Статті в журналах: "Anomalous hydrodynamics"

1

Newman, George M. "Anomalous hydrodynamics." Journal of High Energy Physics 2006, no. 01 (January 30, 2006): 158. http://dx.doi.org/10.1088/1126-6708/2006/01/158.

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2

Nakayama, Yu. "Anomalous hydrodynamics with dyonic charge." International Journal of Modern Physics A 36, no. 18 (June 16, 2021): 2150133. http://dx.doi.org/10.1142/s0217751x21501335.

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In this paper, we study anomalous hydrodynamics with a dyonic charge. We show that the local second law of thermodynamics constrains the structure of the anomaly in addition to the structure of the hydrodynamic constitutive equations. In particular, we show that not only the usual [Formula: see text] term but also [Formula: see text] term should be present in the anomaly with a specific coefficient for the local entropy production to be positive definite.

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3

Dhia, Hamed Ben. "Thermal regime and hydrodynamics in Tunisia and Algeria." GEOPHYSICS 56, no. 7 (July 1991): 1093–102. http://dx.doi.org/10.1190/1.1443121.

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The thermal regime of Algeria and Tunisia and its relation to hydrodynamics is studied by means of available geological and geothermal, and petroleum data. Heat flow densities in the area range from [Formula: see text] to [Formula: see text]. Several Paleozoic to Tertiary aquifers have been identified, together with potential recharge and discharge areas. The area is a transition zone between the African and European plates. The more tectonically active northern Alpine domain does not exhibit an obvious geothermal trend, and high heat flow anomalies that occur there may be related to structure rather than hydrodynamics. The more stable southern Saharan tectonic domain, with background heat flow of approximately [Formula: see text], exhibits anomalous zones correlated to the hydrodynamic regime with low values in recharge areas (Algerian Tinrhert and High Plateaux) and values in discharge areas (Tunisian Jeffara and Algerian Tademait). The hydrodynamic perturbation to the normal heat flow is estimated to be as great as [Formula: see text] in recharge and discharge zones.

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4

BANERJEE, RABIN. "Anomalous hydrodynamics in two dimensions." Pramana 86, no. 2 (January 14, 2016): 453–58. http://dx.doi.org/10.1007/s12043-015-1167-5.

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5

Lin, Shu. "On the anomalous superfluid hydrodynamics." Nuclear Physics A 873 (January 2012): 28–46. http://dx.doi.org/10.1016/j.nuclphysa.2011.10.001.

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6

Kaminski, Matthias, Christoph F. Uhlemann, Marcus Bleicher, and Jürgen Schaffner-Bielich. "Anomalous hydrodynamics kicks neutron stars." Physics Letters B 760 (September 2016): 170–74. http://dx.doi.org/10.1016/j.physletb.2016.06.054.

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7

Megías, Eugenio, and Manuel Valle. "Anomalous transport in second order hydrodynamics." EPJ Web of Conferences 126 (2016): 04032. http://dx.doi.org/10.1051/epjconf/201612604032.

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8

Morningstar, Alan, and Waseem Bakr. "Anomalous fluid flow in quantum systems." Science 376, no. 6594 (May 13, 2022): 699–700. http://dx.doi.org/10.1126/science.abn6376.

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9

Wiegmann, P. "Anomalous hydrodynamics of fractional quantum Hall states." Journal of Experimental and Theoretical Physics 117, no. 3 (September 2013): 538–50. http://dx.doi.org/10.1134/s1063776113110162.

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10

Joshi, M. K., F. Kranzl, A. Schuckert, I. Lovas, C. Maier, R. Blatt, M. Knap, and C. F. Roos. "Observing emergent hydrodynamics in a long-range quantum magnet." Science 376, no. 6594 (May 13, 2022): 720–24. http://dx.doi.org/10.1126/science.abk2400.

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Identifying universal properties of nonequilibrium quantum states is a major challenge in modern physics. A fascinating prediction is that classical hydrodynamics emerges universally in the evolution of any interacting quantum system. We experimentally probed the quantum dynamics of 51 individually controlled ions, realizing a long-range interacting spin chain. By measuring space-time–resolved correlation functions in an infinite temperature state, we observed a whole family of hydrodynamic universality classes, ranging from normal diffusion to anomalous superdiffusion, that are described by Lévy flights. We extracted the transport coefficients of the hydrodynamic theory, reflecting the microscopic properties of the system. Our observations demonstrate the potential for engineered quantum systems to provide key insights into universal properties of nonequilibrium states of quantum matter.

