glass formation followed by in situ tomography
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Glass formation followed by in-situ tomography E. Gouillart M.-H. - PowerPoint PPT Presentation

Glass formation followed by in-situ tomography E. Gouillart M.-H. Chopinet, J. Grynberg, M.J. Toplis Joint Unit CNRS/Saint-Gobain, Aubervilliers (France) Collaborations 1 Why study glass formation ? 2 In-situ tomography 3


  1. − Glass formation followed by in-situ tomography E. Gouillart M.-H. Chopinet, J. Grynberg, M.J. Toplis Joint Unit CNRS/Saint-Gobain, Aubervilliers (France)

  2. − Collaborations

  3. − 1 Why study glass formation ? 2 In-situ tomography 3 Reactions in the Na 2 CO 3 − SiO 2 system 4 Evolution of calcium carbonate

  4. − Outline 1 Why study glass formation ? 2 In-situ tomography 3 Reactions in the Na 2 CO 3 − SiO 2 system 4 Evolution of calcium carbonate

  5. − Coarse raw materials -> slow kinetics 1500°C 1000°C A lot of room for energy saving ?

  6. − Producing homogeneous glass is difficult Defects Unmolten grains, bubble, chemical gradients... How are they related to the grain sizes, the temperature path, etc. ?

  7. − Literature: TGA in-situ XRD in-situ NMR

  8. − Outline 1 Why study glass formation ? 2 In-situ tomography 3 Reactions in the Na 2 CO 3 − SiO 2 system 4 Evolution of calcium carbonate

  9. − Visualizing glass melting from the inside T = 760 ◦ C T = 799 ◦ C T = 820 ◦ C T = 835 ◦ C T = 850 ◦ C T = 860 ◦ C T = 877 ◦ C T = 920 ◦ C

  10. − Faster and faster imaging ! ⇒ huge amounts of (noisy) data to process... O ( 100 Gb ) for one experiment Courtesy Luc Salvo

  11. − Absorption and phase contrast Phase reconstruction (Paganin Absorption reconstruction algorithm, single distance)

  12. − Datasets and issues In-situ images : speed vs. quality tradeoff. Noisy images, poor contrast, artifacts... Huge datasets : O ( 1 ) Go / image × # images in timeseries. Complicated system : what information do we want ?

  13. − Quantitative image processing Denoising Segmentation of the phases Tracking objects, measuring contacts statistics...

  14. − Outline 1 Why study glass formation ? 2 In-situ tomography 3 Reactions in the Na 2 CO 3 − SiO 2 system 4 Evolution of calcium carbonate

  15. − The Na 2 O − SiO 2 system 1000 900 874 865: NC melts 830 800 790 Na O NS NS 2 SiO 2 ... 2 50 66 33 Starting from Na 2 CO 3 and not from Na 2 O : where/how does the system enter the phase diagram ? T < 865 ◦ C : solid-state reactions (Turner, Wilburn, ...) Na 2 CO 3 + SiO 2 → Na 2 SiO 3 + CO 2 Na 2 SiO 3 + SiO 2 → Na 2 Si 2 O 5 T ≥ 865 ◦ C : reactions between molten Na 2 CO 3 and SiO 2 .

  16. − Both transformations mechanisms of Na 2 CO 3 can be observed Reaction in solid and liquid state Volume fraction of sodium carbonate + crystalline silicates ternary batch, 5 K . min − 1 ramp 0.20 Na 2 CO 3 0.15 melts 0.10 c 0.05 NS − NS 2 0.00 RT 760 800 840 880 T ( ◦ C ) 1000 900 874 865: NC melts 830 800 790 [Gouillart et al., JACS 2012] Na O NS NS 2 SiO 2 ... 2 33 50 66

  17. − Both transformations mechanisms of Na 2 CO 3 can be observed Reaction in solid and liquid state Volume fraction of sodium carbonate + crystalline silicates ternary batch, 5 K . min − 1 ramp 0.20 Na 2 CO 3 0.15 melts 0.10 c 0.05 NS − NS 2 0.00 RT 760 800 840 880 T ( ◦ C ) 1000 900 874 865: NC melts [Gouillart et al., JACS 2012] 830 800 790 Na O NS NS 2 SiO 2 ... 2 33 50 66

  18. − Porous grains with a large specific area Novacarb sodium carbonate

  19. − Porous grains with a large specific area Novacarb sodium carbonate grain open porosity

  20. − A very reactive system in the solid-state Formation of crystalline silicates : Na 2 CO 3 + SiO 2 → Na 2 SiO 3 + CO 2 metasilicate NS Na 2 SiO 3 + SiO 2 → Na 2 Si 2 O 5 disilicate NS 2 Reaction without contact ? ? Solid-state reaction at interspecies contacts 36% Na 2 CO 3 , 74% SiO 2 , 36% Na 2 CO 3 , 74% SiO 2 , 760 ◦ C 730 ◦ C

  21. − Tracking individual grains to learn reaction paths Sodium carbonate, blue and yellow : two sand grains, white : sodium silicates ⇒ sodium carbonate is extremely reactive and mobile : "semi-local" process

  22. − Reaction in vapor phase Yes ! ! Reaction without contact ? ?

