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  • 1
    Electronic Resource
    Electronic Resource
    Springer
    Journal of engineering physics and thermophysics 38 (1980), S. 573-580 
    ISSN: 1573-871X
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract Extremal properties are established for the solution of the problem of cohesionless normal-rupture crack formation: namely, that the true contour of a Christianovich crack corresponds to the maximum volume of the cavity. Examples of the application of this principle are considered.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    Springer
    Fluid dynamics 7 (1972), S. 226-231 
    ISSN: 1573-8507
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
    Notes: Abstract We show the applicability of Stokes' approximation at large distances from the vertex of a cone. We discuss the statement of the problem and formulate new asymptotic representations of the solution, which replace the paradoxical solution of Harrison for cone vertex angles α≥120°. A solution of the problem concerning the axially symmetric Stokes' flow of a viscous liquid in a conical diffuser was first obtained by Harrison [1] (see also [2, 3]). The velocity field of this flow has the form $$\upsilon _R = \frac{{3Q}}{{2\pi R^2 }}\frac{{\cos ^2 - \cos ^2 \alpha }}{{\left( {1 - \cos \alpha } \right)^2 \left( {1 + 2\cos \alpha } \right)}}, \upsilon _\theta = 0$$ where R and Θ are spherical coordinates, Θ=0 and Θ=α correspond, respectively, to the axis and to the wall of the diffuser, and Q is the volumetric outflow rate of the liquid. We note that the values of the velocity in this purely radial flow become infinite when the angle α approaches 120°.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    Springer
    Theoretical and computational fluid dynamics 6 (1994), S. 235-254 
    ISSN: 1432-2250
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
    Notes: Abstract Numerical simulations of the evolution equation [14] for thickness of a film flowing down a vertical fiber are presented. Solutions with periodic boundary conditions on extended axial intervals develop trains of pulse-like structures. Typically, a group of several interacting pulses (or a solitary pulse) is bracketed by spans of nearly uniform thinned film and is virtually isolated: The evolution of such a “section” is modeled as a solution with periodic boundary conditions on the corresponding, comparatively short, interval. Single-pulse sections are steady-shape traveling waveforms (“cells” of shorter-period solutions). The collision of two pulses can be either a particle-like “elastic” rebound, or—and only if a control parameter S (proportional to the average thickness) exceeds a certain critical value, S c ≈ 1—a “deeply inelastic” coalescence. A pulse which grows by a cascade of coalescences is associated with large drops observed in experiments by Quéré [39] and our S c is in excellent agreement with its laboratory value.
    Type of Medium: Electronic Resource
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