Cavitation in lubrication. Part 1. On boundary conditions and cavity—fluid interfaces

1977 ◽  
Vol 80 (4) ◽  
pp. 743-755 ◽  
Author(s):  
M. D. Savage

The flow of viscous lubricant in narrow gaps is considered for those geometries in which cavitation arises. A detailed review is presented of those boundary conditions which have been proposed for terminating the lubrication regime (i.e. those valid where the cavity forms). Finally it is shown that a uniform cavity-fluid interface remains stable to small disturbances provided that \[ \frac{d}{dx}\left(P+\frac{T}{r}\right) < 0, \] in which T and r represent the surface tension of the fluid and the radius of curvature of the interface respectively whilst dP/dx is the gradient of fluid pressure immediately upstream of the interface.

The paper is about free vibration problems in fuel tanks with different levels of fillers both under overloads and low gravity. The fuel tanks are considered as rigid shells of revolution. The liquid, contained in the tanks, is supposed to be an ideal and incompressible one, and its flow, induced by external excitations, is irrotational. The problem of free axisymmetric harmonic oscillations of the fluid-filled rigid compound shell is considered. The mixed boundary value problem is formulated, and boundary conditions are received on the boundaries of the fluid domain. The non-penetration conditions is formulated on the rigid shell boundaries, and on the free liquid surface there are kinematic and dynamic boundary conditions. The flow fluctuations are described by using the velocity potential that for ideal and incompressible liquids satisfies the Laplace equation. For its solution, the integral representation is in use. But there are two unknown functions, the velocity potential and the function describing the shape and position of the free surface during time. The transformation of the boundary conditions leads to eliminating one of these unknown functions. So, the system of boundary singular integral equations is obtained to determine the velocity potential. The discrete singularity method and the boundary element method are applied for its numerical solution. The problem of determining own modes and frequencies is solved by using the techniques, where the surface tension effects are neglected. Then these modes are considered as basic functions to determine the modes and frequencies of the liquid taking into account the surface tension. Thus, in this work the method is developed which takes into account the surface tension effect on the frequency of fluid fluctuations in the rigid tank under low gravity conditions. The surface of the interaction between liquid media and gas is considered as a thin membrane, whose thickness is neglected. The fluid pressure on this surface is determined by the Laplace-Young equation. The developed method is useful for the investigation of free and forced fluid oscillations in rigid compound shells with arbitrary meridians.


Soft Matter ◽  
2019 ◽  
Vol 15 (10) ◽  
pp. 2284-2291 ◽  
Author(s):  
Harinadha Gidituri ◽  
Mahesh V. Panchagnula ◽  
Andrey Pototsky

Marangoni flow created by the gradient of surface tension can be used to transport small objects along fluid interfaces.


2020 ◽  
Vol 117 (51) ◽  
pp. 32238-32243
Author(s):  
Sylvain Courrech du Pont ◽  
Jens Eggers

When a fluid interface is subjected to a strong viscous flow, it tends to develop near-conical ends with pointed tips so sharp that their radius of curvature is undetectable. In microfluidic applications, tips can be made to eject fine jets, from which micrometer-sized drops can be produced. Here we show theoretically that the opening angle of the conical interface varies on a logarithmic scale as a function of the distance from the tip, owing to nonlocal coupling between the tip and the external flow. Using this insight we are able to show that the tip curvature grows like the exponential of the square of the strength of the external flow and to calculate the universal shape of the interface near the tip. Our experiments confirm the scaling of the tip curvature as well as of the interface’s universal shape. Our analytical technique, based on an integral over the surface, may also have far wider applications, for example treating problems with electric fields, such as electrosprays.


