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Updated: Mar 13, 2026

Ice Generation and the Heat and Mass Transfer Phenomena of Introducing Water to a Cold Bath of Brine
Published on: March 13, 2017
Thermodynamic origin of surface melting on ice crystals.
Ken-Ichiro Murata1, Harutoshi Asakawa2, Ken Nagashima3
1Institute of Low Temperature Science, Hokkaido University, Kita-ku, Sapporo 060-0819, Japan; murata@lowtem.hokudai.ac.jp.
Quasi-liquid layers (QLLs) on ice surfaces exhibit multiple wetting states and transitions, challenging the long-held belief of complete wetting. These QLLs are metastable, forming transiently rather than existing at equilibrium.
Area of Science:
- Physical Chemistry
- Materials Science
- Surface Science
Background:
- The conventional understanding posits that quasi-liquid layers (QLLs) homogeneously and completely wet ice surfaces, a concept originating from Michael Faraday's work.
- This widely accepted view has guided research in ice-surface interactions for decades.
Purpose of the Study:
- To challenge the established paradigm of complete wetting of ice surfaces by QLLs.
- To investigate the existence of multiple wetting states and thermodynamic behaviors of QLLs.
- To elucidate the formation conditions and equilibrium status of QLLs.
Main Methods:
- Theoretical modeling of interfacial potentials and wetting phenomena.
- Experimental validation of predicted QLL behaviors.
- Analysis of QLL formation under varying humidity conditions (supersaturation and undersaturation).
Main Results:
- Demonstrated that QLLs exhibit more than two distinct wetting states.
- Identified a first-order wetting transition between these QLL states.
- Showed that QLLs form under both supersaturated and undersaturated conditions, but are absent at equilibrium.
- Established QLLs as metastable transient states, not equilibrium phenomena.
Conclusions:
- The spontaneous formation of QLLs in ice-vapor equilibrium is questioned.
- A novel physical model explains the wetting and thermodynamic behaviors of QLLs.
- A unique interfacial potential is identified as the sole determinant of QLL properties.
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