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11

Guo, Xingyu, Dmitri E. Kharzeev, Xu-Guang Huang, Wei-Tian Deng, and Yuji Hirono. "Chiral Vortical and Magnetic Effects in Anomalous Hydrodynamics." Nuclear Physics A 967 (November 2017): 776–79. http://dx.doi.org/10.1016/j.nuclphysa.2017.06.039.

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12

Hirono, Yuji, Tetsufumi Hirano, and Dmitri E. Kharzeev. "Charge-dependent correlations from event-by-event anomalous hydrodynamics." Nuclear Physics A 956 (December 2016): 393–96. http://dx.doi.org/10.1016/j.nuclphysa.2016.03.049.

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13

Hattori, Koichi, and Yi Yin. "Charge redistribution from novel magneto-vorticity coupling in anomalous hydrodynamics." Nuclear Physics A 967 (November 2017): 768–71. http://dx.doi.org/10.1016/j.nuclphysa.2017.05.009.

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14

Dwivedi, Vatsal, and Michael Stone. "Chiral kinetic theory and anomalous hydrodynamics in even spacetime dimensions." Journal of Physics A: Mathematical and Theoretical 50, no. 15 (March 14, 2017): 155202. http://dx.doi.org/10.1088/1751-8121/aa6262.

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15

Tunga, Ashwin, Kexin Li, Ethan White, Nicholas C. Miller, Matt Grupen, John D. Albrecht, and Shaloo Rakheja. "A comparison of a commercial hydrodynamics TCAD solver and Fermi kinetics transport convergence for GaN HEMTs." Journal of Applied Physics 132, no. 22 (December 14, 2022): 225702. http://dx.doi.org/10.1063/5.0118104.

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Various simulations of a GaN HEMT are used to study the behaviors of two different energy-transport models: the Fermi kinetics transport model and a hydrodynamics transport model as it is implemented in the device simulator Sentaurus from Synopsys. The electron transport and heat flow equations of the respective solvers are described in detail. The differences in the description of electron flux and the discretization methods are highlighted. Next, the transport models are applied to the same simulated device structure using identical meshes, boundary conditions, and material parameters. Static simulations show the numerical convergence of Fermi kinetics to be consistently quadratic or faster, whereas the hydrodynamic model is often sub-quadratic. Further comparisons of large-signal transient simulations reveal the hydrodynamic model produces certain anomalous electron ensemble behaviors within the transistor structure. The fundamentally different electron dynamics produced by the two models suggest an underlying cause for their different numerical convergence characteristics.

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16

Graf von der Schulenburg, D. A., L. F. Gladden, and M. L. Johns. "Modelling biofilm-modified hydrodynamics in 3D." Water Science and Technology 55, no. 8-9 (April 1, 2007): 275–81. http://dx.doi.org/10.2166/wst.2007.268.

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A simulation–based study to predict the impact of biofilm growth on displacement distributions for flow of water through a supporting packed bed is presented. The lattice Boltzmann method and a directed random walk algorithm are used, and are applied to the system with and without biofilm being present. The aim of this simulation study is to model the anomalous transport dynamics induced by biofilm, as reported in the literature, and thus to study the impact of observation time, Δ, on the shape of the displacement distributions (propagators). We believe that this is the first demonstration of a propagator simulation for flow through a complex porous structure modulated by biofilm growth. The propagator distributions undergo a transition from a pre-asymptotic to a Gaussian-shaped distribution with increasing Δ. The propagators were simulated for a wide range of Δ going up to 500 seconds. This transition occurs with and without biofilm, but is very significantly delayed when biofilm is present due to the consequential development of essentially stagnant regions. The transition can be classified into three stages: a diffusion-dominated stage, a “twin-peak” stage and an advection-dominated stage.

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17

Gustafsson, B., K. Kodaira, D. F. Gray, A. G. Hearn, W. Kalkofen, R. P. Kudritski, D. Mihalas, et al. "Commission 36: Theory of Stellar Atmospheres." Transactions of the International Astronomical Union 19, no. 1 (1985): 503–7. http://dx.doi.org/10.1017/s0251107x00006556.

