Formation regularities of liquid body of Dombrovsky quarry

Author(s):  
Y. Malkova ◽  
V. Dolin ◽  
Y. Yakovlev
Keyword(s):  
2019 ◽  
Vol 72 (10) ◽  
Author(s):  
Palmira G Petrova ◽  
Eya E Egorova ◽  
Victoriya E Egorova ◽  
Semen E Grigor'ev ◽  
Lena R Turkebaeva
Keyword(s):  

2014 ◽  
Vol 743 ◽  
Author(s):  
Stefan Karpitschka ◽  
Hans Riegler

AbstractUnexpectedly, under certain conditions, sessile drops from different but completely miscible liquids do not always coalesce instantaneously upon contact: the drop bodies remain separated in a temporary state of non-coalescence, connected through a thin liquid bridge. Here we investigate the transition between the states of instantaneous coalescence and temporary non-coalescence. Experiments reveal that it is barely influenced by viscosities and absolute surface tensions. The main system control parameters for the transition are the arithmetic means of the three-phase angles, $\overline{\Theta }_{a}$, and the surface tension differences $\Delta \gamma $ between the two liquids. These relevant parameters can be combined into a single system parameter, a specific Marangoni number $\widetilde{M}=3\Delta \gamma /(2\overline{\gamma }\overline{\Theta }_{a}^2)$. This $\widetilde{M}$ universally characterizes the coalescence transition behaviour as a function of both the physicochemical liquid properties and the shape of the liquid body in the contact region. The transition occurs at a certain threshold value $\widetilde{M}_t$ and is sharp within the experimental resolution. The experimentally observed threshold value of $\widetilde{M}_t\approx 2$ agrees quantitatively with values obtained by simulations assuming realistic material parameters. The simulations indicate that the absolute value of $\widetilde{M}_t$ very weakly depends on the molecular diffusivity.


1997 ◽  
Vol 337 ◽  
pp. 49-66 ◽  
Author(s):  
Q. CHEN ◽  
E. RAMÉ ◽  
S. GAROFF

The dynamics of a spreading liquid body are dictated by the interface shape and flow field very near the moving contact line. The interface shape and flow field have been described by asymptotic models in the limit of small capillary number, Ca. Previous work established the validity and limitations of these models of the interface shape (Chen et al. 1995). Here, we study the flow field near the moving contact line. Using videomicroscopy, particle image velocimetry, and digital image analysis, we simultaneously make quantitative measurements of both the interface shape and flow field from 30 μm to a few hundred microns from the contact line. We compare our data to the modulated-wedge solution for the velocity field near a moving contact line (Cox 1986). The measured flow fields demonstrate quantitative agreement with predictions for Ca[les ]0.1, but deviations of ∼5% of the spreading velocity at Ca≈0.4. We observe that the interface shapes and flow fields become geometry independent near the contact line. Our experimental technique provides a way of measuring the interface shape and velocity field to be used as boundary conditions for numerical calculations of the macroscopic spreading dynamics.


2015 ◽  
Vol 38 (11) ◽  
Author(s):  
Matthew Lai Ho Chong ◽  
Michael Cheng ◽  
Mayur Katariya ◽  
Murat Muradoglu ◽  
Brandon Huey-Ping Cheong ◽  
...  

1864 ◽  
Vol 13 ◽  
pp. 335-341 ◽  

The prevalent notions respecting solubility have been derived chiefly from observations on crystalline salts, and are very imperfectly applicable to the ss of colloidal substances. Hydrated silicic acid, for instance, when in a soluble condition, is property, speaking a liquid body, like alcohol, scible with water in all proportions. We have no degrees of solubility speak of with respect to silicic acid, like the gelatinous condition, which is usually looked upon as destitute of solubility. The jelly of silicic acid may be more or less rich in combined water, as it is first pre-red, and it appears to be soluble in proportion to the extent of its hydragon. A jelly containing 1 per cent. of silicic acid, gives with cold water solution containing about 1 of silicic acid in 5000 water; a jelly con-ining 5 per cent. of silicic acid, gives a solution containing about 1 per acid in 10,000 water. A less hydrated jelly than the last mentioned still less soluble; and finally, when the jelly is rendered anhydrous, it ves gummy-looking white masses, which appear to be absolutely insoble, like the light dusty silicic acid obtained by drying a jelly charged with salts, in the ordinary analysis of a silicate. The liquidity of silicic acid is only affected by a change, which is permanent (namely, coagulation or pectization), by which the acid is converted into the gelatinous or pectous form, and loses its miscibility with water. The liquidity is permanent in proportion to the degree of dilution of silicic the contrary, by concentration, and by elevation of temperature. A liquid silicic acid of 10 or 12 per cent. pectizes spontaneously in a few hours at the ordinary temperature, and immediately when heated. A liquid of 5 per cent. may be preserved for five or six days; a liquid of 2 per sent. for two or three months; and a liquid of 1 per cent. or less are no doubt practically unalterable by time, and hence the possibility of soluble silicici acid existing in nature. I may add, however, that no solution, weak or strong, of silicic acid in water has shown any disposition to deposit crystals , but always appears on drying as a colloidal glassy hyalite. The formation of quartz crystals at a low temperature, of so frequent occurrence in nature, remains still a mystery. I can imagine that such crystals are formed at an inconceivably slow rate, and from solutions of silicic acid which are extremely dilute. Dilution no doubt weakens the colloidal character of substances, and may therefore allow their crystallizing tendency to gain ground and develope itself, particularly where the crystal once formed is completely insoluble, as with quartz.


