1981
DOI: 10.1016/0022-0248(81)90007-5
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Containerless undercooling and solidification in drop tubes

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Cited by 72 publications
(17 citation statements)
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“…Measuring the duration of radiant cooling from release to nucleation event, T n may be first calculated via a numerical integration of the cooling rate which takes into account linear evolutions of liquid density (29), heat capacity (72), and hemispherical emissivity. Considering only data at the melting temperature leads to overestimation of T , as made on Nb by Lacy et al (73) in their pioneer work in this field (i.e., 530 K instead of 450 K). Moreover, the initial temperature can be identified with T m only for indisputably gas-free specimens.…”
Section: Iv1 Undercooling Results On Refractory Transition Metalsmentioning
confidence: 87%
“…Measuring the duration of radiant cooling from release to nucleation event, T n may be first calculated via a numerical integration of the cooling rate which takes into account linear evolutions of liquid density (29), heat capacity (72), and hemispherical emissivity. Considering only data at the melting temperature leads to overestimation of T , as made on Nb by Lacy et al (73) in their pioneer work in this field (i.e., 530 K instead of 450 K). Moreover, the initial temperature can be identified with T m only for indisputably gas-free specimens.…”
Section: Iv1 Undercooling Results On Refractory Transition Metalsmentioning
confidence: 87%
“…A more detailed discussion, including justification for the various approximations, has been published previously [6]. The differential equations of motion for the drop arc dx/dt = U (1) dU/dt = gAp/pp -3CapU2/49pd (2) 0022-2461/92 $03..00 + . 12 9 1992 Chapman & Hall where g is the gravitational field strength, p is the density of the gas, Pp is the density of the drop, Ap = Op -P, Ca is the coefficient of drag, d is the drop diameter, U is the drop speed, x is the distance fallen, and t is time.…”
Section: Differential Equations For a Falling Dropmentioning
confidence: 99%
“…The usefulness of drop tubes for studies of containerless liquid-metal supercooling is well established [1][2][3][4]. The typical experiment involves a small (several millimetres in diameter) drop falling from a levitated position within an evacuated or helium-filled drop tube chamber.…”
Section: Introductionmentioning
confidence: 99%
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“…Experimental techniques that have been developed to study droplet supercooling include hot-stage droplet dispersion techniques developed by Turnbull and co-workers, [6,7,8] droplet emulsification methods explored by Turnbull [9] and developed by Perepezko and co-workers, [10,11,12] MacIsaac et al [13] levitation melting techniques, [14,15,16] and drop tower methods. [17,18] However, most of these techniques only apply to stationary droplets, with the exception of drop tower techniques, and as such only generate knowledge specific to the droplets generated by a specific technique. While such knowledge is of scientific importance, it cannot be immediately extended to predict the droplet supercooling and solidification in industrial processes, such as gas atomization, centrifugal atomization, spray forming, and thermal spraying, in which droplets in various sizes solidify while traveling in a gas.…”
Section: Introductionmentioning
confidence: 99%