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Purpose of this talk. Diffusion. Ronald Griessen ACTS workshop May 24, 2007. Water droplet. Waves. Wave equation. Diffusion. Fick’s law Equation of continuity. J. dx. C(x,t). Singularities decay immediately. is a solution of. Diffusion in semi-infinite space.
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Purpose of this talk Diffusion Ronald Griessen ACTS workshop May 24, 2007
Waves Wave equation
Fick’s law Equation of continuity J dx C(x,t)
Singularities decay immediately is a solution of
Cu Pd Y Pd
Cu Pd
Cu Pd Cu Pd
Cu Pd Cu Y Pd Y
Cu Pd Cu Y Pd Y
Cu Pd Cu Y Pd Pd
Fast H diffusion in bcc Pd-Cu Y Pd Cu Pd
Fast H diffusion in bcc Pd-Cu Temperature oC Cu atomic percent palladium
Fick’s law Equation of continuity ? ? dx Is this true Is this true
Pressure-composition isotherm of YHx at T=293 K Kooij et al. 1999
H Hydrogenography in Yttrium Y2O3 Pd Y Den Broeder, van der Molen et al, Nature 394 (1998) 656
3 g hcp- H/Y g hcp- 2 b metal insulator 1 a 0
3 g hcp- H/Y g hcp- 2 b metal insulator 1 a 0
This picture demonstrates that instead of
Switchable mirrors as indicators H Y2O3 Pd Y V SiO2
Sample architecture SiO2 V V
Sample architecture Pd 10 nm Y 50 nm SiO2 V V
Hydrogen loading Pd Y SiO2 V V H x=0 x
H-loading: 473K, 1mbar, 3h Pd x=0 10 mm dV 25 nm 50 nm 75 nm 100 nm 125 nm YH2 front x
Diffusion in a multilayer The chemical potential MUST be continuous The concentration MAY have discontinuities
? Usual diffusion Real diffusion
Usual diffusion Real diffusion However, the chemical potential MUST be continuous
Ni Ni Mg Mg Ti Ti
c = c(x,t) cH = f(t) Ni Ni Mg Mg Ti Ti
c = c(x,t) cH = f(t) Ni Ni Mg Fast loading, Very slow unloading Mg Ti Ti Relatively slow loading, Very fast unloading
Random walk of a photon With vthe velocity of light athe absorption coefficient
Sample architecture Y 50 nm V 250 nm SiO2 V 50 nm Pd 10 nm
Hydrogen loading 32 min 1 bar 373 K V 250 nm V 50 nm YH2 YH3 Pd
110 min 1 bar 373 K YH2 YH3 Pd