1983 ◽  
Vol 3 (5) ◽  
pp. 165-168 ◽  
Author(s):  
P. Annamalai ◽  
R. Cole

2016 ◽  
Vol 6 (1) ◽  
Author(s):  
Taewoo Kim ◽  
Jeong Seok Lee ◽  
Geonhui Lee ◽  
Dong Kyun Seo ◽  
Youngbin Baek ◽  
...  
Keyword(s):  

2014 ◽  
Vol 4 (2) ◽  
pp. 1-22
Author(s):  
Srinivas Reddy ◽  
Havovi Joshi

Subject area – Marketing, innovation, strategy. Study level/applicability – Undergraduate, post-graduate and executive education. Case overview – This case is set in January 2012, a few days before the launch of Mysore Sandal Millennium, a super-premium luxury soap offering from the Indian public sector enterprise, Karnataka Soaps and Detergents Ltd. (“KS&DL”). Three years of research had been put into this product, which contained some of the finest, high-quality ingredients. KS&DL had, over the past decade or so, observed a significant fall in brand image for its signature product, the Mysore Sandalwood soap. While this soap had for many years been considered the premium brand in India, it had lost its place when well-known foreign brands became available in India, and local manufacturers moved towards this segment, manufacturing a whole new range of competitive products such as liquid body washes and gels. It was with an aim to rebuild its image that the company decided to launch the Millennium soap. KS&DL was clear that the product would be initially aimed at the high-income Indians, and then move to expand into the overseas market. However, it remained to be seen if the company could be truly successful in marketing a product priced at a level which would make it unaffordable to most Indians, other than a very thin layer of the ultra-rich. The question remains as to how KS&DL could best go about executing and communicating its strategy to make this launch a success. Expected learning outcomes – This case provides students the opportunity to learn about the challenges faced when a company launches a new brand, particularly a luxury brand in a developing country such as India. Through this case, students will learn about the concepts of brand extension, and, above all, vertical brand extension. It can also be used to discuss the spill-over effects of the launch (and its success) on other existing brands of the company, as well as the overall corporate brand. Supplementary materials – Teaching notes are available for educators only. Please contact your library to gain login details or email: [email protected] to request teaching notes.


2013 ◽  
Vol 2013 (0) ◽  
pp. _G0306-01_-_G0306-04_
Author(s):  
Masumi ITO ◽  
Masaya SHIGETA ◽  
Seiichiro IZAWA ◽  
Yu FUKUNISHI

In the course of his experimental investigation of a general and important law of electro-chemical action, which required the accurate measurement of the gases evolved during the decomposition of water and other substances, the author was led to the detection of a curious effect, which had never been previously noticed, and of which the knowledge, had he before possessed it, would have prevented many of the errors and inconsistencies occurring in the conclusions he at first deduced from his earlier experiments. The phenomenon observed was the gradual recombination of elements which had been previously separated from each other by voltaic action. This happened when, after water had been decomposed by voltaic electricity, the mixed gases resulting from such decomposition were left in contact with the platina wires or plates, which had acted as poles; for under these circumstances they gradually diminished in volume, water was reproduced, and at last the whole of the gases disappeared. On inquiring into the cause of this reunion of the elements of water, the author found that it was occasioned principally by the action of the piece of platina, which had served for the positive pole; and also that the same piece of platina would produce a similar effect on a mixture of oxygen and hydrogen gases obtained by other and more ordinary kinds of chemical action. By closer examination, it was ascertained that the platina, which had been the negative pole, could produce the same effect. Finally, it was found that the only condition requisite for rendering the pieces of platina effective in this recombination of oxygen and hydrogen is their being perfectly clean, and that ordinary mechanical processes of cleaning are quite sufficient for bringing them into that condition, without the use of the battery. Plates of platina, cleaned by means of a cork, with a little emery and water, or dilute sulphuric acid, were rendered very active; but they acquired the greatest power when first heated in a strong solution of caustic alkali, then dipped in water to wash off the alkali, next dipped in hot strong oil of vitriol, and finally left for ten or fifteen minutes in distilled water. Plates thus prepared, placed in tubes containing mixtures of oxygen and hydrogen gases, determined the gradual combination of their elements: the effect was at first slow, but became by degrees more rapid; and heat was evolved to such a degree, indeed, as frequently to give rise to ignition and explosion. The author regards this phenomenon as of the same kind as that discovered by Davy in the glowing platinap; that observed by Döbereiner in spongy platina, acting on a jet of hydrogen gas in atmospheric air; and those so well experimented on by MM. Dulong and Thenard. In discussing the theory of these remarkable effects, the author advances some new views of the conditions of elasticity at the exterior of a mass of gaseous matter confined by solid surfaces. The elasticity of gases he considers as being dependent on the mutual action of the particles, especially of those which are contiguous to each other; but this reciprocity of condition is wanting on the sides of the exterior particles which are next to the solid substance. Then, reasoning on the principle established by Dalton, that the particles of different gases are indifferent to one another, so that those of one gas may come within almost any distance of those of another gas, whatever may be the respective degrees of tension in each gas among the particles of its own kind, he concludes that the particles of a gas, or of a mixture of gases, which are next to the platina, or other solid body not of their own chemical nature, touch that surface by a contact as close as that by which the particles of a solid or liquid body touch each other. This proximity, together with the absence of any mutual relation of the gaseous particles to particles of their own kind, combined also with the direct attractive force exerted by the platina, or other solid body, on the particles of the gases, is sufficient, in the opinion of the author, to supply what is wanting in order to render effective the affinity between the particles of oxygen and hydrogen; being, in fact, equivalent to an increase of temperature, to solution, or to any of the other circumstances which are known to be capable of adding to the force of the affinities inherent in the substances themselves.


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