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Droplet experiment

To estimate the available interaction time in a free-fall droplet experiment the steady-state balance between gravity and Stokes drag can be analyzed. A free-falling droplet will be subject to both gravitational and drag forces. Assuming that... [Pg.474]

Surface tension is the tendency of liquids to reduce their exposed surface to the smallest possible area. A single drop of water - such as a rain drop - tries to take on the shape of a sphere. We attribute this phenomenon to the attractive forces acting between the molecules of the liquid. The molecules within the liquid bulk are attracted equally from all directions, but those near the outer surface of the droplet experience unequal attractions, which cause them to draw in toward the centre of the droplet - a phenomenon experienced as a tension. [Pg.523]

To determine if a droplet experiences spreading or splashing when it impinges onto a liquid film on a solid surface, the correlation between the Weber number and Ohnesorge number derived by Walzel[398] may be used ... [Pg.237]

H5. Hendricks, C. D., Jr., Charged droplet experiments, paper presented at Symp. Advan. Propulsion Concepts, 2nd, ARDC and AVCO-Everett Res. Labs., Boston, Mass. (1959). [Pg.93]

Based on data of the type displayed in Fig. 40, Davis and his coworkers determined the Sherwood numbers for a number of droplet experiments, and their results are displayed in Fig. 41, a graph of the Sherwood number as a function of the Peclet number. [Pg.73]

Assuming that the internal droplets experience a hard-sphere-like repulsion when surfactant layers come in contact, an estimation of the van der Waals interactions can be obtained from the average length of the surfactant tails (1 3 nm) [20]. The coalescence frequency is therefore the unique free pa-... [Pg.185]

If the water were to be injected into a cold engine cylinder, the flash steam would immediately condense and there would be no pressure rise. To overcome this problem, the cylinder head and walls are heated and supply additional heat to the wet steam entering the cylinder. The atomised water droplets experience extremely high collision rates with the cylinder walls because of the explosive effect of the flash process. The tiny size of the droplets, coupled with high collision rates ensure rapid absorption of heat allowing them to be quickly converted to steam which is then heated further to superheat. [Pg.40]

In the following sections a description of the HED used in these studies, a list of their measured properties, and preliminary results of droplet experiments for solutions of solid HED formulations in JP-10 and liquid HED compounds are given. These data are needed to evaluate the combustion characteristics of these new fuels as individual compounds or as additives to existing fuel systems and to provide a basis for the development of the predictive capability of solid-gas interface tracking in a turbulent reacting flow. [Pg.75]

IR spectroscopy is an elegant technique suitable to sort out experimentally the distribution of tautomers in the isolated molecule. The several NH or OH oscillators are expected to be very close in frequency but nevertheless tautomer-dependent and can therefore be resolved providing that special efforts are done to avoid spectral congestion. To this purpose, matrix studies, gas phase experiments as well as He droplets experiments have been carried out. [Pg.347]

S. Sikalo, H.D. Wilhelm, I.V. Roisman, S. Jakirhc, and C. Tropea, Dynamic Contact Angle of Spreading Droplets Experiments and Simulations, Phys. Fluids, 17, 062103 (2005). [Pg.242]

In 1908 Robert Millikan (1923 Nobel Prize in Physics) first performed his famous oil droplet experiment in which he determined a unit charge of 4.77 x 10 ° esu (later 4.80 x 10 °) esu. With the modem e/m value (1.7 x 10 esu/g), the mass of the electron was found to be only Yim that of the lightest atom, hydrogen. [Pg.525]

Fig. 10.16 Left optical microscopy imageof the electrode array with overlay of the spreading of 1,5, and 10 pL droplets added after grinding of the array. Right humidity and temperature control during droplet experiments using saturated salt solutions of KCl and MgCl2 [64]. Fig. 10.16 Left optical microscopy imageof the electrode array with overlay of the spreading of 1,5, and 10 pL droplets added after grinding of the array. Right humidity and temperature control during droplet experiments using saturated salt solutions of KCl and MgCl2 [64].
Emulsions are thermodynamically unstable systems and will, as a function of time, separate to minimize the interfacial area between the oil phase and the water phase. If a density difference exists between the dispersed and continuous phases, dispersed droplets experience a vertical force in a gravitational field. The gravitational force is opposed by the fractional drag force and the buoyancy force. The resulting creaming rate vq of a single droplet is given by Stokes law ... [Pg.361]

Williams plotted the film-thinning time for deformable and nondeformable droplets against droplet radius. While an increase in droplet size increases the time required for thinning of a deformable droplet, nondeformable droplets experience a reduction in film thinning time as their size increases. It is interesting also to note the square relationship on thinning rate wifii nondeformable droplets and an inverse square relationship for deformable droplets. Clearly, increasing the apphed field across a system with deformable droplets could result in a reduction in coalescence efficiency. [Pg.687]

S.R. Snarski, P.F. Duim Experiments characterizing the interaction between two sprays of electrically charged liquid droplets. Experiments in Fluids, 11, 268-278 (1991). [Pg.474]

Figure 3.45 shows a schematic demonstrating the idealized stages involved in the formation of a dense particle from a droplet of solution [224, 225]. The droplet experiences evaporation, when the solute concentration in the outer layer increases to a value of above the supersaturation limit, thus resulting in the precipitation of fine particles. Precipitation is followed by a drying stage, in which the vapor phase diffuses through the pores in the precipitated layer. Decomposition of the... [Pg.150]

The dried-droplet experiment clearly demonstrates that this sample preparation makes peptides migrate out of the tissue, rendering the procedure unsuitable for peptide localizations. However, a set of lipid ions remain in the tissue (as shown for the typical 610.444 MH+ ion), nicely demarcating the tissue on the MS target plate/slide. [Pg.447]

Starting from an earlier work by Frederick and Hupa (1993) a new simplified black liquor droplet model is developed to replace the standard droplet model in CFD simulations of black liquor recovery furnaces. Liquor specific input data obtained from single droplet experiments is incorporated into the new droplet model. The model is implemented in a commercial CFD code and simulations in an environment that represents well the experimental setup of the single droplet furnace are performed (Figure 3). This way, model expressions for droplet swelling during devolatilisation and carbon release curves during devolatilisation and char carbon conversion can be validated. After this validation procedure the model can be used for full scale recovery furnace simulations. [Pg.814]

Fig. 16. a A molecular dynamics simulation was used to create a schematic image of polymer nano- and macro-scale particles generated from the submicron liquid droplets experiment The solvent molecules (typically H2O and THF in the experiment,not considered in the simulation) are streaming away as the polymer molecules are left behind collapsing into a nano or micrometer particle. Within the experimental time scale, the solvent evaporation was completed before the particles collected on a substrate, b Bright field image (inverted grayscale) of 2 pm diameter of PE particles... [Pg.50]


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See also in sourсe #XX -- [ Pg.286 ]




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