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1

Holt, Maurice, Graham F. Carey, and J. Tinsley Oden. "Finite Elements: Fluid Mechanics." Mathematics of Computation 52, no. 185 (1989): 249. http://dx.doi.org/10.2307/2008669.

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2

Barnes, H. A. "Fluid Mechanics." Journal of Non-Newtonian Fluid Mechanics 37, no. 2-3 (1990): 387. http://dx.doi.org/10.1016/0377-0257(90)90014-3.

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3

Cartwright, Julyan H. E., and Oreste Piro. "The fluid mechanics of poohsticks." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 378, no. 2179 (2020): 20190522. http://dx.doi.org/10.1098/rsta.2019.0522.

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The year 2019 marked the bicentenary of George Gabriel Stokes, who in 1851 described the drag—Stokes drag—on a body moving immersed in a fluid, and 2020 is the centenary of Christopher Robin Milne, for whom the game of poohsticks was invented; his father A. A. Milne’s The House at Pooh Corner , in which it was first described in print, appeared in 1928. So this is an apt moment to review the state of the art of the fluid mechanics of a solid body in a complex fluid flow, and one floating at the interface between two fluids in motion. Poohsticks pertains to the latter category, when the two fluids are water and air. This article is part of the theme issue ‘Stokes at 200 (part 2)’.
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4

Manikta Puspitasari, M. Dewi, Kuni Nadliroh, and Muhammad Najibulloh Muzaki. "Students’ Epistemic Game according to SOLO Taxonomy in Completing Fluid Mechanics Problem." Jurnal Pembelajaran Fisika 8, no. 2 (2019): 167–75. http://dx.doi.org/10.23960/jpf.v8.n2.202005.

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The purpose of this study is to describe the students’ epistemic game of high physics-capable. This study is qualitative. The participants are students taking fluid mechanics courses. The collect data of this study use fluid mechanics test, physics understanding test, and interview. The understanding test determines the students’ understanding level, while the determining students’ epistemic game by SOLO taxonomy uses the fluid mechanic's test. The students complete the first test by using mapping mathematics to meaning at a relational level and transliteration to mathematics at a multi structural level. Pictorial analysis in level extended abstract and transliteration to mathematics in level relational are used by the students in completing the problem of the second test. Meanwhile, this study result showed that mapping mathematics to the meaning and recursive plug and chug at a relational level is used by the students for completing the third test. Furthermore, the students completing the fourth test used transliteration to mathematics and recursive plug and chug at a relational level The students’ epistemic game by SOLO taxonomy of this study can be used to develop physics learning. Keywords: epistemic game, SOLO taxonomy, fluid mechanics
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5

Et. al., Santosh Jakapure,. "Regular Pertibution Solutions In Fluid Mechanics." Turkish Journal of Computer and Mathematics Education (TURCOMAT) 12, no. 2 (2021): 1578–84. http://dx.doi.org/10.17762/turcomat.v12i2.1436.

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Disregarding the fast advances in both scalar and equal computational devices, the huge number and expansiveness of factors associated with both plan and opposite issues utilize refined and even generally straightforward (parabolized or limit layer) liquid stream models unreasonable. With this limitation, it very well might be presumed that a significant group of strategies for numerical/computational advancement are decreased or surmised models. In this examination a joined perturbation/mathematical displaying approach is created which will give a thoroughly inferred chain of importance of arrangements. These arrangements are described by changing degrees of unpredictability versus logical devotion.
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6

ZAGANESCU, Nicolae-Florin, Rodica ZAGANESCU, and Constantin-Marcian GHEORGHE. "Academician CAIUS IACOB – a Brilliant Mathematician Fascinated by Mechanics." INCAS BULLETIN 12, no. 1 (2020): 243–48. http://dx.doi.org/10.13111/2066-8201.2020.12.1.23.

