Related Experiment Video
Updated: Jun 18, 2025

06:42
Magnetically Induced Rotating Rayleigh-Taylor Instability
Published on: March 3, 2017
9.5K
Lagrangian Irreversibility and Energy Exchanges in Rotating-Stratified Turbulent Flows
S Gallon1, A Sozza1,2, F Feraco3,4
1Univ Lyon, <a href="https://ror.org/04zmssz18">ENS de Lyon</a>, CNRS, Laboratoire de Physique, F-69342 Lyon, France.
Physical Review Letters
|July 29, 2024
Summary
In stratified and rotating turbulent flows, particle separation dictates energy transfer. Below a characteristic length, potential energy converts to kinetic energy, reducing irreversibility.
Area of Science:
- Fluid dynamics
- Turbulence research
- Geophysical flows
Background:
- Stratified and rotating turbulent flows exhibit complex interactions between waves and eddies.
- These interactions drive continuous energy exchanges between potential and kinetic energy forms.
Purpose of the Study:
- To investigate the impact of wave-eddy interplay on the turbulent energy cascade.
- To analyze how these processes influence the irreversible evolution of kinetic energy between tracer particles.
Main Methods:
- Analysis of turbulent energy cascade dynamics.
- Examination of relative kinetic energy evolution between tracer particles at varying separations.
- Identification of characteristic length scales governing energy transfer.
Main Results:
- A characteristic length scale (ℓt) was identified, influencing energy transfer direction based on particle separation (r0).
- When r0 < ℓt, potential energy is transferred to kinetic energy, decreasing irreversibility.
- When r0 > ℓt, the opposite energy transfer occurs, increasing irreversibility.
- The characteristic length scale ℓt was found to coincide with the buoyancy length scale (LB) across many configurations.
Conclusions:
- The study reveals a scale-dependent mechanism controlling energy transfer and irreversibility in stratified and rotating turbulence.
- The buoyancy length scale (LB) plays a crucial role in this energy transfer process.
- A transition to a wave-dominated regime was observed, altering the dynamics beyond a certain scale.
Related Concept Videos
Irrotational Flow
437
Irrotational flow is characterized by fluid motion where particles do not rotate around their axes, resulting in zero vorticity. For a flow to be irrotational, the curl of the velocity field must be zero. This imposes specific conditions on velocity gradients. For instance, to maintain zero rotation about the z-axis, the gradient condition:
437
Energy Conservation and Bernoulli's Equation
8.9K
Applying the conservation of energy principle or the work-energy theorem to an incompressible, inviscid fluid in laminar, steady, irrotational flow leads to Bernoulli's equation. It states that the sum of the fluid pressure, potential, and kinetic energy per unit volume is constant along a streamline.
All the terms in the equation have the dimension of energy per unit volume. The kinetic energy per unit volume is called the kinetic energy density, and the potential energy per unit volume is...
All the terms in the equation have the dimension of energy per unit volume. The kinetic energy per unit volume is called the kinetic energy density, and the potential energy per unit volume is...
8.9K
Conservation of Energy in Control Volume
829
Consider a turbine operating under steady-flow conditions. The control volume is drawn around the turbine, with fluid entering at one point and exiting at another. The turbine extracts energy from the fluid, which performs mechanical work (shaft work).
For steady flow systems, the time derivative of the stored energy becomes zero since there is no energy accumulation within the control volume. This simplifies the energy equation to:
For steady flow systems, the time derivative of the stored energy becomes zero since there is no energy accumulation within the control volume. This simplifies the energy equation to:
829
Reversible and Irreversible Processes
4.2K
The thermodynamic processes can be classified into reversible and irreversible processes. The processes that can be restored to their initial state are called reversible processes. It is only possible if the process is in quasi-static equilibrium, i.e., it takes place in infinitesimally small steps, and the system remains at equilibrium However, these are ideal processes and do not occur naturally. An ideal system undergoing a reversible process is always in thermodynamic equilibrium within...
4.2K
Bernoulli's Equation
10.4K
In the middle of the nineteenth century, it was observed that two trains passing each other at a high relative speed get pulled towards each other. The same occurs when two cars pass each other at a high relative speed. The reason is that the fluid pressure drops in the region where the fluid speeds up. As the air between the trains or the cars increases in speed, its pressure reduces. The pressure on the outer parts of the vehicles is still the atmospheric pressure, while the resultant...
10.4K
Turbulent Flow
162
Turbulent flow is characterized by unpredictable fluctuations in velocity and pressure, which result in a chaotic fluid movement distinct from the orderly patterns of laminar flow. While laminar flow is governed by smooth, parallel layers with minimal mixing, turbulent flow exhibits highly irregular, three-dimensional patterns. This behavior arises due to instabilities in the fluid's velocity profile, and amplifies as the flow velocity increases. Minor disturbances, known as turbulent...
162

