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Freezing latent heat

Keywords Cocoa butter Crystallization Freezing Latent heat Nucleation Nusselt number Ranz-Marshall correlation Recalescence Schmidt number Sherwood number Solidification Supercooling... [Pg.327]

Conduction with Change of Phase A special type of transient problem (the Stefan problem) involves conduction of heat in a material when freezing or melting occurs. The liquid-solid interface moves with time, and in addition to conduction, latent heat is either generated or absorbed at the interface. Various problems of this type are discussed by Bankoff [in Drew et al. (eds.). Advances in Chemical Engineering, vol. 5, Academic, New York, 1964]. [Pg.557]

The cloudiness of ordinary ice cubes is caused by thousands of tiny air bubbles. Air dissolves in water, and tap water at 10°C can - and usually does - contain 0.0030 wt% of air. In order to follow what this air does when we make an ice cube, we need to look at the phase diagram for the HjO-air system (Fig. 4.9). As we cool our liquid solution of water -i- air the first change takes place at about -0.002°C when the composition line hits the liquidus line. At this temperature ice crystals will begin to form and, as the temperature is lowered still further, they will grow. By the time we reach the eutectic three-phase horizontal at -0.0024°C we will have 20 wt% ice (called primary ice) in our two-phase mixture, leaving 80 wt% liquid (Fig. 4.9). This liquid will contain the maximum possible amount of dissolved air (0.0038 wt%). As latent heat of freezing is removed at -0.0024°C the three-phase eutectic reaction of... [Pg.42]

This is of exactly the same form as eqn. (5.10) and AH is simply the "latent heat of melting" that generations of schoolchildren have measured in school physics labs." We now take some water at a temperature T < T, . We know that this will have a definite tendency to freeze, so Wf is positive. To calculate Wf we have Wf=- A A, and H = U + pV to give us... [Pg.52]

Physical and Chemical Properties - Physical State at 15 X and 1 atm. Liquid Molecular Weight S5.W -, Boiling Point at 1 atm. Decomposes-, Freezing PoirU -5.8, -21,252 Critical Temperature Not pertinent Critical Pressure Not pertinent Specific Gravity 0.925 at 25 °C (liquid) Vapor (Gas) Density Not pertinent Ratio of Specific Heats of Vapor (Gas) 1.074 Latent Heat of Vaporization No... [Pg.3]


See other pages where Freezing latent heat is mentioned: [Pg.478]    [Pg.478]    [Pg.434]    [Pg.183]    [Pg.502]    [Pg.427]    [Pg.247]    [Pg.247]    [Pg.91]    [Pg.1]    [Pg.3]    [Pg.6]    [Pg.9]    [Pg.10]    [Pg.11]    [Pg.11]    [Pg.15]    [Pg.16]    [Pg.23]    [Pg.26]    [Pg.27]    [Pg.28]   


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Latent heat of freezing

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