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The paper presents some interesting aspects related to the biography and works of Romanian mathematician Caius Iacob (1912–1992). He was famous for his works in the fields of mathematical analysis, fluid mechanics, classical hydrodynamics and compressible-flow theory. At the age of 19, he graduated from the Mathematics Faculty in Bucharest, and then he went to Paris to continue his studies at the Faculty of Sciences, where he worked on a PhD thesis under the advice of famous French mathematician Henri Villat. On 24 June 1935, Caius Iacob successfully presented to the Sorbonne committee his PhD thesis about “Determination of conjugated harmonic functions with some limit conditions, and their applications in hydrodynamics”. Returning to Romania, Caius Iacob had a long and successful career teaching mathematics and mechanics at the universities of Timişoara, Cluj and Bucharest. His most important work is considered the “Mathematical introduction to the mechanics of fluids”. This book, providing original ways to work with classical hydrodynamics and compressible-flow theory, was published in Romanian in 1952 and in French in 1959. In 1955, he was elected a Corresponding Member of the Romanian Academy, becoming a titular Member in 1963. He was also President of the Mathematics Section of the Romanian Academy from 1980 until the end of his life, in 1992. In 1991, he initiated the foundation of the “Romanian Academy Institute of Applied Mathematics”. In 2001 the institute merged with the “Centre for Mathematical Statistics”, which had been created in 1964 by mathematician Gheorghe Mihoc, thus creating the “Gheorghe Mihoc – Caius Iacob Institute of Mathematical Statistics and Applied Mathematics” of the Romanian Academy.
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7

Feistauer, M. "Analysis in Compressible Fluid Mechanics." ZAMM 78, no. 9 (1998): 579–96. http://dx.doi.org/10.1002/(sici)1521-4001(199809)78:9<579::aid-zamm579>3.0.co;2-c.

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8

Craik, Alex D. D. "Thomas Young on fluid mechanics." Journal of Engineering Mathematics 67, no. 1-2 (2009): 95–113. http://dx.doi.org/10.1007/s10665-009-9298-7.

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9

Bazilevs, Yuri, Kenji Takizawa, and Tayfun E. Tezduyar. "Special issue on computational fluid mechanics and fluid–structure interaction." Computational Mechanics 48, no. 3 (2011): 245. http://dx.doi.org/10.1007/s00466-011-0621-6.

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10

Smith, D. J., A. A. Smith, and J. R. Blake. "Mathematical embryology: the fluid mechanics of nodal cilia." Journal of Engineering Mathematics 70, no. 1-3 (2010): 255–79. http://dx.doi.org/10.1007/s10665-010-9383-y.

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11

Fomin, N. A. "Speckle Photography for Fluid Mechanics Measurements." Measurement Science and Technology 11, no. 7 (2000): 1088. http://dx.doi.org/10.1088/0957-0233/11/7/703.

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12

I., E., Dale A. Anderson, John C. Tannehill, and Richard H. Pletcher. "Computational Fluid Mechanics and Heat Transfer." Mathematics of Computation 46, no. 174 (1986): 764. http://dx.doi.org/10.2307/2008017.

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13

Shankar, P. N., and R. Kidambi. "The contact angle in inviscid fluid mechanics." Proceedings Mathematical Sciences 115, no. 2 (2005): 227–40. http://dx.doi.org/10.1007/bf02829629.

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14

WILLANDER, M., E. MAMONTOV, and Z. CHIRAGWANDI. "MODELLING LIVING FLUIDS WITH THE SUBDIVISION INTO THE COMPONENTS IN TERMS OF PROBABILITY DISTRIBUTIONS." Mathematical Models and Methods in Applied Sciences 14, no. 10 (2004): 1495–520. http://dx.doi.org/10.1142/s0218202504003702.

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As it follows from the results of C. H. Waddigton, F. E. Yates, A. S. Iberall, and other well-known bio-physicists, living fluids cannot be modelled within the frames of the fundamental assumptions of the statistical-mechanics formalism. One has to go beyond them. The present work does it by means of the generalized kinetics (GK), the theory enabling one to allow for the complex stochasticity of internal properties and parameters of the fluid particles. This is one of the key features which distinguish living fluids from the nonliving ones. It creates the disparity of the particles and hence breaks the each-fluid-component-uniformity requirement underlying statistical mechanics. The work deals with the corresponding modification of common kinetic equations which is in line with the GK theory and is the complement to the latter. This complement allows a subdivision of a fluid into the fluid components in terms of nondiscrete probability distributions. The treatment leads to one more equation that describes the above internal parameters. The resulting model is the system of these two equations. It appears to be always nonlinear in case of living fluids. In case of nonliving fluids, the model can be linear. Moreover, the living-fluid model, as a whole, cannot have the thermodynamic equilibrium, only partial equilibriums (such as the motional one) are possible. In contrast to this, in case of nonliving fluids, the thermodynamic equilibrium is, of course, possible. The number of the fluid components is treated as the number of the modes of the particle-characteristic probability density. In so doing, a fairly general extension of the notion of the mode from the one-dimensional case to the multidimensional case is proposed. The work also discusses the variety of the time-scales in a living fluid, the simplest quantum-mechanical equation relevant to living fluids, and the non-equilibrium nonlinear stochastic hydrodynamics option. The latter is simpler than, but conceptually comparable to, stochastic kinetic equations. A few directions for future research are suggested. The work notes a cohesion of mathematical physics and fluid mechanics with the living-fluid-related fields as a complex interdisciplinary problem.
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15