1984 ◽  
Vol 24 (02) ◽  
pp. 203-208
Author(s):  
Mahn Won Kim ◽  
John S. Huang ◽  
Jan Bock

Abstract Thermally excited waves at the interface between two fluids contain information about the structure and tension at this interface. A surface light-scattering technique based on photon correlation spectroscopy has been developed to probe the dynamics of these interfacial waves for microemulsions. The interfacial tension (IFT) as measured by this nonperturbing technique is consistent with the values obtained by conventional methods. We have studied the temperature and salinity dependence of sigma (IFT) in a three-phase microemulsion system, and found that sigma epsilon, where epsilon is the reduced variable and with and representing the critical values of temperature and salinity, respectively. Furthermore, the correlation length, L, in the microemulsion phase has also been measured by dynamic light scattering. In the two-phase regions it was observed that, in accordance with the scaling law predictions. Thus, the scaled salinity and temperature parameters influence the IFT through their effect on the correlation length in the bulk microemulsion phase. phase. Introduction The tension and the structure of a fluid interface have been well studied subjects for those who are interested in thermodynamics, surface properties, hydrodynamics, and a host of practical applications, including properties, hydrodynamics, and a host of practical applications, including chemical EOR. About 100 years ago, van der Waals recognized the special relation between the vanishing of interfacial (surface) tension and the critical point transitions in fluids and fluid mixtures. This relation linked the bulk properties of liquids to their interfacial behavior. More recent investigations into the structure and the tension of the critical interface have shown that van der Waals was qualitatively correct. It was also recognized by Mandelstam in 1913 that a vanishing IFT would lead to increasing amplitude in the spontaneous thermal fluctuation on the interface. This prediction could be understood in the following manner. Interface fluctuations are produced by the random thermal motions of fluid molecules. Consequently, these fluctuations cause the interface to deviate from a planar surface, which corresponds to the minimum free-energy state of the system. The lower the IFT, the easier it is for the interfacial area to increase by producing large amplitudes in fluctuations. Mathematically, we can describe these fluctuations by their Fourier components, each corresponding to a particular normal mode of the surface wave (capillary wave), subjected to the boundary conditions of the container. After the invention of optical mixing spectroscopy, Katyl and Ingard first demonstrated that the surface tension of a free liquid could be measured by light scattering. Huang and Webbs then took advantage of the vanishing IFT and density difference in a binary liquid mixture near the critical point, to develop a correlation spectroscopy. This technique analyzed the scattered light from the diverging interfacial capillary waves on the critical interface. This method allows one to determine extremely low IFT's in the range of 10 -5 to 10 -6 mN/m [10 -5 to 10 -6 dyne/cm] without perturbing the system. The advantages of determining IFT by using an optical probe over the conventional means involving direct or indirect measurements of the mechanical restoring forces are higher sensitivity and complete equilibrium of the surface under study. Furthermore, optical techniques can be used to study fluids at elevated pressures and temperatures. This optical technique was used to study the relation between the IFT of a microemulsion and its bulk properties. Scaling concepts have been used to interpret the data. Even though the scaling laws were developed to describe the critical phenomena, there is evidence to show that these are relevant and useful concepts, especially for the understanding of low-tension microemulsion systems. Light Scattering From Interfacial Capillary Waves Capillary waves are described by the solutions of the linearized Navier-Stokes equation in a uniform gravitational field, subject to boundary conditions at the fluid interface and infinity. The restoring forces are the gravitational force and the IFT. Interfacial and bulk shear viscosity provide the damping mechanism. A detailed derivation of the dispersion relation can be found in Ref. 14. The major conclusion is that for a low tension interface, the normal modes that can be easily probed by visible light are over damped waves with time constant, given by the expression ............................(1) SPEJ p. 203


Soft Matter ◽  
2014 ◽  
Vol 10 (36) ◽  
pp. 6999-7007 ◽  
Author(s):  
Antonio Stocco ◽  
Ge Su ◽  
Maurizio Nobili ◽  
Martin In ◽  
Dayang Wang

Contact angles and surface coverage of nanoparticles adsorbing at the fluid interface are assessed by ellipsometry. Results reveal the competition between wetting and colloidal interactions.