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Commission 36 acts as a sponsor or co-sponsor at the following symposi and colloquia: IAU Colloquium No. 90 “Upper Main Sequence Stars with Anomalous Abundances”, Crima, USSR (May 1985), IAU Colloquium No. 89 “Radiation Hydrodynamics in Stars and Compact Objects”, Copenhagen, Denmark (June 1985), IAU Symposium No. 120 “Astrochemistry”, Goa, India (December 1985), IAU Colloquium No. 87 “Hydrogen Deficient Stars and Related Objects”, Bangalore, India (December 1985).

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18

Alexandrov, Dmitri V., and Andrey Yu Zubarev. "Transport phenomena in complex systems (part 1)." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 379, no. 2205 (July 19, 2021): 20200301. http://dx.doi.org/10.1098/rsta.2020.0301.

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The issue, in two parts, is devoted to theoretical, computational and experimental studies of transport phenomena in various complex systems (in porous and composite media; systems with physical and chemical reactions and phase and structural transformations; in biological tissues and materials). Various types of these phenomena (heat and mass transfer; hydrodynamic and rheological effects; electromagnetic field propagation) are considered. Anomalous, relaxation and nonlinear transport, as well as transport induced by the impact of external fields and noise, is the focus of this issue. Modern methods of computational modelling, statistical physics and hydrodynamics, nonlinear dynamics and experimental methods are presented and discussed. Special attention is paid to transport phenomena in biological systems (such as haemodynamics in stenosed and thrombosed blood vessels magneto-induced heat generation and propagation in biological tissues, and anomalous transport in living cells) and to the development of a scientific background for progressive methods in cancer, heart attack and insult therapy (magnetic hyperthermia for cancer therapy, magnetically induced circulation flow in thrombosed blood vessels and non-contact determination of the local rate of blood flow in coronary arteries). The present issue includes works on the phenomenological study of transport processes, the derivation of a macroscopic governing equation on the basis of the analysis of a complicated internal reaction and the microscopic determination of macroscopic characteristics of the studied systems. This article is part of the theme issue ‘Transport phenomena in complex systems (part 1)’.

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19

Belyi, V. V., D. Dewulf, and I. Paiva‐Veretennicoff. "Anomalous transport in strongly inhomogeneous systems. II. The generalized hydrodynamics of a two‐component plasma." Physics of Fluids B: Plasma Physics 1, no. 2 (February 1989): 317–24. http://dx.doi.org/10.1063/1.859144.

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20

Gopalakrishnan, Sarang, Romain Vasseur, and Brayden Ware. "Anomalous relaxation and the high-temperature structure factor of XXZ spin chains." Proceedings of the National Academy of Sciences 116, no. 33 (July 30, 2019): 16250–55. http://dx.doi.org/10.1073/pnas.1906914116.

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We compute the spin-structure factor of XXZ spin chains in the Heisenberg and gapped (Ising) regimes in the high-temperature limit for nonzero magnetization, within the framework of generalized hydrodynamics, including diffusive corrections. The structure factor shows a hierarchy of timescales in the gapped phase, owing to s-spin magnon bound states (“strings”) of various sizes. Although short strings move ballistically, long strings move primarily diffusively as a result of their collisions with short strings. The interplay between these effects gives rise to anomalous power-law decay of the spin-structure factor, with continuously varying exponents, at any fixed separation in the late-time limit. We elucidate the cross-over to diffusion (in the gapped phase) and to superdiffusion (at the isotropic point) in the half-filling limit. We verify our results via extensive matrix product operator calculations.

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21

Takae, Kyohei, and Hajime Tanaka. "Role of hydrodynamics in liquid–liquid transition of a single-component substance." Proceedings of the National Academy of Sciences 117, no. 9 (February 12, 2020): 4471–79. http://dx.doi.org/10.1073/pnas.1911544117.

