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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.
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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.
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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).
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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).
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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.
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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.
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Analysis of Coarse-grained Stochastic Reaction-diffusion Equations for Schloegl's Second Model on A Square Lattice. Here, Ac C1/2 (P+C- C2) 1/2 Ac Is the Nonconserved Particle Annihilation-creation Noise, and Diff ∇ [h1/2 C1/2 (1-C) 1/2 Diff] Is the Conserved Particle Diffusion Noise. Ac and Diff Are Independent White Noises."
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