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| Naji, M. |
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| Motta, Antonella |
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| Aletan, Dirar |
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| Mohamed, Tarek |
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| Ertürk, Emre |
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| Taccardi, Nicola |
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| Kononenko, Denys |
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| Petrov, R. H. | Madrid |
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| Alshaaer, Mazen | Brussels |
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| Bih, L. |
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| Casati, R. |
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| Muller, Hermance |
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| Kočí, Jan | Prague |
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| Šuljagić, Marija |
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| Kalteremidou, Kalliopi-Artemi | Brussels |
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| Azam, Siraj |
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| Ospanova, Alyiya |
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| Blanpain, Bart |
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| Ali, M. A. |
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| Popa, V. |
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| Rančić, M. |
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| Ollier, Nadège |
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| Azevedo, Nuno Monteiro |
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| Landes, Michael |
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| Rignanese, Gian-Marco |
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Bockowski, Michal
Institute of High Pressure Physics
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (22/22 displayed)
- 2024Explaining an anomalous pressure dependence of shear modulus in germanate glasses based on Reverse Monte Carlo modelling
- 2024Explaining an anomalous pressure dependence of shear modulus in germanate glasses based on Reverse Monte Carlo modelling
- 2024History matters for glass structure and mechanical properties
- 2023Evolution of the Growth Mode and Its Consequences during Bulk Crystallization of GaNcitations
- 2022Novel High-Pressure Nanocomposites for Cathode Materials in Sodium Batteriescitations
- 2022Thermal conduction in a densified oxide glasscitations
- 2022Thermal conduction in a densified oxide glass:Insights from lattice dynamicscitations
- 2021Vibrational disorder and densification-induced homogenization of local elasticity in silicate glassescitations
- 2021Thermal conductivity of densified borosilicate glassescitations
- 2021Indentation Response of Calcium Aluminoborosilicate Glasses Subjected to Humid Aging and Hot Compressioncitations
- 2021Volume relaxation in a borosilicate glass hot compressed by three different methodscitations
- 2020Composition and pressure effects on the structure, elastic properties and hardness of aluminoborosilicate glasscitations
- 2020Achieving ultrahigh crack resistance in glass through humid agingcitations
- 2020Volume relaxation in a borosilicate glass hot compressed by three different methodscitations
- 2019Luminescence behaviour of Eu 3+ in hot-compressed silicate glassescitations
- 2019Revisiting the Dependence of Poisson’s Ratio on Liquid Fragility and Atomic Packing Density in Oxide Glassescitations
- 2019(Invited) Advances in Ion Implantation of GaN and AlN
- 2018Deformation and cracking behavior of La2O3-doped oxide glasses with high Poisson's ratiocitations
- 2017Thermal Conductivity of Foam Glasses Prepared using High Pressure Sintering
- 2017Foaming Glass Using High Pressure Sintering
- 2016Structure and mechanical properties of compressed sodium aluminosilicate glassescitations
- 2014Pressure-Induced Changes in Inter-Diffusivity and Compressive Stress in Chemically Strengthened Glass
Places of action
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conferencepaper
Foaming Glass Using High Pressure Sintering
Abstract
Foam glass is a high added value product which contributes to waste recycling and energy efficiency through heat insulation. The foaming can be initiated by a chemical or physical process. Chemical foaming with aid of a foaming agent is the dominant industrial process. Physical foaming has two variations. One way is by saturation of glass melts with gas. The other involves sintering of powdered glass under a high gas pressure resulting in glass pellets with high pressure bubbles entrapped. Reheating the glass pellets above the glass transition temperature under ambient pressure allows the bubbles to expand. After heat-treatment foam glass can be obtained with porosities of 80–90 %. In this study we conduct physical foaming of cathode ray tube (CRT) panel glass by sintering under high pressure (5-25 MPa) using helium, nitrogen, or argon at 640 °C (~108 Pa s). Reheating a sample in a heating microscope above maximum foaming temperature gives a suitable foaming temperature for the remaining samples. We show that the foaming kinetics depend on the type of gas and the pressure. A critical pressure of around 20 MPa is found to give the largest expansion for all gasses. Samples are obtained with 100 % closed porosity for argon and nitrogen samples (5-20 MPa) and for helium samples (5-15 MPa). The pore structure of the samples is analysed to understand the critical pressure.