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Liquid–liquid transition (LLT) is an unconventional transition between two liquid states in a single-component system. This phenomenon has recently attracted considerable attention not only because of its counterintuitive nature but also since it is crucial for our fundamental understanding of the liquid state. However, its physical understanding has remained elusive, particularly of the critical dynamics and phase-ordering kinetics. So far, the hydrodynamic degree of freedom, which is the most intrinsic kinetic feature of liquids, has been neglected in its theoretical description. Here we develop a Ginzburg–Landau-type kinetic theory of LLT taking it into account, based on a two-order parameter model. We examine slow critical fluctuations of the nonconserved order parameter coupled to the hydrodynamic degree of freedom in equilibrium. We also study the nonequilibrium process of LLT. We show both analytically and numerically that domain growth becomes faster (slower), depending upon the density decrease (increase) upon the transition, as a consequence of hydrodynamic flow induced by the density change. The coupling between nonconserved order parameter and hydrodynamic interaction results in anomalous domain growth in both nucleation-growth–type and spinodal-decomposition–type LLT. Our study highlights the characteristic features of hydrodynamic fluctuations and phase ordering during LLT under complex interplay among conserved and nonconserved order parameters and the hydrodynamic transport intrinsic to the liquid state.

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22

Hristov, Jordan. "Starting radial subdiffusion from a central point through a diverging medium (a sphere): Heat-balance integral method." Thermal Science 15, suppl. 1 (2011): 5–20. http://dx.doi.org/10.2298/tsci11s1005h.

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The work presents an integral solution of the time-fractional subdiffusion equation as alternative approach to those employing hypergeometric functions. The integral solution suggests a preliminary defined profile with unknown coefficients and the concept of penetration (boundary layer) well known from the heat diffusion and hydrodynamics. The profile satisfies the boundary conditions imposed at the boundary of the boundary layer that allows its coefficients to be expressed through the boundary layer depth as unique parameter describing the profile. The technique is demonstrated by a solution of a time fractional radial equation concerning anomalous diffusion from a central point source in a sphere.

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23

Iubini, Stefano, Stefano Lepri та Stefano Ruffo. "Hydrodynamics and transport in the long-range-interacting φ ⁴ chain". Journal of Statistical Mechanics: Theory and Experiment 2022, № 3 (1 березня 2022): 033209. http://dx.doi.org/10.1088/1742-5468/ac59b6.

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Abstract We present a simulation study of the one-dimensional φ 4 lattice theory with long-range interactions decaying as an inverse power r −(1+σ) of the intersite distance r, σ > 0. We consider the cases of single and double-well local potentials with both attractive and repulsive couplings. The double-well, attractive case displays a phase transition for 0 < σ ⩽ 1 analogous to the Ising model with long-range ferromagnetic interactions. A dynamical scaling analysis of both energy structure factors and excess energy correlations shows that the effective hydrodynamics is diffusive for σ > 1 and anomalous for 0 < σ < 1, where fluctuations propagate superdiffusively. We argue that this is accounted for by a fractional diffusion process and we compare the results with an effective model of energy transport based on Lévy flights. Remarkably, this result is fairly insensitive on the phase transition. Nonequilibrium simulations with an applied thermal gradient are in quantitative agreement with the above scenario.

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24

Drazic, Dragutin, Jovan Popic, B. Jegdic, and D. Vasiljevic-Radovic. "Electrochemistry of active chromium, part IV: Dissolution of chromium in deaerated sulfuric acid." Journal of the Serbian Chemical Society 69, no. 12 (2004): 1099–110. http://dx.doi.org/10.2298/jsc0412099d.

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Chromium dissolution in aqueous sulfuric acid solutions in the pH range 0.5 ?3 was studied electrochemically by the potentiostatic or very slow potentiodynamic method, and by the analyses of the Cr ion concentrations in the electrolyte formed during the experiments. It was shown that the electrochemical anodic dissolution follows a common Tafel line with a slope of ca. 120 mVdec-1, independent of the solution pH and the hydrodynamics while the passivation potentials and passivation currents were independent on hydrodynamics but strongly dependent on the pH. In parallel with the electrochemical dissolution, a considerable "anomalous" or chemical Cr dissolution process occurs, as evidenced by the spectrophotometric analyses of the electrolytes for Cr ions after prolonged potentiostating of the electrodes at different potentials, as well as by measuring the electrode weight losses. All these results indicate the existence of a potential independent reaction of Cr dissolution occurring in parallel to the anodic dissolution process. Mechanisms for both the electrochemical and the chemical process are proposed. The consequences of these phenomena on the behavior of some practical systems where chromium or a chromium alloy (e.g., stainless steels) are used are discussed.

