<abstract xmlns="http://www.w3.org/1999/xhtml"><p>Mechanoluminescence (ML) from deformed ductile materials is caused by sliding of charged dislocations. The main source of the ML in loaded brittle solids is the interatomic bond breakage. In this work, the ML from impact damaged ductile ZnS ceramics was studied. It was revealed that the time series of ML pulses exhibited two well-separated peaks. A two-stage ML excitation of this kind in ZnS ceramics was observed when the applied load exceeded an ultimate plastic deformation. The positions of each peak along the time axis were found to be dependent in different ways on physical and mechanical properties of crystallites that constituted the given ceramics. The investigated ceramics were produced by four different technological methods. The obtained samples differing in the dimensions of grains and separation of grain boundaries were tested. The statistical analysis of a temporal pattern of the ML lighting showed that the mechanisms of excitation of the two peaks were not the same. The first ML peak was assigned to the plastic deformation preceding the ceramics cracking. The second peak originated from the interatomic bond breakage in nucleated and growing cracks.</p></abstract>

Mechanoluminescence (ML) from deformed ductile materials is caused by sliding of charged dislocations. The main source of the ML in loaded brittle solids is the interatomic bond breakage. In this work, the ML from impact damaged ductile ZnS ceramics was studied. It was revealed that the time series of ML pulses exhibited two well-separated peaks. A two-stage ML excitation of this kind in ZnS ceramics was observed when the applied load exceeded an ultimate plastic deformation. The positions of each peak along the time axis were found to be dependent in different ways on physical and mechanical properties of crystallites that constituted the given ceramics. The investigated ceramics were produced by four different technological methods. The obtained samples differing in the dimensions of grains and separation of grain boundaries were tested. The statistical analysis of a temporal pattern of the ML lighting showed that the mechanisms of excitation of the two peaks were not the same. The first ML peak was assigned to the plastic deformation preceding the ceramics cracking. The second peak originated from the interatomic bond breakage in nucleated and growing cracks.

Temporal pattern of the mechanoluminescent lighting from impact-loaded ZnS ceramics

Materials Science-Poland

This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 International License.

Mechanoluminescence (ML) from deformed ductile materials is caused by sliding of charged dislocations. The main source of the ML in loaded brittle solids is...

Temporal pattern of the mechanoluminescent lighting from impact-loaded ZnS ceramics

Data publikacji: 06 paź 2020

Zakres stron: 279 - 282

Otrzymano: 27 wrz 2017

Przyjęty: 23 kwi 2019

DOI: https://doi.org/10.2478/msp-2020-0039

Słowa kluczowe
ZnS ceramics, impact damage, mechanoluminescence, time series

© 2020 Alexandre Chmel et al., published by Sciendo

This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 International License.

Temporal pattern of the mechanoluminescent lighting from impact-loaded ZnS ceramics

Data publikacji: 06 paź 2020

Zakres stron: 279 - 282

Otrzymano: 27 wrz 2017

Przyjęty: 23 kwi 2019

DOI: https://doi.org/10.2478/msp-2020-0039

Słowa kluczoweZnS ceramics, impact damage, mechanoluminescence, time series

© 2020 Alexandre Chmel et al., published by Sciendo

This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 International License.

Słowa kluczowe
ZnS ceramics, impact damage, mechanoluminescence, time series