1990 ◽  
Vol 112 (1) ◽  
pp. 47-56 ◽  
Author(s):  
S. Yossifon ◽  
J. Tirosh

The concept of Maximum Drawing Ratio (MDR), supplementary to the well-known Limit Drawing Ratio (LDR), is defined, examined, and illustrated by experiments. In essence the MDR is reached when the two basic failure modes, namely: rupture (due to tensile instability) and wrinkling (due to buckling instability) are delayed till they occur simultaneously. Thus the process is beneficially utilized for higher drawing ratio by postponing earlier interception of either one of the above failures alone. The ability to suppress (up to a certain extent) the appearance of these failure modes depends heavily on the fluid-pressure path which controls the hydroforming process. The effect of the material properties, like the strain hardening exponent, the normal anisotropy of the blank, etc., as well as the geometrical properties (i.e., the thickness of the blank, the radius of curvature at the lip, etc.) on the MDR, are considered here in some detail. The nature of the solutions by which MDR is reached is discussed.


Author(s):  
Benjamin Sauer ◽  
Nikolaos Spyrou ◽  
Amsini Sadiki ◽  
Johannes Janicka

The primary breakup under high-altitude relight conditions is investigated in this study where ambient pressure is as low as 0.4 bar and air, fuel and engine parts are as cold as 265 K. The primary breakup is crucial for the fuel atomization. As of today, the phenomena dictating the primary breakup are not fully understood. Direct Numerical Simulations (DNS) of liquid breakup under realistic conditions and geometries are hardly possible. The embedded DNS (eDNS) approach represents a reliable numerical tool to fill this gap. The concept consists of three steps: a geometry simplification, the generation of realistic boundary conditions for the DNS and the DNS of the breakup region. The realistic annular airblast atomizer geometry is simplified to a Y-shaped channel representing a planar geometry. Inside this domain the eDNS is located. The eDNS domain requires the generation of boundary conditions. A Large Eddy Simulation (LES) of the entire Y-shaped channel and a Reynolds-Averaged Navier-Stokes Simulation (RANS) of the liquid wall film are performed prior to the DNS. All parameters are stored transiently on all virtual DNS planes. These variables are then mapped to the DNS. Thus, high-quality boundary conditions are generated. The Volume-of-Fluid (VOF) method is used to solve for the two-phase flow. The results provide a qualitative insight into the primary breakup under realistic high-altitude relight conditions. Instantaneous snapshots in time illustrate the behavior of the liquid wall film along the prefilmer lip and illustrate the breakup process. It is seen that a slight variation of the surface tension force has a strong impact on the appearance of the primary breakup. Case 1 with the surface tension corresponding to kerosene at 293 K indicates large flow structures that are separated from the liquid sheet. By lowering the surface tension related to kerosene at 363 K, the breakup is dominated by numerous small structures and droplets. This study proves the applicability of the eDNS concept for investigating breakup processes as the transient nature of the phase interface behavior can be captured. At this time, the authors only present a qualitative insight which can be explained by the lack of quantitative data. The approach offers the potential of simulating realistic annular highly-swirled airblast atomizer geometries under realistic conditions.


2021 ◽  
Vol 54 (1) ◽  
Author(s):  
Charles Maldarelli ◽  
Nicole T. Donovan ◽  
Subramaniam Chembai Ganesh ◽  
Subhabrata Das ◽  
Joel Koplik

Colloid-sized particles (10 nm–10 μm in characteristic size) adsorb onto fluid interfaces, where they minimize their interfacial energy by straddling the surface, immersing themselves partly in each phase bounding the interface. The energy minimum achieved by relocation to the surface can be orders of magnitude greater than the thermal energy, effectively trapping the particles into monolayers, allowing them freedom only to translate and rotate along the surface. Particles adsorbed at interfaces are models for the understanding of the dynamics and assembly of particles in two dimensions and have broad technological applications, importantly in foam and emulsion science and in the bottom-up fabrication of new materials based on their monolayer assemblies. In this review, the hydrodynamics of the colloid motion along the surface is examined from both continuum and molecular dynamics frameworks. The interfacial energies of adsorbed particles is discussed first, followed by the hydrodynamics, starting with isolated particles followed by pairwise and multiple particle interactions. The effect of particle shape is emphasized, and the role played by the immersion depth and the surface rheology is discussed; experiments illustrating the applicability of the hydrodynamic studies are also examined. Expected final online publication date for the Annual Review of Fluid Mechanics, Volume 54 is January 2022. Please see http://www.annualreviews.org/page/journal/pubdates for revised estimates.


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