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25

Cook, Kerry H., and Edward K. Vizy. "Hydrodynamics of the Caribbean Low-Level Jet and Its Relationship to Precipitation." Journal of Climate 23, no. 6 (March 15, 2010): 1477–94. http://dx.doi.org/10.1175/2009jcli3210.1.

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Abstract The easterly Caribbean low-level jet (CLLJ) is a prominent climate feature over the Intra-America Seas, and it is associated with much of the water vapor transport from the tropical Atlantic into the Caribbean Basin. In this study, the North American Regional Reanalysis (NARR) is analyzed to improve the understanding of the dynamics of the CLLJ and its relationship to regional rainfall variations. Horizontal momentum balances are examined to understand how jet variations on both diurnal and seasonal time scales are controlled. The jet is geostrophic to the first order. Its previously documented semidiurnal cycle (with minima at about 0400 and 1600 LT) is caused by semidiurnal cycling of the meridional geopotential height gradient in association with changes in the westward extension of the North Atlantic subtropical high (NASH). A diurnal cycle is superimposed, associated with a meridional land–sea breeze (solenoidal circulation) onto the north coast of South America, so that the weakest jet velocities occur at 1600 LT. The CLLJ is present throughout the year, and it is known to vary in strength semiannually. Peak magnitudes in July are related to the seasonal cycle of the NASH, and a second maximum in February is caused by heating over northern South America. From May through September, zonal geopotential gradients associated with summer heating over Central America and Mexico induce meridional flow. The CLLJ splits into two branches, including a southerly branch that connects with the Great Plains low-level jet (GPLLJ) bringing moisture into the central United States. During the rest of the year, the flow remains essentially zonal across the Caribbean Basin and into the Pacific. A strong (weak) CLLJ is associated with reduced (enhanced) rainfall over the Caribbean Sea throughout the year in the NARR. The relationship with precipitation over land depends on the season. Despite the fact that the southerly branch of the CLLJ feeds into the meridional GPLLJ in May through September, variations in the CLLJ strength during these months do not impact U.S. precipitation, because the CLLJ strength is varying in response to regional-scale forcing and not to changes in the large-scale circulation. During the cool season, there are statistically significant correlations between the CLLJ index and rainfall over the United States. When the CLLJ is strong, there is anomalous northward moisture transport across the Gulf of Mexico into the central United States and pronounced rainfall increases over Louisiana and Texas. A weak jet is associated with anomalous westerly flow across the southern Caribbean region and significantly reduced rainfall over the south-central United States. No connection between the intensity of the CLLJ and drought over the central United States is found. There are only three drought summers in the NARR period (1980, 1988, and 2006), and the CLLJ was extremely weak in 1988 but not in 1980 or 2006.

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26

Berman, Gregory A., David F. Naar, Albert C. Hine, Gregg R. Brooks, Sarah F. Tebbens, Brian T. Donahue, and Robert Wilson. "Geologic Structure and Hydrodynamics of Egmont Channel: An Anomalous Inlet at the Mouth of Tampa Bay, Florida." Journal of Coastal Research 212 (March 2005): 331–57. http://dx.doi.org/10.2112/03-0015.1.

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27

Асадуллин, Наиль, and Nail Asadullin. "CLASSIFICATION OF FODDER MASSES APPLIED TO ITS HYDRO-MECHANICS." Vestnik of Kazan State Agrarian University 13, no. 2 (August 6, 2018): 71–75. http://dx.doi.org/10.12737/article_5b35058f6bef38.44028308.

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The current stage in the development of agricultural production in livestock is characterized by the extensive use of pipeline transport to move the forage masses, which are related to non-Newtonian fluids. Production experience and scientific work on the study of hydrotransport systems showed that this method of transportation is the most economical and promising, it has high reliability of structural elements, improves sanitary and hygienic working conditions and makes it possible to fully automate the transportation process. The complex nature of the transportation of mixtures has not allowed to create a unified theory of hydrodynamic calculation of their parameters to date, therefore, various models are used for theoretical investigation of the nature of motion. To select a particular model, it is always important to correctly classify viscous semiliquid media with respect to hydrodynamics. Therefore, the article did not set out the specific goal of choosing a method for studying non-Newtonian systems, but solved the problem of their classification by known defining characteristics. The proposed classification does not pretend to be exhaustive in terms of the physical and chemical nature of the fluid, especially their combinations, but it covers almost all the anomalous phenomena that occur in the fluid during its transportation and helps to select a quantitative method for calculating the transporting fluid. The classification of non-Newtonian fluids with respect to their hydromechanics is based on the dependence of the shear stress on the shear gradient. For this dependence, each type of liquid is considered. The developed classification scheme further promotes a more complete account of the rheological properties of high-viscosity liquids during their transportation through pipes and facilitates the development of quantitative calculation methods.

