Abstract:The theoretical treatment of self-sustained periodic motion of the explosive crystallization ͑EC͒ front in a thin amorphous film is presented. The main attention is given to the study of nonlinear resonance phenomena occurring due to the presence of a small external periodic perturbation with the frequency being in the vicinity of the ordinary or parametric resonance. Weakly anharmonic oscillations of the EC front velocity are considered with the Van der Pole method, and the expressions for the limit cycle amp… Show more
“…This is in contrast to any formulation in terms of a local heat transfer coefficient, which is often found in the literature, e.g. in Geiler et al (1986); Grigoropoulos et al (2006); ; Kurtze (1986); Shklovskij & Ostroushko (1996). It is also at odds with a more general polynomial relationship between heat loss and temperature, as reported in Ma et al (1990).…”
Section: Inversion Of the Interface Coupling Conditionmentioning
confidence: 77%
“…This influence is examined e.g. in Geiler et al (1986); Grigoropoulos et al (2006); ; Kurtze (1986); Rogers et al (2006); Shklovskij & Ostroushko (1996). The heat loss can even lead to the explosive crystallization process dying out (Heinig & Geiler, 1986;Provatas et al, 1996).…”
Section: Heat Loss Influencementioning
confidence: 99%
“…Specifically, the influence of heat loss into the substrate on the explosive crystallization process is examined in detail. Often, inclusion of heat loss is realized semi-empirically using an apparent heat transfer coefficient (Geiler et al, 1986;Grigoropoulos et al, 2006;Kurtze, 1986;Shklovskij & Ostroushko, 1996). In contrast, the present work derives the equations governing heat conduction into the substrate from first principles, avoiding the use of an empirical heat transfer coefficient.…”
Section: Motivation Of Present Workmentioning
confidence: 99%
“…It is often assumed in the literature -e.g. in Grigoropoulos et al (2006); ; Kurtze (1986); Shklovskij & Ostroushko (1996) -that the heat loss into the substrate can be described by a local heat transfer coefficient (see also section 5.2.2). If that were the case, a constant temperature would require a constant rate of crystallization, i.e.…”
Section: Non-local Influence On Heat Lossmentioning
The self-sustaining process of transformation from an amorphous state to the crystalline state is considered. The crystallizing layer, which is mounted on a substrate, is assumed to be very thin. Thus the energy balance for the layer reduces to the equation of one-dimensional heat diffusion with a source term due to the local liberation of latent heat and a heat loss term due to thermal contact with the substrate. The crystallization rate is determined by a rate equation based on the crystallization theory due to A.N. Kolmogorov and M. Avrami. Heat conduction in the substrate is described by introducing a continuous distribution of moving heat sources at the interface. The problem is solved numerically with a collocation method. The propagation speed of the crystallization wave is obtained as an eigenvalue. Dual solutions are found below a critical value of a non-dimensional heat-loss parameter, whereas no solution exists above that value.
“…This is in contrast to any formulation in terms of a local heat transfer coefficient, which is often found in the literature, e.g. in Geiler et al (1986); Grigoropoulos et al (2006); ; Kurtze (1986); Shklovskij & Ostroushko (1996). It is also at odds with a more general polynomial relationship between heat loss and temperature, as reported in Ma et al (1990).…”
Section: Inversion Of the Interface Coupling Conditionmentioning
confidence: 77%
“…This influence is examined e.g. in Geiler et al (1986); Grigoropoulos et al (2006); ; Kurtze (1986); Rogers et al (2006); Shklovskij & Ostroushko (1996). The heat loss can even lead to the explosive crystallization process dying out (Heinig & Geiler, 1986;Provatas et al, 1996).…”
Section: Heat Loss Influencementioning
confidence: 99%
“…Specifically, the influence of heat loss into the substrate on the explosive crystallization process is examined in detail. Often, inclusion of heat loss is realized semi-empirically using an apparent heat transfer coefficient (Geiler et al, 1986;Grigoropoulos et al, 2006;Kurtze, 1986;Shklovskij & Ostroushko, 1996). In contrast, the present work derives the equations governing heat conduction into the substrate from first principles, avoiding the use of an empirical heat transfer coefficient.…”
Section: Motivation Of Present Workmentioning
confidence: 99%
“…It is often assumed in the literature -e.g. in Grigoropoulos et al (2006); ; Kurtze (1986); Shklovskij & Ostroushko (1996) -that the heat loss into the substrate can be described by a local heat transfer coefficient (see also section 5.2.2). If that were the case, a constant temperature would require a constant rate of crystallization, i.e.…”
Section: Non-local Influence On Heat Lossmentioning
The self-sustaining process of transformation from an amorphous state to the crystalline state is considered. The crystallizing layer, which is mounted on a substrate, is assumed to be very thin. Thus the energy balance for the layer reduces to the equation of one-dimensional heat diffusion with a source term due to the local liberation of latent heat and a heat loss term due to thermal contact with the substrate. The crystallization rate is determined by a rate equation based on the crystallization theory due to A.N. Kolmogorov and M. Avrami. Heat conduction in the substrate is described by introducing a continuous distribution of moving heat sources at the interface. The problem is solved numerically with a collocation method. The propagation speed of the crystallization wave is obtained as an eigenvalue. Dual solutions are found below a critical value of a non-dimensional heat-loss parameter, whereas no solution exists above that value.
“…A thorough investigation of various instabilities, cf. [37][38][39][40][41][42], is certainly desirable. The present analysis as well as previous theoretical work, e.g.…”
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