Matter transport Sintering is possible only if the atoms can diffuse to form the necks that weld the particles with one another. The transport of matter can occur in vapor phase, in a liquid, by diffusion in a crystal, or through the viscous flow of a glass. J = (D/kT)(dP/dx) (vapor phase) J is the flow of atoms passing through a unit surface, per time unit, D the diffusion coefficient of the species that diffuses and k is the Boltzmann constant ,T temperature, dP/dx the difference in pressure between the two sides of an interface causes a matter flow. J = (– DLiquid/ kT)(?P/L) (liquid phase) where DLiquid is transport coefficient in the liquid , L viscous liquid flow rate , ?P grows homothetically, particles p at times coarser imply neck. Most mechanisms are activated thermally because the action of temperature is necessary to overcome the potential barrier between the initial state of higher energy (compacted powder) and the final state of lower energy (consolidated material). Atomic diffusion in ceramics is sufficiently rapid only at temperatures higher than 0.6-0.8 TF, where TF is the melting point (in K). For alumina, for example, which melts at around 2,320 K the sintering temperature chosen is generally around 1,900 K. The matter movement takes place from the high energy areas towards the low energy areas , primarily, the sintering neck between the particles. We must distinguish two cases depending on the location of the source of matter: – when the source of matter is the surface, the mechanism is nondensifying, which means that the spheres take an ellipsoidal form, without their centers approaching one another. There is no macroscopic shrinkage and the porosity of the granular compact is not reduced significantly. The decrease in interfacial energy primarily comes from the grain coarsening. – when the source of matter is inside the grains (near the boundaries, or near defects such as dislocations), the mechanism is densifying: there is shrinkage and reduction in porosity. Sintering -------------------Lecture (4) 13 For solid phase sintering, there are four ways of diffusion: i) surface diffusion. ii) volume diffusion (often called lattice diffusion). iii) vapor phase transport (evaporation-condensation. iv) grain boundary diffusion: the boundaries are very disturbed areas, which allow “diffusion short-circuits”. For liquid phase sintering, we must add dissolution-reprecipitation effects or a vitreous flow. Finally, for pressure sintering the pressure exerted allows the plastic deformation of the crystallized phases and the viscous flow of the amorphous phases. SINTERING AND DIFFUSION There is a significant difference between the paths for matter transport. Transfer of material into the “pore” must occur if the porosity of the compact is to shrink. You can imagine that in three dimensions (3D), this requires that matter transfer from the bulk of the grain, from the GB between particles, or from the outer surface by diffusion through the grain or through the GB. (Alternatively, you can think of vacancies moving out from the pores.) For the case of matter transport from the grain boundary to the neck by lattice diffusion, we can derive an equation for the rate of growth of the neck area between particles. x r = ( 40?a3D? kT )1/5 r-3/5 t1/5 Here, the volume of the diffusing vacancy is a3 and D* is the selfdiffusion coefficient , x is the neck radius , r the radius of the particles, t time , ? is the specific interface energy. REACTION SINTERING reactive sintering, is a particular type of sintering process in which the chemical reaction of the starting materials and the densification of the powder compact are both achieved in a single heat treatment step. These systems can be divided into two main classes depending on whether single-phase solids or composites are produced. For a powder compact consisting of a mixture of two reactant powders, the simplest example of reaction. Sintering -------------------Lecture (4) 14 During sintering, reaction between two starting powders A (e.g., ZnO) and B (e.g., Fe2O3) and densification occur to produce a polycrystalline, single-phase solid C (e.g., ZnFe2O4): ZnO + Fe O ? ZnFe2O4 A more complex example of reaction sintering .Reaction between two starting powders D (e.g., Al2O3) and E (e.g., zircon, ZrSiO4) and densification occur to produce a composite solid consisting of two phases F (mullite, 3Al2O3_2SiO2) and G (ZrO2): 3 Al2O3 +2 (ZrO2 . SiO2)? 3Al2O3+2SiO2 +2 ZrO2 The energy changes for chemical reaction are much larger than those for surface area changes and it would be very desirable if the free energy of the reaction could be used to drive the densification process. ZnFe2O4 as an example, the conventional route for producing a dense polycrystalline solid involves calcinations of a loose mixture of ZnO and Fe2O3 powders to form a single-phase ZnFe2O4 powder, milling the calcined powder to break down agglomerates, followed by powder compaction and sintering. In reaction sintering, the reaction and densification occurs in the same heating cycle, so the calcination and subsequent milling steps in the conventional route are eliminated.
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