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28

Fujimoto, Yusuke, Mark R. Krumholz, and Shu-ichiro Inutsuka. "Distribution and kinematics of 26Al in the Galactic disc." Monthly Notices of the Royal Astronomical Society 497, no. 2 (July 24, 2020): 2442–54. http://dx.doi.org/10.1093/mnras/staa2125.

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ABSTRACT 26Al is a short-lived radioactive isotope thought to be injected into the interstellar medium (ISM) by massive stellar winds and supernovae (SNe). However, all-sky maps of 26Al emission show a distribution with a much larger scale height and faster rotation speed than either massive stars or the cold ISM. We investigate the origin of this discrepancy using an N-body + hydrodynamics simulation of a Milky-Way-like galaxy, self-consistently including self-gravity, star formation, stellar feedback, and 26Al production. We find no evidence that the Milky Way’s spiral structure explains the 26Al anomaly. Stars and the 26Al bubbles they produce form along spiral arms, but, because our simulation produces material arms that arise spontaneously rather than propagating arms forced by an external potential, star formation occurs at arm centres rather than leading edges. As a result, we find a scale height and rotation speed for 26Al similar to that of the cold ISM. However, we also show that a synthetic 26Al emission map produced for a possible Solar position at the edge of a large 26Al bubble recovers many of the major qualitative features of the observed 26Al sky. This suggests that the observed anomalous 26Al distribution is the product of foreground emission from the 26Al produced by a nearby, recent SN.

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29

Gao, Christina, and Albert Stebbins. "Structure of stellar remnants with coupling to a light scalar." Journal of Cosmology and Astroparticle Physics 2022, no. 07 (July 1, 2022): 025. http://dx.doi.org/10.1088/1475-7516/2022/07/025.

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Abstract In this paper, we study how a Yukawa coupling of the Standard Model fermions to a light scalar field affects the stellar structure of cold stellar remnants such as neutron stars. We elucidate the stellar structure phenomenology using a simple model of a massive scalar coupled to a single dominant fermion with no other interactions. For a broad scalar mass range (10-10 eV ≪ mϕ ≪ 103 eV for neutron stars) we show that the equation-of-state and stellar structure depends on the effective coupling ℊ = gf mf /mϕ , where gf is the Yukawa coupling, mf is the fermion mass, and mϕ is the scalar kinematic mass at nuclear densities. If ℊ > 𝒪(1) the Yukawa coupled matter exhibits various anomalous behaviors including hydrodynamic instability, negative pressure, distinct phases (soft and hard) of matter with sharp phase boundaries between them and with the vacuum. These anomalies can lead to stars consisting of only soft, only hard, or a hybrid of soft and hard matter. These stars can have either sign for the slope of the mass-radius relation, anomalously large and small masses, gaps in allowed radii, multiple radii for the same mass, thin crusts and radiate anomalously large amounts of energy when they form (in the form of neutrinos for neutron stars). To the extent that these anomalies have not and/or will not be observed limits the effective coupling to ℊ < 𝒪(1). We argue this phenomenology is generic to stars with Yukawa coupled matter.

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30

Ingel, L. Kh. "Anomalous hydrodynamic drag due to differential diffusion." Technical Physics 55, no. 2 (February 2010): 309–11. http://dx.doi.org/10.1134/s1063784210020258.

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31

Abbasi, Navid, Ali Davody, Kasra Hejazi, and Zahra Rezaei. "Hydrodynamic waves in an anomalous charged fluid." Physics Letters B 762 (November 2016): 23–32. http://dx.doi.org/10.1016/j.physletb.2016.09.002.

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32

Ryltsev, R. E., and N. M. Chtchelkatchev. "Hydrodynamic anomalies in supercritical fluid." Journal of Chemical Physics 141, no. 12 (September 28, 2014): 124509. http://dx.doi.org/10.1063/1.4895726.

