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Grain growth in the initial deposit

This equation is derived by considering the transfer of material from a flat surface to a droplet. For the transfer of a small mass Sm from the flat surface of vapour pressure p° to the droplet of vapour pressure p, the Gibbs energy of transfer is [Pg.30]

The addition of this small mass increases the radius of the droplet, r, to r + dr, and the surface area by 8jrr dr. If the fluid density is p, then the [Pg.30]

The term f rin p/p° is clearly the chemical potential of a surface of radius r with respect to a flat surface of the same material as standard state. It follows that the difference in chemical potential between two surfaces, p1 — p11, where surface I is convex of radius n, and the other surface II is concave of radius r2 is given by [Pg.31]

The Einstein equation for the flux of atoms across the interface is [Pg.31]

The mobility, M, is a function of the substance, and obeys an Arrhenius expression M = Mo exp — (AE/RT) where AE is the energy of transfer across the grain boundary. [Pg.31]


See other pages where Grain growth in the initial deposit is mentioned: [Pg.30]    [Pg.30]   


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