Add notes on diffusion
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@ -1065,3 +1065,68 @@ $$\sigma_{yield} = \sigma_0 + k_yd^{-0.5}$$
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where $d$ is the grain size and $\sigma_0$ and $k_y$ are material constants.
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Therefore a plot of $\sigma_{yield}$ against $d^{-0.5}$ would results in a straight line.
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# Diffusion
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Diffusion is atomic or ionic movement down a concentration gradient.
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## Solid State Diffusion
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![](./images/vimscrot-2021-12-22T13:54:09,340198890+00:00.png)
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Solid state diffusion is the stepwise migration (*march*) of atoms or ions through a lattice, from
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site to site.
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In order for this to happen, there must an adjacent vacant site.
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The diffusion particle must also have sufficient thermal energy to 'jump' to the new site.
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### Vacancy Diffusion (Diffusion of Metal Ions)
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![](./images/vimscrot-2021-12-22T13:59:03,553059517+00:00.png)
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### Interstitial DIffusion (Diffusion of Small, Non-Metallic Particles)
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![](./images/vimscrot-2021-12-22T13:59:53,080635889+00:00.png)
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## The Math(s) of Diffusion
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Diffusion is time dependent.
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For steady state diffusion, Fick's 1st Law holds:
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$$J = -D \frac{\mathrm{d}C}{\mathrm{d}x}$$
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where $J$ is the *flux*, $\frac{\mathrm{d}C}{\mathrm dx}$ is the concentration gradient, and $D$ is
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the constant of proportionality known as the *diffusion coefficient*.
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$D$ is constant for a particular metal at a particular temperature.
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The *flux*is the number of atoms or ions moving per second through a cross sectional area.
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### Things that Affect the Speed of Diffusion
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- size of the diffusion species --- smaller species results in faster diffusion
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- temperature --- more thermal energy allows more particles to have enough energy to make the 'jump'
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- host lattice
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- simple cubic --- 52% occupancy of ions
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- body centered cubic --- 68% occupancy of ions
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- face centered cubic --- 74% occupancy of ions
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Diffusion is faster in a BCC host than in an FCC host for iron ions in an iron host and also for
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carbon atoms diffusing into an iron host.
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However this is not always the case.
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### Influence of Temperature on Diffusion (Arrhenius Equation)
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You can apply the Arrhenius equation for all thermally activated diffusion:
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$$D = D_0 \exp{\left( - \frac{Q}{RT} \right)}$$
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where $Q$ is the activation energy and $R$ is the ideal gas constant (8.31 J k$^{-1}$ mol$^{-1}$).
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# Glossary
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- liquidus - for a system of more than one component, the liquidus is the lowest temperature at
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which the whole system is all in the liquid state.
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- solidus - for a system of more than one component, the solidus is the highest temperature at which
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the whole system is still in the solid state
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