  23. − Reaction in vapor phase Yes ! ! Reaction without contact ? ? K ≪ 1 ( 10 − 7 ) Na 2 CO 3 → ” Na 2 O ” + CO 2

  24. − Reaction in vapor phase Yes ! ! Reaction without contact ? ? Na 2 CO 3 → Na 2 O + CO 2 Na 2 O reacts with silica surface Na 2 O + SiO 2 → Na 2 SiO 3

  25. − Reaction in vapor phase Yes ! ! Reaction without contact ? ? Na 2 CO 3 → Na 2 O + CO 2 decomposition depends on CO 2 partial pressure

  26. − 2 different reaction mechanims, depending on the atmosphere 10 -1 MM-N 2 MG-N 2 MP-N 2 PM-N 2 MM-CO 2 10 -2 v ( % NC . s − 1 ) 10 -3 10 -4 0.00090 0.00095 0.00100 1/T ( K − 1 ) Kinetics of Na 2 CO 3 transformation measured by TGA coll. N. Ferruaud, C. Cazako, S. Papin

  27. − 2 different reaction mechanims, depending on the atmosphere 10 -1 MM-N 2 MG-N 2 MP-N 2 PM-N 2 MM-CO 2 10 -2 v ( % NC . s − 1 ) 10 -3 10 -4 0.00090 0.00095 0.00100 1/T ( K − 1 ) low CO 2 partial pressure : vapor-phase reactions are favored Small samples in tomography → CO 2 is easily removed.

  28. − 2 different reaction mechanims, depending on the atmosphere 10 -1 MM-N 2 MG-N 2 MP-N 2 PM-N 2 MM-CO 2 10 -2 v ( % NC . s − 1 ) 10 -3 10 -4 0.00090 0.00095 0.00100 1/T ( K − 1 ) high CO 2 partial pressure : Na 2 CO 3 decomposes only when in contact with silica.

  29. − Solid-state reactions 800 ◦ C, 4 × speed-up (scans of 2s every 6s)

  30. − Raman + XRD → chemical / crystalline composition of the system 100 100 liq 60-66 liq 60-66 NC 75 75 liq 66-72 liq wt% wt% 66-72 50 50 NS liq 72-78 liq NS 2 72-78 NS 25 25 Si Si 0 30 60 120 30 60 120 t (min) t (min) 4-h plateau at 820 ◦ C direct melting at 900 ◦ C

  31. − Raman + XRD → chemical / crystalline composition of the system 100 100 liq 60-66 liq 60-66 NC 75 75 liq 66-72 liq wt% wt% 66-72 50 50 NS liq 72-78 liq NS 2 NS 72-78 25 25 Si Si 0 30 60 120 30 60 120 t (min) t (min) 4-h plateau at 820 ◦ C direct melting at 900 ◦ C Better homogeneity when solid-state reactions have been favored.

  32. − Raman + XRD → chemical / crystalline composition of the system 100 100 liq 60-66 liq 60-66 NC 75 75 liq 66-72 liq wt% wt% 66-72 50 50 NS liq 72-78 liq NS 2 NS 72-78 25 25 Si Si 0 30 60 120 30 60 120 t (min) t (min) 4-h plateau at 820 ◦ C direct melting at 900 ◦ C Better homogeneity when solid-state reactions have been favored. Can it be explained by the spatial distribution of sodium silicates ?

  33. − Reactions above the melting point of Na 2 CO 3 900 ◦ C, 4 × speed-up (scans of 1s every 6s)

  34. − Outline 1 Why study glass formation ? 2 In-situ tomography 3 Reactions in the Na 2 CO 3 − SiO 2 system 4 Evolution of calcium carbonate

  35. − The Na 2 CO 3 − CaCO 3 system 1000 900 800 700 600 0 20 40 60 80 100 Kracek

  36. − The Na 2 CO 3 − CaCO 3 system 1000 900 Possible formation of a double carbonate 800 Also possible : calcination of CaCO 3 700 600 0 20 40 60 80 100 Kracek

  37. − Solid-state reactions between the two carbonates Coll. S. Papin (SGR), G. Matzen, E. Véron (CEMHTI) Mixture of the two carbonates (50/50) : significant reaction

  38. − Evolution of calcium carbonate in a ternary batch Two very different reaction paths depending on contacts with sodium carbonate Ternary batch 75 % SiO 2 13 % Na 2 CO 3 12 % CaCO 3 : < 1 one contact with Na 2 CO 3 for CaCO 3 grains (monodisperse grains) Double carbonate path : contacts Na 2 CO 3 - CaCO 3 → formation of a crystalline double carbonate. 25 ◦ C 760 ◦ C 760 ◦ C

  39. − Evolution of calcium carbonate in a ternary batch Two very different reaction paths depending on contacts with sodium carbonate Calcination path : no contacts with Na 2 CO 3 CaCO 3 → CaO + CO 2 formation of refractory calcium oxide

  40. − A clue for explaining chemical segregation ? [Chopinet et al., Glass. Tech. 2010]

  41. − Bubbles Bubbles are created as a result of the production of melts and the deconnexion of the granular network : open pores between grains are closed down by the melts.

  42. − Bubbles ⇒ the initial distribution of bubble sizes is partially determined by the geometry of the granular packing Need for faster acquisitions to follow bubbles creation and evolution.

  43. − Domain coarsening in phase-separating glasses PhD of David Bouttes Barium-borosilicate glass Phase-separation in liquid state (1000 - 1400 ◦ C) ID19 t = 65 min t = 42 min t = 17 min t = 25 min Evolution of the shape of the domains Hydrodynamical regime

  44. − Conclusions In-situ tomography : a great technique for studying glass melting Quantitative data on transformations Rich source of inspiration Needs to be coupled with other techniques The technique is still developing Towards faster and faster imaging Challenging data processing Could in-situ tomography be used to study other systems in glass science ?

  45. − Thank you for your attention !

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