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Volumn 130, Issue 7, 2009, Pages

Schloegl's second model for autocatalysis with particle diffusion: Lattice-gas realization exhibiting generic two-phase coexistence

Author keywords

[No Author keywords available]

Indexed keywords

DIFFUSION IN SOLIDS; STOCHASTIC MODELS;

EID: 60749088867     PISSN: 00219606     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.3074308     Document Type: Article
Times cited : (24)

References (57)
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    • For a planar interface with small slope y/x measured relative to S=1, the normal velocity is denoted V (S=1+h/x). By a Pythagorean construction, the velocity in the y -direction is y/t=V (S=1+h/x) [1+ (h/x) 2] 1/2 ≈ V0 +δV+1/2 V0 (h/x) 2, where V0 =V (S=1), and δV=V (S=1+h/x) -V (S=1) ≈C (h/x) 2 (Ref.). Thus, one has λ=2C+ V0.
    • For a planar interface with small slope y/x measured relative to S=1, the normal velocity is denoted V (S=1+h/x). By a Pythagorean construction, the velocity in the y -direction is y/t=V (S=1+h/x) [1+ (h/x) 2] 1/2 ≈ V0 +δV+1/2 V0 (h/x) 2, where V0 =V (S=1), and δV=V (S=1+h/x) -V (S=1) ≈C (h/x) 2 (Ref.). Thus, one has λ=2C+ V0.
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    • Writing ̃ eff (θ) ≈ av (h) +f (h) cos (4θ), it follows that eff (θ) ≈ av (h) -f (h) cos (4θ) /15. These identities are equivalent to Eqs. noting that ̃ 1 (h) = av (h) -f (h) and g (h) =2f (h).
    • Writing ̃ eff (θ) ≈ av (h) +f (h) cos (4θ), it follows that eff (θ) ≈ av (h) -f (h) cos (4θ) /15. These identities are equivalent to Eqs. noting that ̃ 1 (h) = av (h) -f (h) and g (h) =2f (h).
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    • An increasing number of vacuum clusters which nucleate just ahead of the interface can be incorporated into the advancing interface as time progresses corrupting estimation of V.
    • An increasing number of vacuum clusters which nucleate just ahead of the interface can be incorporated into the advancing interface as time progresses corrupting estimation of V.


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