E.M. LIFSHITZ’s research while affiliated with Russian Academy of Sciences and other places

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Publications (264)


Fluid Mechanics: Landau and Lifshitz: Course of Theoretical Physics
  • Book

September 2013

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1,492 Reads

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650 Citations

L D Landau

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E M Lifshitz

Fluid Mechanics, Second Edition deals with fluid mechanics, that is, the theory of the motion of liquids and gases. Topics covered range from ideal fluids and viscous fluids to turbulence, boundary layers, thermal conduction, and diffusion. Surface phenomena, sound, and shock waves are also discussed, along with gas flow, combustion, superfluids, and relativistic fluid dynamics. This book is comprised of 16 chapters and begins with an overview of the fundamental equations of fluid dynamics, including Euler's equation and Bernoulli's equation. The reader is then introduced to the equations of motion of a viscous fluid; energy dissipation in an incompressible fluid; damping of gravity waves; and the mechanism whereby turbulence occurs. The following chapters explore the laminar boundary layer; thermal conduction in fluids; dynamics of diffusion of a mixture of fluids; and the phenomena that occur near the surface separating two continuous media. The energy and momentum of sound waves; the direction of variation of quantities in a shock wave; one- and two-dimensional gas flow; and the intersection of surfaces of discontinuity are also also considered. This monograph will be of interest to theoretical physicists.











Citations (64)


... Thermodynamics yield for the critical diameter the expression d c = 4σ/ΔG, where σ is the surface tension at the metal−matrix interface and ΔG is the bulk free energy decrease associated with the formation of the metal phase. 70 During the normal (second) growth stage, the NPs' mean size increases with time approximately as t 1/2 but the distribution remains approximately Gaussian. In the third stage, some (larger) particles grow at the expense of the disappearance of smaller ones, yielding a specific asymmetric size distribution derived by Lifshitz and Slyozov, 68 and the average size increases approximately as t 1/3 . ...

Reference:

Broadband Optical Absorption caused by Plasmonic Response of Coalesced Au Nanoparticles Embedded in a TiO2 Matrix
Chapter XII - Kinetics of phase transitions
  • Citing Article
  • January 2008

... Furthermore, according to the Euler-Bernoulli beam theory, the bending moment is proportional to the change of curvature. Without any curvature in the initial configuration, the bending moment is = − , where is bending stiffness, more specifically = ℎ 3 ∕(12(1 − 2 )) in a plane strain case, where ℎ, and are the thickness of the beam, Young's modulus and Poisson's ratio, respectively, Lifshitz et al. (1986). Furthermore, the curvature can be expressed as the rate of change of the tangent vector, = ′ ( ). ...

CHAPTER II. THE EQUILIBRIUM OF RODS AND PLATES
  • Citing Chapter
  • December 1986

... The bulk modulus measures the material's resistance to uniform compression, indicating its incompressibility [66], [67]. Poisson's ratio, the ratio of lateral to longitudinal strain, reflects the volumetric change behavior of a material under uniaxial stress and helps in assessing its deformation characteristics [68]- [77]. These mechanical properties are vital for designing materials in structural, aerospace, and electronic applications, as they determine the strength, flexibility, and resilience of the material under different conditions. ...

CHAPTER III. ELASTIC WAVES
  • Citing Chapter
  • December 1986

... However, since the density distribution profiles vary smoothly between the liquid and gas phases, h is ill defined (particularly when it is small), and it is arguably better to consider the binding potential as a function of the adsorption [see Eq. (1) below], i.e., g = g( ) [21]. Such binding potentials (or wetting energies), once extracted from microscopic models [22][23][24][25] or appropriate approximations [26][27][28], are employed as crucial elements of mesoscale hydrodynamic models where they enter as the Derjaguin (or disjoining) pressure [20,29,30]. ...

Van der Waals forces in liquid films
  • Citing Chapter
  • January 1992

... At the same time, the research of the intermediate state (IS) in the high pure type I superconductors, using the ultrasound, did not lead to any significant results (see the review [2]). As it is known345, the type I superconductors of final dimensions transit to an intermediate state, dividing on a big number of altering superconducting and normal layers of the at an action by the external magnetic field H with the magnitude of (1−n )H c <H<H c (n is the demagnetization factor of a sample). The field H is equal to the critical magnetic field value H c in the normal phase layers, and it is directed along the normal phase layers; whereas there is no any magnetic field in the diamagnetic superconducting phase layers. ...

The intermediate state of superconductors
  • Citing Chapter
  • January 1992

... Macroscopic excitations play an essential role in many areas of physics, particularly in Bose-Einstein condensates (BECs), which exhibit phenomena such as solitons [1][2][3][4][5][6][7][8][9], quantized vortices [10][11][12][13][14][15][16][17], vortex sheets [18][19][20][21][22][23][24], domain walls [25,26], textures [27][28][29]. These excitations are crucial for understanding the phase, superfluidity and magnetic properties of condensates. ...

On the rotation of liquid helium
  • Citing Chapter
  • January 1992

... Aside from its purely academic interest, its resolution has wide implications in many areas of science and technology on many disparate scales [1] [2] [3] [4] [5] [6] [7] [8] [9]. These vary from quantum optics, metamaterials , nanofluidics, nanomachinery, cold atom technology and early Universe cosmology. ...

Influence of temperature on molecular attraction forces between condensed bodies
  • Citing Chapter
  • January 1992