Related Experiment Video
Updated: Feb 23, 2026

10:11
Temperature-Controlled Assembly and Characterization of a Droplet Interface Bilayer
Published on: April 19, 2021
4.2K
Temperature profile in a liquid-vapour interface near the critical point
Henri Gouin1, Pierre Seppecher2,3
1Aix-Marseille Univ., Centrale Marseille, CNRS, M2P2 UMR 7340, 13451 Marseille, France.
Summary
This study introduces a thermocapillary fluid model for inhomogeneous fluids, expanding on existing theories by including energy and entropy densities. Near critical points, liquid-vapor interfaces behave similarly to the Cahn-Hilliard model.
Area of Science:
- Thermodynamics
- Fluid Dynamics
- Materials Science
Background:
- Existing models for inhomogeneous fluids, like Cahn-Hilliard, primarily consider mass-density gradients.
- Realistic molecular theories indicate entropy and temperature variations at liquid-vapor interfaces differ from bulk phases.
- A need exists for more comprehensive models of thermocapillary fluids accounting for multiple density expansions.
Purpose of the Study:
- To develop a more realistic model for thermocapillary fluids by incorporating energy, mass, and entropy density expansions.
- To modify the non-convex state law for inhomogeneous fluids using density gradient terms.
- To compare the behavior of liquid-vapor interfaces in the new model with the established Cahn-Hilliard model.
Main Methods:
- Expansion of thermodynamic state laws with respect to energy, mass, and entropy densities.
- Inclusion of terms accounting for density gradients in the modified state law.
- Application of a rescaling process near the critical point to analyze interface behavior.
Main Results:
- A modified state law for thermocapillary fluids is proposed, incorporating energy and entropy density gradients.
- The study demonstrates that liquid-vapor interfaces exhibit behavior consistent with the Cahn-Hilliard model near the critical point.
- The proposed model offers a more realistic description of inhomogeneous fluids compared to models based solely on mass-density gradients.
Conclusions:
- The developed thermocapillary fluid model provides a more accurate representation of inhomogeneous systems.
- Despite incorporating additional density terms, the fundamental behavior of liquid-vapor interfaces near critical points remains consistent with prior models.
- This research refines the understanding of fluid behavior at interfaces, particularly in the context of thermodynamic properties.
Related Concept Videos
pV-Diagrams
6.3K
The pV diagram, which is a graph of pressure versus volume of the gas under study, is helpful in describing certain aspects of the substance. When the substance behaves like an ideal gas, the ideal gas equation describes the relationship between its pressure and volume. On a pV diagram, it is common to plot an isotherm, which is a curve showing p as a function of V with the number of molecules and the temperature fixed. Then, for an ideal gas, the product of the pressure of the gas and its...
6.3K
Distillation: Vapor–Liquid Equilibria
4.8K
Distillation is a separation technique that takes advantage of the boiling point properties of disparate elements in a mixture. To perform distillation, we begin by heating a miscible mixture of two liquids with a significant difference in boiling points (at least 20°C). As the solution heats up and reaches the bubble point of the more volatile component, some molecules of the more volatile component transition into the gas phase and travel upward into the condenser, which is a glass tube...
4.8K
Vapor Pressure
41.3K
When a liquid vaporizes in a closed container, gas molecules cannot escape. As these gas phase molecules move randomly about, they will occasionally collide with the surface of the condensed phase, and in some cases, these collisions will result in the molecules re-entering the condensed phase. The change from the gas phase to the liquid is called condensation. When the rate of condensation becomes equal to the rate of vaporization, neither the amount of the liquid nor the amount of the vapor...
41.3K
Vapor Pressure of Fluid
2.0K
The vapor pressure of a fluid is a crucial concept in fluid mechanics, influencing phenomena such as boiling and cavitation. Vapor pressure refers to the pressure exerted by a vapor at a state of thermodynamic equilibrium with its corresponding liquid phase at a specific temperature. It represents the tendency of molecules to escape from the fluid surface into the vapor phase.
When a liquid is placed in a closed container with a small air space, and the space is evacuated, vapor molecules will...
When a liquid is placed in a closed container with a small air space, and the space is evacuated, vapor molecules will...
2.0K
Clausius-Clapeyron Equation
63.5K
The equilibrium between a liquid and its vapor depends on the temperature of the system; a rise in temperature causes a corresponding rise in the vapor pressure of its liquid. The Clausius-Clapeyron equation gives the quantitative relation between a substance’s vapor pressure (P) and its temperature (T); it predicts the rate at which vapor pressure increases per unit increase in temperature.
63.5K
Phase Transitions: Vaporization and Condensation
21.7K
The physical form of a substance changes on changing its temperature. For example, raising the temperature of a liquid causes the liquid to vaporize (convert into vapor). The process is called vaporization—a surface phenomenon. Vaporization occurs when the thermal motion of the molecules overcome the intermolecular forces, and the molecules (at the surface) escape into the gaseous state. When a liquid vaporizes in a closed container, gas molecules cannot escape. As these gas phase molecules...
21.7K