Gerard-Varet, David. "Formal Derivation of Boundary Layers in Fluid Mechanics." Journal of Mathematical Fluid Mechanics 7, no. 2 (2005): 179–200. http://dx.doi.org/10.1007/s00021-004-0115-9.

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16

Ellahi, Rahmat. "Special Issue on Symmetry and Fluid Mechanics." Symmetry 12, no. 2 (2020): 281. http://dx.doi.org/10.3390/sym12020281.

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This Special Issue invited researchers to contribute their original research work and review articles on “Symmetry and Fluid Mechanics” that either advances the state-of-the-art mathematical methods through theoretical or experimental studies or extends the bounds of existing methodologies with new contributions related to the symmetry, asymmetry, and lie symmetries of differential equations proposed as mathematical models in fluid mechanics, thereby addressing current challenges. In response to the call for papers, a total of 42 papers were submitted for possible publication. After comprehensive peer review, only 25 papers qualified for acceptance for final publication. The rest of the papers could not be accommodated. The submissions may have been technically correct but were not considered appropriate for the scope of this Special Issue. The authors are from geographically distributed countries such as the USA, Australia, China, Saudi Arabia, Iran, Pakistan, Malaysia, Abu Dhabi, UAE, South Africa, and Vietnam. This reflects the great impact of the proposed topic and the effective organization of the guest editorial team of this Special Issue.
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17

Spelce, T. "Finite element computational fluid mechanics." Finite Elements in Analysis and Design 1, no. 4 (1985): 389–90. http://dx.doi.org/10.1016/0168-874x(85)90035-6.

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18

Misra, J. C., G. C. Shit, S. Chandra, and P. K. Kundu. "Electro-osmotic flow of a viscoelastic fluid in a channel : Applications to physiological fluid mechanics." Applied Mathematics and Computation 217, no. 20 (2011): 7932–39. http://dx.doi.org/10.1016/j.amc.2011.02.075.

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19

de Souza Mendes, Paulo R. "Dimensionless non-Newtonian fluid mechanics." Journal of Non-Newtonian Fluid Mechanics 147, no. 1-2 (2007): 109–16. http://dx.doi.org/10.1016/j.jnnfm.2007.07.010.

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20

W.F.A. "Ocean waves mechanics, computational fluid dynamics, and mathematical modelling." Mathematics and Computers in Simulation 33, no. 2 (1991): 179. http://dx.doi.org/10.1016/0378-4754(91)90173-z.

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21

Marchioro, Carlo, and Piero Negrini. "On a dynamical system related to fluid mechanics." NoDEA : Nonlinear Differential Equations and Applications 6, no. 4 (1999): 473–99. http://dx.doi.org/10.1007/s000300050013.

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22

GUSTAFSSON, BERTIL. "Analysis and Methods in Fluid Mechanics." International Journal of Modern Physics C 02, no. 01 (1991): 75–85. http://dx.doi.org/10.1142/s0129183191000093.

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When constructing numerical methods for partial differential equations, it is important to have a thorough understanding of the continuous model and the characteristic properties of its solutions. We shall present methods of analysis for determining well-posedness of hyperbolic and mixed hyperbolic-parabolic équations which are applicable to the time-dependent Euler and Navier-Stokes equations. We shall then discuss difference- and finite volume methods and the construction of grids. The geometry of realistic problems is usually such that it is almost impossible to construct one structured grid. One way to overcome this difficulty is to use overlapping grids, where each domain has a structured grid. We discuss stability and accuracy of difference methods applied on such grids. Many problems in physics and engineering are defined in boundary domains, and artificial boundaries are introduced for computational reasons. In some cases one can construct accurate boundary conditions at these open boundaries. We shall indicate how this can be achieved, but we will also point out certain cases where accurate solutions are impossible to be obtained on limited domains. Finally some comments will be given on the difficulties arising when almost incompressible flow is computed. This corresponds to small Mach-numbers, and extra care must be taken when designing numerical methods. The theory will be complemented by numerical experiments for various flow problems in two space dimensions.
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23

Renardy, Michael. "Mathematical Topics in Fluid Mechanics (J. F. Rodrigues and A. Sequeira)." SIAM Review 36, no. 1 (1994): 139–40. http://dx.doi.org/10.1137/1036040.