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33

Bleibel, J., A. Domínguez, F. Günther, J. Harting, and M. Oettel. "Hydrodynamic interactions induce anomalous diffusion under partial confinement." Soft Matter 10, no. 17 (February 17, 2014): 2945–48. http://dx.doi.org/10.1039/c3sm53043d.

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34

DEKKER, H. "THEORY OF TURBULENCE: ANOMALOUS THERMAL FLUX SPECTRUM." Modern Physics Letters B 16, no. 13 (June 10, 2002): 491–95. http://dx.doi.org/10.1142/s0217984902003919.

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A recent theory of fully-developed 3D hydrodynamic turbulence, involving dynamical response functions for turbulent thermal shear flow, yields analytical results for the anomalous Kolmogorov spectrum of streamwise heat flux.

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35

Bakli, Chirodeep, and Suman Chakraborty. "Anomalous interplay of slip, shear and wettability in nanoconfined water." Nanoscale 11, no. 23 (2019): 11254–61. http://dx.doi.org/10.1039/c9nr01572h.

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36

L'vov, Victor S., and Itamar Procaccia. "Viscous Lengths in Hydrodynamic Turbulence are Anomalous Scaling Functions." Physical Review Letters 77, no. 17 (October 21, 1996): 3541–44. http://dx.doi.org/10.1103/physrevlett.77.3541.

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37

Bacri, J. ‐C, N. Rakotomalala, and D. Salin. "Anomalous dispersion and finite‐size effects in hydrodynamic dispersion." Physics of Fluids A: Fluid Dynamics 2, no. 5 (May 1990): 674–80. http://dx.doi.org/10.1063/1.857720.

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38

Grechannyi, O. A., and V. V. Tokarchuk. "Anomalous hydrodynamic fluctuations during the development of thermal convection." Journal of Applied Mathematics and Mechanics 51, no. 3 (January 1987): 338–45. http://dx.doi.org/10.1016/0021-8928(87)90110-9.

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39

Broders-Bondon, Florence, Thanh Huong Nguyen Ho-Bouldoires, Maria-Elena Fernandez-Sanchez, and Emmanuel Farge. "Mechanotransduction in tumor progression: The dark side of the force." Journal of Cell Biology 217, no. 5 (February 21, 2018): 1571–87. http://dx.doi.org/10.1083/jcb.201701039.

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Cancer has been characterized as a genetic disease, associated with mutations that cause pathological alterations of the cell cycle, adhesion, or invasive motility. Recently, the importance of the anomalous mechanical properties of tumor tissues, which activate tumorigenic biochemical pathways, has become apparent. This mechanical induction in tumors appears to consist of the destabilization of adult tissue homeostasis as a result of the reactivation of embryonic developmental mechanosensitive pathways in response to pathological mechanical strains. These strains occur in many forms, for example, hypervascularization in late tumors leads to high static hydrodynamic pressure that can promote malignant progression through hypoxia or anomalous interstitial liquid and blood flow. The high stiffness of tumors directly induces the mechanical activation of biochemical pathways enhancing the cell cycle, epithelial–mesenchymal transition, and cell motility. Furthermore, increases in solid-stress pressure associated with cell hyperproliferation activate tumorigenic pathways in the healthy epithelial cells compressed by the neighboring tumor. The underlying molecular mechanisms of the translation of a mechanical signal into a tumor inducing biochemical signal are based on mechanically induced protein conformational changes that activate classical tumorigenic signaling pathways. Understanding these mechanisms will be important for the development of innovative treatments to target such mechanical anomalies in cancer.

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40

Voeltzel, Nicolas, Andrew Giuliani, Nicolas Fillot, Philippe Vergne, and Laurent Joly. "Nanolubrication by ionic liquids: molecular dynamics simulations reveal an anomalous effective rheology." Physical Chemistry Chemical Physics 17, no. 35 (2015): 23226–35. http://dx.doi.org/10.1039/c5cp03134f.

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41

Michaud, Georges, Olivier Richard, and Jacques Richer. "Main Sequence Evolution, Abundance Anomalies and Particle Transport." Highlights of Astronomy 12 (2002): 279–81. http://dx.doi.org/10.1017/s1539299600013526.

