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Dynamics and unsteady morphologies at ice interfaces driven by D2O-H2O exchange.


ABSTRACT: The growth dynamics of D2O ice in liquid H2O in a microfluidic device were investigated between the melting points of D2O ice (3.8 °C) and H2O ice (0 °C). As the temperature was decreased at rates between 0.002 °C/s and 0.1 °C/s, the ice front advanced but retreated immediately upon cessation of cooling, regardless of the temperature. This is a consequence of the competition between diffusion of H2O into the D2O ice, which favors melting of the interface, and the driving force for growth supplied by cooling. Raman microscopy tracked H/D exchange across the solid H2O-solid D2O interface, with diffusion coefficients consistent with transport of intact H2O molecules at the D2O ice interface. At fixed temperatures below 3 °C, the D2O ice front melted continuously, but at temperatures near 0 °C a scalloped interface morphology appeared with convex and concave sections that cycled between growth and retreat. This behavior, not observed for D2O ice in contact with D2O liquid or H2O ice in contact with H2O liquid, reflects a complex set of cooperative phenomena, including H/D exchange across the solid-liquid interface, latent heat exchange, local thermal gradients, and the Gibbs-Thomson effect on the melting points of the convex and concave features.

SUBMITTER: Drori R 

PROVIDER: S-EPMC5676873 | biostudies-other | 2017 Oct

REPOSITORIES: biostudies-other

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Dynamics and unsteady morphologies at ice interfaces driven by D<sub>2</sub>O-H<sub>2</sub>O exchange.

Drori Ran R   Holmes-Cerfon Miranda M   Kahr Bart B   Kohn Robert V RV   Ward Michael D MD  

Proceedings of the National Academy of Sciences of the United States of America 20171017 44


The growth dynamics of D<sub>2</sub>O ice in liquid H<sub>2</sub>O in a microfluidic device were investigated between the melting points of D<sub>2</sub>O ice (3.8 °C) and H<sub>2</sub>O ice (0 °C). As the temperature was decreased at rates between 0.002 °C/s and 0.1 °C/s, the ice front advanced but retreated immediately upon cessation of cooling, regardless of the temperature. This is a consequence of the competition between diffusion of H<sub>2</sub>O into the D<sub>2</sub>O ice, which favors  ...[more]

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