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24

Nithiarasu, P., and O. C. Zienkiewicz. "Adaptive mesh generation for fluid mechanics problems." International Journal for Numerical Methods in Engineering 47, no. 1-3 (2000): 629–62. http://dx.doi.org/10.1002/(sici)1097-0207(20000110/30)47:1/3<629::aid-nme786>3.0.co;2-y.

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25

Tan, Changhui. "Singularity formation for a fluid mechanics model with nonlocal velocity." Communications in Mathematical Sciences 17, no. 7 (2019): 1779–94. http://dx.doi.org/10.4310/cms.2019.v17.n7.a2.

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26

Liu, Zheng, Jing Zhu, and Lian Cun Zheng. "Research on Fluid Mechanics with Slip Flow of Viscoelastic Fluid in the Micro Channel." Applied Mechanics and Materials 387 (August 2013): 51–54. http://dx.doi.org/10.4028/www.scientific.net/amm.387.51.

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Stagnation flow, an import research branch of fluid mechanics, describing the fluid motion near the stagnation region, exists on all solid bodies moving in a fluid. And stagnation point boundary layer flow problems described by partial differential equations have attracted many scholars attention nowadays. These problems have become difficult and hot in the study of applied mathematics, mechanics and materials engineering. This paper has transformed the governing boundary layer equations into a system of nonlinear differential equations through the similarity transformation, and the analytical approximations of solutions are derived by homotopy analysis method (HAM). In addition, the effects of physical factors (such as the slip parameter, Magnetic field parameter and Reynolds number) on the flow are examed and discussed graphically. They have a great impact on the speed.
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27

Yin, Chen, Chunwu Wang, and Shaowei Wang. "Thermal instability of a viscoelastic fluid in a fluid-porous system with a plane Poiseuille flow." Applied Mathematics and Mechanics 41, no. 11 (2020): 1631–50. http://dx.doi.org/10.1007/s10483-020-2663-7.

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Abstract The thermal convection of a Jeffreys fluid subjected to a plane Poiseuille flow in a fluid-porous system composed of a fluid layer and a porous layer is studied in the paper. A linear stability analysis and a Chebyshev τ-QZ algorithm are employed to solve the thermal mixed convection. Unlike the case in a single layer, the neutral curves of the two-layer system may be bi-modal in the proper depth ratio of the two layers. We find that the longitudinal rolls (LRs) only depend on the depth ratio. With the existence of the shear flow, the effects of the depth ratio, the Reynolds number, the Prandtl number, the stress relaxation, and strain retardation times on the transverse rolls (TRs) are also studied. Additionally, the thermal instability of the viscoelastic fluid is found to be more unstable than that of the Newtonian fluid in a two-layer system. In contrast to the case for Newtonian fluids, the TRs rather than the LRs may be the preferred mode for the viscoelastic fluids in some cases.
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28

Marušić-Paloka, Eduard. "Mathematical modeling of junctions in fluid mechanics via two-scale convergence." Journal of Mathematical Analysis and Applications 480, no. 1 (2019): 123399. http://dx.doi.org/10.1016/j.jmaa.2019.123399.

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29

Saunders, H. "Finite elements—Fluid mechanics, Vol. VI." Finite Elements in Analysis and Design 3, no. 4 (1987): 355–57. http://dx.doi.org/10.1016/0168-874x(87)90016-3.

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30

Mironer, Alan. "An Informal Introduction to Theoretical Fluid Mechanics (James Lighthill)." SIAM Review 30, no. 3 (1988): 523–24. http://dx.doi.org/10.1137/1030121.

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31

Manguoglu, Murat, Kenji Takizawa, Ahmed H. Sameh, and Tayfun E. Tezduyar. "A parallel sparse algorithm targeting arterial fluid mechanics computations." Computational Mechanics 48, no. 3 (2011): 377–84. http://dx.doi.org/10.1007/s00466-011-0619-0.

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32

Takizawa, Kenji, Tayfun E. Tezduyar, Austin Buscher, and Shohei Asada. "Space–time fluid mechanics computation of heart valve models." Computational Mechanics 54, no. 4 (2014): 973–86. http://dx.doi.org/10.1007/s00466-014-1046-9.

