Boundary-condition control of reaction–diffusion band spacing in metamorphic rocks

Abstract We develop a reaction--diffusion model of the activator--inhibitor type for metamorphic band spacing, with a slowly diffusing solid phase as activator and a rapidly diffusing fluid phase as inhibitor. We show that the observable spacing is selected not by the critical wavelength $\lambda_c$ alone but by mode locking: on a finite domain, the boundaries quantise the admissible wavenumbers and lock the pattern onto the nearest permitted mode. Linear stability analysis yields $d_c \approx 43.4$ and $\lambda_c = 2\pi (D_u D_v / \det \JJ)^{1/4}$. Neumann boundaries on hand-specimen-sized domains shift the observed spacing by up to $29\,\%$ from $\lambda_c$. We map $d_c(k_3,k_4)$ over three orders of magnitude and provide a calibration recipe linking model parameters to petrological observables. For the East Kimberley zebra rock, the predicted spacing of $0.3$--$12$~mm brackets the observed $3$--$10$~mm. We state explicitly what the model predicts and what it only permits. \bigskip\noindent\textbf{Keywords:} reaction--diffusion; activator--inhibitor kinetics; Turing instability; metamorphic banding; zebra rock; orbicular granite; boundary conditions; finite-difference modelling; Onsager coefficients.

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Publication Details

Journal
Research Square
Published
2026-11-09
DOI
https://doi.org/10.21203/rs.3.rs-11323379/v1
Primary Topic
Nonlinear Dynamics and Pattern Formation
Type
preprint
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preprint

Boundary-condition control of reaction–diffusion band spacing in metamorphic rocks

Manas Kumar Roy, Biswajit Saha
2 links
Research Square
Nonlinear Dynamics and Pattern Formation
preprint

Boundary-condition control of reaction–diffusion band spacing in metamorphic rocks

Manas Kumar Roy, Biswajit Saha
preprint en

Abstract

Abstract We develop a reaction--diffusion model of the activator--inhibitor type for metamorphic band spacing, with a slowly diffusing solid phase as activator and a rapidly diffusing fluid phase as inhibitor. We show that the observable spacing is selected not by the critical wavelength $\lambda_c$ alone but by mode locking: on a finite domain, the boundaries quantise the admissible wavenumbers and lock the pattern onto the nearest permitted mode. Linear stability analysis yields $d_c \approx 43.4$ and $\lambda_c = 2\pi (D_u D_v / \det \JJ)^{1/4}$. Neumann boundaries on hand-specimen-sized domains shift the observed spacing by up to $29\,\%$ from $\lambda_c$. We map $d_c(k_3,k_4)$ over three orders of magnitude and provide a calibration recipe linking model parameters to petrological observables. For the East Kimberley zebra rock, the predicted spacing of $0.3$--$12$~mm brackets the observed $3$--$10$~mm. We state explicitly what the model predicts and what it only permits. \bigskip\noindent\textbf{Keywords:} reaction--diffusion; activator--inhibitor kinetics; Turing instability; metamorphic banding; zebra rock; orbicular granite; boundary conditions; finite-difference modelling; Onsager coefficients.

Research Square
Gobardanga Hindu College (IN), Brahmananda Keshab Chandra College (IN)
Nonlinear Dynamics and Pattern Formation
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