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March 6, 2026Journal of Fluid Mechanics0 citationsOpen Access

Interface tracking simulation for subcooled flow boiling of water at 10 bar

YSYohei SatoAKArtyom KossolapovBNBojan Ničeno

Key Points

  • The study aims to clarify heat-transfer mechanisms in subcooled flow boiling of water at moderate pressure and validate the simulation method.
  • Computational fluid dynamics simulation using an interface tracking method.
  • Simulation conditions modeled after an MIT experiment with specific applied heat flux and subcooling.
  • Fine grids employed to accurately model small bubble sizes at high pressure.
  • Simulated bubble shapes and wall temperatures aligned closely with experimental results.
  • A highly effective thin liquid layer around bubbles enhances heat removal from the surface.
  • Local wall heat fluxes were approximately 0.9 MW/m² under medium bubbles and 0.4 MW/m² under large bubbles due to thicker liquid films.
  • Heat transfer coefficient in the single-phase liquid reached 42 kW/m²/K, indicating strong turbulence.

Abstract

A computational fluid dynamics simulation of subcooled flow boiling of water at 10. 5 bar, with an applied heat flux of 1\, MW\, m^-2 and subcooling of 10 K, was performed using an interface tracking method. The simulation replicated the conditions of an experiment conducted at MIT. The objectives are to elucidate heat-transfer mechanisms in moderate-pressure subcooled boiling and to validate the simulation method, with a focus on quantities that are difficult to measure experimentally, such as the distributions of velocity, temperature, bubble number density and heat-flux partitioning. Due to the small bubble size under high pressure, fine grids are required. Simulated bubble shapes, wall temperatures and vapour area fractions show good agreement with the experimental results. The simulations reveal that a very thin liquid layer (4\, x03BC m) surrounding the bubbles is highly effective at removing heat from the surface. The local wall heat fluxes beneath medium and large bubbles, excluding the heat flux associated with seed-bubble generation, are approximately 0. 9 and 0. 4 MW\, m^-2, respectively; the latter is smaller because of the presence of thicker liquid films (14–70 x03BC m) that thermally insulate the wall. In the single-phase liquid region, the heat transfer coefficient reaches 42\, kW\, m^-2\, K^-1 as a result of strong turbulent heat flux in the wall-normal direction; this turbulent heat flux is approximately eight times larger than in the equivalent single-phase liquid flow.

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Cite This Study

Sato et al. (2026) studied this question.

synapsesocial.com/papers/69aa70a9531e4c4a9ff5aa32https://doi.org/10.1017/jfm.2026.11253
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