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AbstractThe availability of large atomic data bases has made it possible to calculate stellar evolution models taking into detailed account the abundance variations of all important contributors to opacity. In a first step, in addition to nuclear reactions, the atomic diffusion, radiative accelerations and opacity are continuously calculated during evolution taking the abundance changes of 28 species into account. This leads to the first self consistent main sequence stellar evolution models. In A and F stars (M≥ 1.5Mʘ) an iron peak convection zone is shown to appear at a temperature of 200000 K. The calculated surface abundance anomalies, that follow without any arbitrary parameter, are very similar to those observed in AmFm stars in open clusters except that they are larger by a factor of about 3. The second step, is then to introduce a competing hydrodynamical process. To reduce the calculated anomalies to the observed ones, turbulence has been introduced. It is found that the mixed zone must be about 5 times deeper than the iron convection zone. Detailed comparisons to a few AmFm stars have been carried out. The determination of the abundance anomalies of a large number of atomic species (20 to 30 are probably accessible) makes it possible to constrain stellar hydrodynamics. In clusters, the original abundances and age may be known and the accurate determination of surface abundances may constrain turbulence, mass loss and differential rotation when the required atomic data bases are available and used for the modeling of particle transport in stellar evolution.

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42

Yamamoto, Jun, and Koji Okano. "Anomalous Hydrodynamic Behaviors of Smectic Liquid Crystals at Low Frequencies." Japanese Journal of Applied Physics 30, Part 1, No. 4 (April 15, 1991): 754–63. http://dx.doi.org/10.1143/jjap.30.754.

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43

Gorodtsov, V. A. "The anomalous diffusion of wave disturbances in hydrodynamic-type systems." Journal of Applied Mathematics and Mechanics 67, no. 4 (January 2003): 565–74. http://dx.doi.org/10.1016/s0021-8928(03)90059-1.

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44

Yamamoto, Jun, Ken Fujita, Nobuhiko Inoue, Haruki Nakamura, and Koji Okano. "Anomalous Hydrodynamic Behavior of Smectic Liquid Crystals at Low Frequencies." Japanese Journal of Applied Physics 26, Part 2, No. 10 (October 20, 1987): L1718—L1720. http://dx.doi.org/10.1143/jjap.26.l1718.

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45

Mitkin, P. G., and V. I. Zakharov. "Macroscopic Manifestations of Quantum Anomalies in Hydrodynamics (Brief Review)." JETP Letters 113, no. 7 (March 29, 2021): 433–44. http://dx.doi.org/10.1134/s0021364021070018.

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46

MITKIN, P. G., and V. I. ZAKHAROV. "MACROSCOPIC MANIFESTATIONS OF QUANTUM ANOMALIES IN HYDRODYNAMICS (MINI-REVIEW)." ПИСЬМА В ЖУРНАЛ ЭКСПЕРИМЕНТАЛЬНОЙ И ТЕОРЕТИЧЕСКОЙ ФИЗИКИ 113, no. 7-8(4) (2021): 446–47. http://dx.doi.org/10.31857/s123456782107003x.

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47

Ng, Gim Seng, and Piotr Surówka. "One-loop effective actions and 2D hydrodynamics with anomalies." Physics Letters B 746 (June 2015): 281–84. http://dx.doi.org/10.1016/j.physletb.2015.05.011.

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48

Biferale, L., M. Cencini, A. S. Lanotte, M. Sbragaglia, and F. Toschi. "Anomalous scaling and universality in hydrodynamic systems with power-law forcing." New Journal of Physics 6 (March 18, 2004): 37. http://dx.doi.org/10.1088/1367-2630/6/1/037.

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49

Begam, Nafisa, Sivasurender Chandran, M. Sprung, and J. K. Basu. "Anomalous Viscosity Reduction and Hydrodynamic Interactions of Polymeric Nanocolloids in Polymers." Macromolecules 48, no. 18 (August 28, 2015): 6646–51. http://dx.doi.org/10.1021/acs.macromol.5b00759.

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50

Donovan, K. J., and K. Scott. "Anomalous effective hydrodynamic radius of octadecylamine functionalised single walled carbon nanotubes." Carbon 50, no. 10 (August 2012): 3807–15. http://dx.doi.org/10.1016/j.carbon.2012.04.007.

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