基のシグナルの移動も,天然型のCω位の水酸基がaxial配位であることを示している。...

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塙 友雄 関西造船協会誌 147 (0), 33-42, 1973

...The procedure to be taken is as follows. (1) C_p curve is obtained by analysing its slope curve, comparing actual hull forms with theoretical ones. (2) C_ω curve is drawn based on both C_p curve and the...

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稲津 博, 河野 誠一, 篠崎 悌五, 金丸 国雄 日本放射線技術学会雑誌 28 (4), 362-367, 1973

...C(ω)=A_1(ω)/A_2(ω)……(1) If the efficiency of X-ray grids is estimated by MTF, eliminating effect by X-ray grids can be estimated quantitatively at every spatial frequency....

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余越, 正一郎 信州大学工学部紀要 32 217-225, 1972-07-25

...The asymptotic form of the spectrum is expressed in the form, E₁₁(ω) = AL<ε>/ω₀² exp[-c²(ω/ω∞)²] / 1+(ω/ω₀)² where AL is the universal constant. AL ≈ c/4. 4....

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Craig L. Olson The Physics of Fluids 15 (1), 160-165, 1972-01-01

...If the latter inequality does not hold, then the free-streaming and branch-cut terms persist well past z = c/ωce as ω1 approaches ωce, making experimental measurement of cyclotron damping essentially impossible...

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赤崎 繁 西部造船会々報 43 (0), 23-34, 1972

...The coefficient of keinetic energy of ship turning is taken 1/2 in the equaticn KE=cω^2I_O....

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Roswell Lee, R. N. Sudan The Physics of Fluids 14 (6), 1213-1225, 1971-06-01

...ωp, and ωp is the plasma frequency of the plasma electrons....

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長谷川 秋雄, 能本 乙彦, 畑岡 宏 日本音響学会誌 26 (8), 347-356, 1970

...Fig. 3 or Fig. 8), k=ω/c, ω=circular frequency, k_z=propagation constant in z-direction (cf. Fig3 or Fig. 8), α=attenuation constant which should be determined by experimental data (cf. Fig. 7)....

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Brian L. Murphy The Physics of Fluids 12 (11), 2381-2387, 1969-11-01

...It is found that the length scale of the magnetic field before the electron turning point is the plasma skin depth c/ωpe as in the boundary layer with γ ≪ 1, but that the electron number density diverges...

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J. R. Apel, T. O. Poehler, C. R. Westgate Applied Physics Letters 14 (5), 161-163, 1969-03-01

...At 119 μm, a number of subsidiary maxima was observed on the low field side at ωc = ω(laser)/n where n = 1, 2, …, 6, apparently due to intraband transitions to higher Landau levels.</jats:p>...

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井川 博, 新 成夫, 宮城 政和, 森川 正樹 日本金属学会誌 33 (2), 152-157, 1969

...In the Ti-8%Mn alloy brine quenched from 950°C, ω′ (which gives diffuse diffraction spots at the same positions as ω) and α″ (<I>fcc</I> martensite) phases besides retained β phase were observed by electron...

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F.L. Ribe Nuclear Fusion 7 (2-3), 81-89, 1967-09-01

...The sheath which separates the plasma from the confining magnetic field has the dimension c/ω<jats:sub>pi</jats:sub> (the ion collisionless skin depth), indicating that sheath ions carry the current. θ-pinch...

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C. Kennel The Physics of Fluids 9 (11), 2190-2202, 1966-11-01

...The low-frequency whistler mode, cB/M+c « ω « eB/M−c, is treated in detail....

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仲 三郎 繊維機械学会論文集 19 (2), T56-T62, 1966

One of the many causes for streaks in seamless hosiery is the action exerted by the latch on the loop during the downward and upward movements of a needle. This article derives theoretical equations …

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向井 毅 日本建築学会論文報告集 119 (0), 1-9,77, 1966

...C, ω/c : 55%). That is, the almost satisfiies the design strength for a structural Member....

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掛見 喜一郎, 有田 隆一, 堀 了平, 武仲 宏, 中川 寛 薬学雑誌 86 (9), 797-802, 1966

...The compounds synthesized were p-aminophenol derivatives of ω, ω'-bis(2-hydroxy-5-aminophenyl)alkanes (A), ω, ω'-bis(2-hydroxy-5-dimethylaminophenyl)alkanes (C), ω, ω'-bis(2-hydroxy-4-methyl-5-aminophenyl...

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V. L. Granatstein, S. P. Schlesinger Journal of Applied Physics 35 (10), 2846-2855, 1964-10-01

...The parameter space is 3-dimensional with coordinates ωp/ω, ωb/ω, and c/ωa....

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加地 郁夫, 鬼頭 正史, 小沢 保知 核融合研究 12 (6), 564-572, 1964

...<BR>When the range of vainable kc/ω<SUB>p</SUB> and parameters σ<SUB>⊥</SUB>/ c, , Ω/ω<SUB>p</SUB> is taken such that kc/ω<SUB>p</SUB> = 0, 0.5, …, 9.5, 10, <BR>σ<SUB>⊥</SUB>/c = 2<SUP>n</SUP>×10<SUP>-...

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H. W. Wyld The Physics of Fluids 3 (3), 408-415, 1960-05-01

...<jats:p>The radiation by a thermal distribution of plasma oscillations in a bounded plasma in a magnetic field is calculated in the limit (ωc/ωp)½ « 1, where ωc and ωp are the cyclotron and plasma frequencies...

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Norman Rostoker, M. N. Rosenbluth The Physics of Fluids 3 (1), 1-14, 1960-01-01

...When there is a constant external magnetic field, the problem is characterized by the parameter g, and also the parameter λ = ωc/ωp....

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荒川 秀俊 気象集誌. 第2輯 21 (10), 443-447, 1943

...<i>u</i> and <i>v</i> being the horizontal velocity component, <i>w</i> the vertical component, <i>p</i> the pressure, ρ the density and ƒ the Coriolis parameter, 2ωsinφ, where φ is the latitude and cω...

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上野,敬三 造船協會會報 19-86, 1941-02-25

...Therefore, C_α and C_ω are the effects of the horizontal motion on the free rolling, and the calculated C_α and C_ω agree with the experimental results....

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妹澤, 克惟, 内田, 郁雄, SEZAWA, Katsutada, UTIDA, Ikuo 東京帝國大學航空研究所報告 = Report of Aeronautical Research Institute, Tokyo Imperial University 14 (181), 325-361, 1939-08

...プロペラが斜對稱に振動する場合即ちプロペラの中心が翼の節點になる場合との2種類を取扱つた.尚最初の種類ではボスの半徑を零と見る場合と半徑のある場合とに分けて考へたのである.計算の結果,振動數(p/2π)の2乘と回轉數(ω/2π)の2乘とは必ずしも一次的關係にない事がわかつた.しかし大體に於て一次的であつて,回轉しないときの振動數をp_0/2πとすれば,近似的にはSouthwellの式p^2=p_0^2+Cω...

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