FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W110002918> ?p ?o ?g. }

• W110002918 abstract "Abstract A procedure has been developed to obtain an evolution equation with the temperature for the actual transformed volume fraction under non-isothermal regime, to calculate the kinetic parameters and to analyze the glass-crystal transformation mechanisms in solid systems where a large number of nuclei already exists and no other new nuclei are formed during the thermal treatment. In this case, it is assumed that the nuclei only grow, “site saturation”, during the thermal process. Once an extended volume of transformed material has been defined and spatially random transformed regions have been assumed, a general expression of the extended volume fraction has been obtained as a function of the temperature. Considering the mutual interference of regions which grow from separate nuclei (impingement effect) and from the quoted expression, the actual transformed volume fraction has been deduced. The kinetic parameters have been obtained, by assuming that the reaction rate constant is a time function through its Arrhenian temperature dependence. The developed theoretical method has been applied to the crystallization kinetics of the Ag 0.16 As 0.46 Se 0.38 glassy alloy as-quenched and previously reheated. In accordance with the corresponding results, it is possible to establish that in the considered alloy the nuclei were dominant before the thermal treatment, and because of it the reheating does not change in a considerable way the number of the pre-existing nuclei in the material, which is a case of “site saturation”. The comparison of the quoted results with the values obtained by means of Matusita method confirms the reliability of the theoretical method developed (TMD). Moreover, the obtained values for the kinetic parameters coincide in a satisfactory way with the results calculated by means of the Austin–Rickett (AR) equation under non-isothermal regime. Besides, the experimental curve of the transformed fraction shows a better agreement with the theoretical curves of the developed method and of the Austin–Rickett model than with the corresponding curve of the Avrami model. Accordingly, it seems appropriate to choose the Austin–Rickett equation in order to describe the crystallization mechanism of the above-mentioned glassy alloy." @default.
• W110002918 created "2016-06-24" @default.
• W110002918 creator A5010030779 @default.
• W110002918 creator A5027616277 @default.
• W110002918 creator A5035547416 @default.
• W110002918 creator A5079097778 @default.
• W110002918 creator A5085262781 @default.
• W110002918 creator A5091701652 @default.
• W110002918 date "2009-02-01" @default.
• W110002918 modified "2023-09-26" @default.
• W110002918 title "On the glass-crystal transformation kinetics by using differential scanning calorimetry under non-isothermal regime" @default.
• W110002918 cites W140499693 @default.
• W110002918 cites W1627906083 @default.
• W110002918 cites W1647781763 @default.
• W110002918 cites W1870104632 @default.
• W110002918 cites W1964457736 @default.
• W110002918 cites W1964740351 @default.
• W110002918 cites W1972902650 @default.
• W110002918 cites W1973931811 @default.
• W110002918 cites W1990913602 @default.
• W110002918 cites W1993743776 @default.
• W110002918 cites W1995938322 @default.
• W110002918 cites W2014199690 @default.
• W110002918 cites W2024908520 @default.
• W110002918 cites W2025414772 @default.
• W110002918 cites W2031367501 @default.
• W110002918 cites W2033437232 @default.
• W110002918 cites W2034490983 @default.
• W110002918 cites W2056320034 @default.
• W110002918 cites W2059359339 @default.
• W110002918 cites W2066055743 @default.
• W110002918 cites W2068060490 @default.
• W110002918 cites W2074707536 @default.
• W110002918 cites W2075029788 @default.
• W110002918 cites W2082051881 @default.
• W110002918 cites W2088062112 @default.
• W110002918 cites W2089735397 @default.
• W110002918 cites W2090732497 @default.
• W110002918 cites W2091745890 @default.
• W110002918 cites W2126815279 @default.
• W110002918 cites W2225923242 @default.
• W110002918 doi "https://doi.org/10.1016/j.tca.2008.11.014" @default.
• W110002918 hasPublicationYear "2009" @default.
• W110002918 type Work @default.
• W110002918 sameAs 110002918 @default.
• W110002918 citedByCount "11" @default.
• W110002918 countsByYear W1100029182012 @default.
• W110002918 countsByYear W1100029182015 @default.
• W110002918 countsByYear W1100029182016 @default.
• W110002918 countsByYear W1100029182021 @default.
• W110002918 crossrefType "journal-article" @default.
• W110002918 hasAuthorship W110002918A5010030779 @default.
• W110002918 hasAuthorship W110002918A5027616277 @default.
• W110002918 hasAuthorship W110002918A5035547416 @default.
• W110002918 hasAuthorship W110002918A5079097778 @default.
• W110002918 hasAuthorship W110002918A5085262781 @default.
• W110002918 hasAuthorship W110002918A5091701652 @default.
• W110002918 hasConcept C114614502 @default.
• W110002918 hasConcept C121332964 @default.
• W110002918 hasConcept C123266363 @default.
• W110002918 hasConcept C133347239 @default.
• W110002918 hasConcept C135889238 @default.
• W110002918 hasConcept C148898269 @default.
• W110002918 hasConcept C161680532 @default.
• W110002918 hasConcept C191897082 @default.
• W110002918 hasConcept C192562407 @default.
• W110002918 hasConcept C199360897 @default.
• W110002918 hasConcept C203036418 @default.
• W110002918 hasConcept C2780026712 @default.
• W110002918 hasConcept C2781285689 @default.
• W110002918 hasConcept C33923547 @default.
• W110002918 hasConcept C39519442 @default.
• W110002918 hasConcept C41008148 @default.
• W110002918 hasConcept C44125496 @default.
• W110002918 hasConcept C65590680 @default.
• W110002918 hasConcept C74650414 @default.
• W110002918 hasConcept C87976508 @default.
• W110002918 hasConcept C96288455 @default.
• W110002918 hasConcept C97355855 @default.
• W110002918 hasConcept C9930424 @default.
• W110002918 hasConceptScore W110002918C114614502 @default.
• W110002918 hasConceptScore W110002918C121332964 @default.
• W110002918 hasConceptScore W110002918C123266363 @default.
• W110002918 hasConceptScore W110002918C133347239 @default.
• W110002918 hasConceptScore W110002918C135889238 @default.
• W110002918 hasConceptScore W110002918C148898269 @default.
• W110002918 hasConceptScore W110002918C161680532 @default.
• W110002918 hasConceptScore W110002918C191897082 @default.
• W110002918 hasConceptScore W110002918C192562407 @default.
• W110002918 hasConceptScore W110002918C199360897 @default.
• W110002918 hasConceptScore W110002918C203036418 @default.
• W110002918 hasConceptScore W110002918C2780026712 @default.
• W110002918 hasConceptScore W110002918C2781285689 @default.
• W110002918 hasConceptScore W110002918C33923547 @default.
• W110002918 hasConceptScore W110002918C39519442 @default.
• W110002918 hasConceptScore W110002918C41008148 @default.
• W110002918 hasConceptScore W110002918C44125496 @default.
• W110002918 hasConceptScore W110002918C65590680 @default.
• W110002918 hasConceptScore W110002918C74650414 @default.
• W110002918 hasConceptScore W110002918C87976508 @default.

• next