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Updated: May 2, 2026

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Magnetically Induced Rotating Rayleigh-Taylor Instability
Published on: March 3, 2017
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Faraday instability in a near-critical fluid under weightlessness
G Gandikota1, D Chatain1, S Amiroudine2
1SBT, UMR-E CEA/UJF-Grenoble 1, INAC, Grenoble F-38054, France.
Summary
Near-critical hydrogen experiments reveal Faraday instability transitions. Vibration creates patterns, with density differences dictating square or line formations and wavelength changes near the critical point.
Area of Science:
- Fluid dynamics
- Thermodynamics
- Phase transitions
Background:
- Faraday instability, typically observed under gravity, is studied in zero-gravity conditions using near-critical hydrogen.
- Magnetic compensation of gravity is employed to simulate zero-gravity effects on the liquid-vapor interface.
- Understanding interfacial instabilities is crucial for fluid behavior in microgravity environments.
Purpose of the Study:
- To investigate Faraday instability at the liquid-vapor interface of near-critical hydrogen under simulated zero-gravity conditions.
- To analyze pattern transitions (square to line) and their dependence on proximity to the critical point.
- To compare experimental findings with theoretical predictions for zero-gravity instabilities.
Main Methods:
- Experiments conducted on near-critical hydrogen with magnetic compensation of gravity.
- Application of vibration to destabilize the liquid-vapor interface.
- Observation and analysis of interfacial patterns and wavelength changes.
Main Results:
- Confirmation of Faraday waves in zero-gravity conditions.
- Observed transition from square to line patterns near the critical point.
- Demonstrated transition from Faraday instability to periodic layering as the liquid-vapor density difference decreases.
Conclusions:
- Faraday wave instability is favored when the liquid-vapor density difference is large.
- Periodic layering predominates near the critical point where density differences are small.
- The wavelength of Faraday waves decreases approaching the critical point, consistent with theory except for pattern transitions observed near the critical point.
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