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Supercooled drop

Droplets in clouds, fog and mist are in continuous motion because of the dynamic processes but also due to the advective motion of air. In this way they can impact with surfaces such as trees, towers and buildings and due to the adhesive properties of water, the droplet sticks. When the temperature is higher than 0 °C, the impacted drops can grow by collision and finally flow down this process is called cloud-droplet interception. At temperatures below 0 °C the supercooled drop-... [Pg.165]

The greater the undercooling, the more rapidly the polymer crystallizes. This is due to the increased probability of nucleation the more supercooled the liquid becomes. Although the data in Fig. 4.8 are not extensive enough to show it, this trend does not continue without limit. As the crystallization temperature is lowered still further, the rate passes through a maximum and then drops off as Tg is approached. This eventual decrease in rate is due to decreasing chain mobility which offsets the nucleation effect. [Pg.230]

Johnstone, Feild, and Tassler (7D) have developed a Venturi atomizer to produce dense fogs of liquid drops. This equipment is similar to that used by Comings, Adams, and Shippee (IB). Durbin (6D) has studied the formation of condensation particles in supercooled hypersonic air flow. [Pg.142]

Ontxlal is a liny ice particle, about 10 to 20 microns in diameter, formed by direct freezing of supercooled water droplets at temperatures below - Kf C. The term is coined by combining the words "drop" and "crystal. ... [Pg.819]

Equilibrium vapor pressure is the vapor pressure of a system in which two or more phases or a substance coexist in equilibrium. In meteorology, the reference is to water substance, unless otherwise specified, If the system consists of moist air in equilibrium with a plane surface of pure water or ice, the more specialized term saturation vapor pressure is usually employed, in which case, the vapor pressure is a function of temperature only. In the atmosphere, the system is complicated by the presence of impurities in liquid or solid water substance (see also Raoult s Law), drops or ice crystals or both, existing as aerosols and, in general, the problem becomes one of nucleation. For example, the difference in vapor pressure over supercooled water... [Pg.1670]

The temperature at first will gradually fall, then will become constant as crystallization starts and continues under equilibrium conditions, and finally will start to drop again. Some chemicals may supercool slightly below (0.5°) the solidification point as crystallization begins, the temperature will rise and remain constant as equilibrium conditions are established. Other products may cool more than 0.5° and cause deviation from the normal pattern of temperature change. If the temperature rise exceeds 0.5° after the initial crystallization begins, repeat the test, and seed the melted compound with small crystals of the sample at 0.5° intervals as the temperature approaches the expected solidification point. Crystals for seed-... [Pg.847]

Observe and record the temperature readings at regular intervals until the temperature rises from a minimum, due to supercooling, to a maximum and then finally drops. The maximum temperature reading is the solidification point. Readings 10 s apart should be taken to establish that the temperature is at the maximum level and should continue until the drop in temperature is established. [Pg.848]

Localised Ordering - Dropping Supercooled Ice into Water... [Pg.21]

When a liquid supercools (i.e., does not crystallize when its temperature drops below the thermodynamic melting point), the liquidlike structure is frozen due to the high viscosity of the system. The supercooled liquid is in a so-called viscoelastic state. If the crystallization can be further avoided as the ten ierature continues to drop, a glass transition will happen at a certain temperature, where the frozen liquid turns into a brittle, rigid state known as a glassy state. A well-accepted definition for glass transition is that the relaxation time t of the system is 2 X10 s or the viscosity / isio Pas (an arbitrary standard, of course). [Pg.766]


See other pages where Supercooled drop is mentioned: [Pg.2129]    [Pg.2132]    [Pg.2133]    [Pg.164]    [Pg.85]    [Pg.91]    [Pg.125]    [Pg.2129]    [Pg.2132]    [Pg.2133]    [Pg.164]    [Pg.85]    [Pg.91]    [Pg.125]    [Pg.337]    [Pg.754]    [Pg.52]    [Pg.272]    [Pg.103]    [Pg.106]    [Pg.65]    [Pg.27]    [Pg.320]    [Pg.151]    [Pg.10]    [Pg.56]    [Pg.9]    [Pg.14]    [Pg.180]    [Pg.181]    [Pg.162]    [Pg.236]    [Pg.266]    [Pg.289]    [Pg.268]    [Pg.246]    [Pg.246]    [Pg.126]    [Pg.181]    [Pg.242]    [Pg.736]    [Pg.147]    [Pg.79]    [Pg.91]    [Pg.123]    [Pg.295]   
See also in sourсe #XX -- [ Pg.164 , Pg.415 ]




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