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33

Not Available, Not Available. "First M.I.T. Conference on Computational Fluid and Solid Mechanics." Computational Mechanics 25, no. 5 (2000): 514. http://dx.doi.org/10.1007/s004660050498.

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34

Knight, D. G. "Revisiting Newtonian and non-Newtonian fluid mechanics using computer algebra." International Journal of Mathematical Education in Science and Technology 37, no. 5 (2006): 573–92. http://dx.doi.org/10.1080/03091900600712215.

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35

Hosseinzadeh, Elham, Amin Barari, Fama Fouladi, and Ganji Domairry. "Numerical analysis of forth-order boundary value problems in fluid mechanics and mathematics." Thermal Science 14, no. 4 (2010): 1101–9. http://dx.doi.org/10.2298/tsci1004101h.

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36

Hämäläinen, Jari, Taija Hämäläinen, Teemu Leppänen, Heidi Niskanen, and Joonas Sorvari. "Mathematics in paper - from fiber suspension fluid dynamics to solid state paper mechanics." Journal of Mathematics in Industry 4, no. 1 (2014): 14. http://dx.doi.org/10.1186/2190-5983-4-14.

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37

Ionescu, C. M., I. R. Birs, D. Copot, C. I. Muresan, and R. Caponetto. "Mathematical modelling with experimental validation of viscoelastic properties in non-Newtonian fluids." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 378, no. 2172 (2020): 20190284. http://dx.doi.org/10.1098/rsta.2019.0284.

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The paper proposes a mathematical framework for the use of fractional-order impedance models to capture fluid mechanics properties in frequency-domain experimental datasets. An overview of non-Newtonian (NN) fluid classification is given as to motivate the use of fractional-order models as natural solutions to capture fluid dynamics. Four classes of fluids are tested: oil, sugar, detergent and liquid soap. Three nonlinear identification methods are used to fit the model: nonlinear least squares, genetic algorithms and particle swarm optimization. The model identification results obtained from experimental datasets suggest the proposed model is useful to characterize various degree of viscoelasticity in NN fluids. The advantage of the proposed model is that it is compact, while capturing the fluid properties and can be identified in real-time for further use in prediction or control applications. This article is part of the theme issue ‘Advanced materials modelling via fractional calculus: challenges and perspectives’.
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38

Hamouda, Makram, Jean Michel Rakotoson, and Cédric Verbeke. "Qualitative properties of some equations related to fluid mechanics." Nonlinear Analysis: Theory, Methods & Applications 60, no. 3 (2005): 501–14. http://dx.doi.org/10.1016/j.na.2004.09.025.

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39

HAMOUDA, M., J. RAKOTOSON, and C. VERBEKE. "Qualitative properties of some equations related to fluid mechanics." Nonlinear Analysis 60, no. 3 (2005): 501–14. http://dx.doi.org/10.1016/s0362-546x(04)00391-8.

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40

Platzer, Bernd. "Book Review: Franz Durst: Fluid Mechanics - An Introduction to the Theory of Fluid Flows." ZAMM - Journal of Applied Mathematics and Mechanics / Zeitschrift für Angewandte Mathematik und Mechanik 90, no. 12 (2010): 919. http://dx.doi.org/10.1002/zamm.201090018.

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41

Březina, Jan. "Asymptotic Properties of Solutions to the Equations of Incompressible Fluid Mechanics." Journal of Mathematical Fluid Mechanics 12, no. 4 (2009): 536–53. http://dx.doi.org/10.1007/s00021-009-0301-x.

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42

Moffatt, H. K. "George Keith Batchelor. 8 March 1920 – 30 March 2000." Biographical Memoirs of Fellows of the Royal Society 48 (January 2002): 25–41. http://dx.doi.org/10.1098/rsbm.2002.0002.

