Related Experiment Video
Updated: Jun 29, 2026

11:00
Experimental Investigation of Secondary Flow Structures Downstream of a Model Type IV Stent Failure in a 180° Curved Artery Test Section
Published on: July 19, 2016
Variational principle in dynamics of a vortex filament
1Mechanical Engineering, Wayne State University, Detroit, Michigan 48202, USA.
Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|October 15, 2008
Summary
This study presents a refined variational principle for vortex filament dynamics in fluid flow, accounting for additional terms. The new principle reveals that vortex filament length can evolve during motion, unlike previous approximations.
Area of Science:
- Fluid Dynamics
- Theoretical Physics
- Vortex Dynamics
Background:
- Previous variational principles for vortex filaments approximated dynamics by considering logarithmically large terms.
- These approximations assumed constant filament length (L) during motion, as the Hamiltonian was solely a function of L.
Purpose of the Study:
- To develop a more precise variational principle for vortex filament dynamics.
- To incorporate terms of order unity into the variational principle.
- To investigate the evolution of vortex filament length.
Main Methods:
- Derivation of a new variational principle for vortex filament dynamics.
- Building upon a recently established variational principle for arbitrary vortex motion in incompressible inviscid fluids.
- Inclusion of higher-order terms beyond logarithmic approximations.
Main Results:
- A novel variational principle for vortex filament dynamics is established.
- The refined theory reveals that vortex filament length is not constant but can evolve.
- This evolution is a characteristic feature of the more precise theoretical framework.
Conclusions:
- The developed variational principle offers a more accurate description of vortex filament dynamics.
- The dynamic evolution of filament length is a key finding, expanding upon prior approximations.
- This work advances the theoretical understanding of fluid dynamics and vortex behavior.
Related Concept Videos
Stokes' Law
Viscous forces, like friction, are intermolecular forces that resist the relative motion of molecules over each other. When a solid body moves through a liquid, viscous forces drag it in the opposite direction. The force's magnitude depends on the solid's shape and size, as well as its speed and the liquid's coefficient of viscosity, density and temperature.
The expression for the force on a solid spherical object in a fluid is called Stokes' law. Stokes' law is valid only for low Reynolds...
The expression for the force on a solid spherical object in a fluid is called Stokes' law. Stokes' law is valid only for low Reynolds...
Velocity Potential
In steady, incompressible flow through a long, straight pipe with a uniform cross-section, the flow in the central region (far from the pipe walls) is irrotational. This irrotational nature means that fluid particles do not rotate around their axes, and a scalar function called the velocity potential, represented by ϕ, can be used to describe their movement. In irrotational flows, the velocity field V is defined as the gradient of the velocity potential:
Irrotational Flow
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:
Bernoulli's Equation
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...
Euler's Equations of Motion
In fluid mechanics, shear stresses arise from viscosity, which represents a fluid's internal resistance to deformation. For low-viscosity fluids, like water, these stresses are minimal, simplifying flow analysis by allowing the fluid to be treated as inviscid, or frictionless. In an inviscid fluid, shear stresses are absent, leaving only normal stresses, which act perpendicularly to fluid elements. Notably, pressure — defined as the negative of the normal stress — remains uniform across...
Principle of Moments
The principle of moments, also known as Varignon's theorem, is a fundamental concept in physics and engineering that describes the equilibrium of a rigid body under the influence of external forces. The principle states that the moment of a force about a point is equal to the sum of the moments of the components of the force about the same point.
The moment is calculated by multiplying the magnitude of the force by the perpendicular distance from the point of application to the point about...
The moment is calculated by multiplying the magnitude of the force by the perpendicular distance from the point of application to the point about...

