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The effect of varying the melt time and temperature on the growth rate at a particular temperature was determined.
In this study, an Avrami Analysis was utilized to study the bulk crystallization kinetics as a function of crystallization temperature, melt time and melt temperature.
The melt time and the pulse repetition rate have significant influence on the growth of nanofibers.
Furthermore at 2 MHz, the pulse separation time is 0.5 μs, which is longer than the melt time, only resolidified particles are observed on the irradiated surface.
The estimated melt time based on one-dimensional heat conduction model for glass varies between 0.4 and 0.8 μs [9], which is longer than the pulse separation time of 0.125 μs used in the present experiment.
Specifically, the curves labelled (i) denote the model using the generalised Gibbs-Thomson relation, curves (ii) take c s = c l in Gibbs-Thomson but not the energy balance (see [23]) and curves (iii) are the standard model where T m = T m ∗ and c s = c l. Clearly, the standard model overestimates the melt time considerably.
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Using a lower starting temperature of the xenolith, results in a predictably longer xenolith melting time.
The difference of melting velocity and melting time between ice and snow is compared.
We show that the paraffin melting time is shortest for combination n = 2, r = 2.
Moreover, with increase in inlet temperatures of the air, decreasing degree of their melting times are different, decreasing degree of the melting time of PCM1 is the biggest and that of PCM3 is the smallest.
The melting time of three different initial locations of an internal 20% air void within the EPCM capsule are compared.
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