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George Batchelor was a pioneering figure in two branches of fluid dynamics: turbulence, in which he became a world leader over the 15 years from 1945 to 1960; and suspension mechanics (or ‘microhydrodynamics’), which developed under his initial impetus and continuing guidance throughout the 1970s and 1980s. He also exerted great influence in establishing a universally admired standard of publication in fluid dynamics through his role as founder Editor of the Journal of Fluid Mechanics , the leading journal of the subject, which he edited continuously over four decades. His famous textbook, An introduction to fluid dynamics , first published in 1967, showed the hand of a great master of the subject. Together with D. Küchemann, F.R.S., he established in 1964 the European Mechanics Committee (forerunner of the present European Society for Mechanics), which over the 24-year period of his chairmanship supervised the organization of no fewer than 230 European Mechanics Colloquia spanning the whole field of fluid and solid mechanics; while within Cambridge, where he was a Fellow of Trinity College and successively Lecturer, Reader and Professor of Applied Mathematics, he was an extraordinarily effective Head of the Department of Applied Mathematics and Theoretical Physics from its foundation in 1959 until his retirement in 1983.
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43

Burton, G. R., and J. F. Toland. "Ludwig Edward Fraenkel. 28 May 1927—27 April 2019." Biographical Memoirs of Fellows of the Royal Society 69 (October 7, 2020): 175–201. http://dx.doi.org/10.1098/rsbm.2020.0014.

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Edward Fraenkel’s professional career began as an experimentalist at the Royal Aircraft Establishment, Farnborough, but his preoccupation with the theoretical and mathematical aspects of aerodynamics led him into academia, working initially in aerodynamics and classical applied mathematics, but later in the modern theory of nonlinear partial differential equations and its applications to fluid mechanics. He made outstanding contributions to the mathematical theories of viscous flow separation, steady vortex rings and surface waves on water.
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44

Win, Ko Ko, and A. N. Temnov. "A THEORETICAL STUDY OF OSCILLATIONS OF TWO IMMISCIBLE FLUIDS IN A LIMITED TANK." Vestnik Tomskogo gosudarstvennogo universiteta. Matematika i mekhanika, no. 69 (2021): 97–113. http://dx.doi.org/10.17223/19988621/69/8.

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In the paper, the nonlinear oscillations of a two-layer fluid that completely fills a limited tank are theoretically studied. To determine any smooth function on the deflected interface, the Taylor series expansions are considered using the values of the function and its normal derivatives on the undisturbed interface of the fluids. Using two fundamental asymmetric harmonics, which are generated in two mutually perpendicular planes, the differential equations of nonlinear oscillations of the two-layer fluid interface are investigated. As a result, the frequency-response characteristics are presented and the instability regions of the forced oscillations of the two-layer fluid in the cylindrical tank are plotted, as well as the parametric resonance regions for different densities of the upper and lower fluids. The Bubnov-Galerkin method is used to plot instability regions for the approximate solution to nonlinear differential equations. At the final stage of the work, the nonlinear effects resulting from the interaction of fluids with a rigid tank that executes harmonic oscillations at the interface of the fluids are theoretically studied.
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45

Makinde, Oluwole Daniel, Waqar Ahmed Khan, and Tirivanhu Chinyoka. "New Developments in Fluid Mechanics and Its Engineering Applications." Mathematical Problems in Engineering 2013 (2013): 1–3. http://dx.doi.org/10.1155/2013/797390.

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46

Subba Reddy Gorla, Rama, and Nagasekhar Reddy Gorla. "Probabilistic finite element analysis in fluid mechanics." International Journal of Numerical Methods for Heat & Fluid Flow 13, no. 7 (2003): 849–61. http://dx.doi.org/10.1108/09615530310502064.

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47

MAYNE, GEORGES. "GEOMETRICAL METHOD IN NON-NEWTONIAN FLUID MECHANICS." Quarterly Journal of Mechanics and Applied Mathematics 42, no. 2 (1989): 239–47. http://dx.doi.org/10.1093/qjmam/42.2.239.

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48

Shail, R. "Some regular perturbation solutions in fluid mechanics." Quarterly Journal of Mechanics and Applied Mathematics 50, no. 1 (1997): 129–48. http://dx.doi.org/10.1093/qjmam/50.1.129.

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49

Cyron, Christian J., Keijo Nissen, Volker Gravemeier, and Wolfgang A. Wall. "Stable meshfree methods in fluid mechanics based on Green’s functions." Computational Mechanics 46, no. 2 (2009): 287–300. http://dx.doi.org/10.1007/s00466-009-0405-4.

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50

Ramkissoon, H. "Flow of a Micropolar Fluid Past a Newtonian Fluid Sphere." ZAMM - Journal of Applied Mathematics and Mechanics / Zeitschrift für Angewandte Mathematik und Mechanik 65, no. 12 (1985): 635–37. http://dx.doi.org/10.1002/zamm.19850651218.

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