2
Formation of vortex laments in the regions of bi-axial strain Konrad Bajer Warsaw University, Institute of Geophysics [email protected] The intricate structure of the vorticity eld at small scales of turbulence has been revealed in recent years. The idea that at least the dissipative scales of turbulence might be well represented by random distribution of vortex tubes was put forward by Burgers and pursued in the laboratory experiments by T own send. The evidenc e of intermittency was found in the statistical meausurements, the nature of the struc- ture s could not be veried. More recently the small- scale coherent structu res were identied in numerical simulations of fully developed turbulence and also visualised in laboratory experiments. The two approaches give estimates of the cross-sectional length scale of the coherent structures somewhere between the Kolmogorov scale and the Taylor microscale, the two being not far apart at the values of the Reynolds number that could be ach iev ed. The data is still too scarce for the denite scalin g of the cross-sectional length scale, if such denite scaling exists, to be derived. The intricate structure of the vorticity eld at small scales of turbulence has been revealed in recent years. The idea that at least the dissipative scales of turbulence might be well represented by random distribution of vortex tubes was put forward by Burgers and pursued in the laboratory experiments by T own send. The evidenc e of intermittency was found in the statistical meausurements, the nature of the struc- ture s could not be veried. More recently the small- scale coherent structu res were identied in numerical simulations of fully developed turbulence and also visualised in laboratory experiments. The two approaches give estimates of the cross-sectional length scale of the coherent structures somewhere between the Kolmogorov scale and the Taylor microscale, the two being not far apart at the values of the Reynolds number that could be ach iev ed. The data is still too scarce for the denite scalin g of the cross-sectional length scale, if such denite scaling exists, to be derived. The intricate structure of the vorticity eld at small scales of turbulence has been revealed in recent years. The idea that at least the dissipative scales of turbulence might be well represented by random distribution of vortex tubes was put forward by Burgers and pursued in the laboratory experiments by T own send. The evidenc e of intermittency was found in the statistical meausurements, the nature of the struc- ture s could not be veried. More recently the small- scale coherent structu res were identied in numerical simulations of fully developed turbulence and also visualised in laboratory experiments. The two approaches give estimates of the cross-sectional length scale of the coherent structures somewhere between the Kolmogorov scale and the Taylor microscale, the two being not far apart at the values of the Reynolds number that could be achieved. The structure at the core of a magnetic ux tube was discussed by Bajer & Moatt [1]. 1

Konrad Bajer- Formation of vortex laments in the regions of bi-axial strain

Embed Size (px)

Citation preview

Page 1: Konrad Bajer- Formation of vortex laments in the regions of bi-axial strain

8/3/2019 Konrad Bajer- Formation of vortex laments in the regions of bi-axial strain

http://slidepdf.com/reader/full/konrad-bajer-formation-of-vortex-laments-in-the-regions-of-bi-axial-strain 1/2

Formation of vortex filaments inthe regions of bi-axial strain

Konrad Bajer

Warsaw University, Institute of Geophysics

[email protected]

The intricate structure of the vorticity field at small scales of turbulence has been

revealed in recent years. The idea that at least the dissipative scales of turbulence

might be well represented by random distribution of vortex tubes was put forward

by Burgers and pursued in the laboratory experiments by Townsend. The evidence

of intermittency was found in the statistical meausurements, the nature of the struc-

tures could not be verified. More recently the small-scale coherent structures were

identified in numerical simulations of fully developed turbulence and also visualised

in laboratory experiments. The two approaches give estimates of the cross-sectional

length scale of the coherent structures somewhere between the Kolmogorov scale

and the Taylor microscale, the two being not far apart at the values of the Reynoldsnumber that could be achieved. The data is still too scarce for the definite scaling

of the cross-sectional length scale, if such definite scaling exists, to be derived.

The intricate structure of the vorticity field at small scales of turbulence has been

revealed in recent years. The idea that at least the dissipative scales of turbulence

might be well represented by random distribution of vortex tubes was put forward

by Burgers and pursued in the laboratory experiments by Townsend. The evidence

of intermittency was found in the statistical meausurements, the nature of the struc-

tures could not be verified. More recently the small-scale coherent structures were

identified in numerical simulations of fully developed turbulence and also visualised

in laboratory experiments. The two approaches give estimates of the cross-sectional

length scale of the coherent structures somewhere between the Kolmogorov scale

and the Taylor microscale, the two being not far apart at the values of the Reynolds

number that could be achieved. The data is still too scarce for the definite scaling

of the cross-sectional length scale, if such definite scaling exists, to be derived.

The intricate structure of the vorticity field at small scales of turbulence has been

revealed in recent years. The idea that at least the dissipative scales of turbulence

might be well represented by random distribution of vortex tubes was put forward

by Burgers and pursued in the laboratory experiments by Townsend. The evidence

of intermittency was found in the statistical meausurements, the nature of the struc-tures could not be verified. More recently the small-scale coherent structures were

identified in numerical simulations of fully developed turbulence and also visualised

in laboratory experiments. The two approaches give estimates of the cross-sectional

length scale of the coherent structures somewhere between the Kolmogorov scale

and the Taylor microscale, the two being not far apart at the values of the Reynolds

number that could be achieved. The structure at the core of a magnetic flux tube

was discussed by Bajer & Moffatt [1].

1

Page 2: Konrad Bajer- Formation of vortex laments in the regions of bi-axial strain

8/3/2019 Konrad Bajer- Formation of vortex laments in the regions of bi-axial strain

http://slidepdf.com/reader/full/konrad-bajer-formation-of-vortex-laments-in-the-regions-of-bi-axial-strain 2/2

a) b)

Figure 1: Solid with fluid-filled cylindrical cavity penetrated by the magnetic field which

is uniform at t = 0. of the streamlines around a line vortex

References

[1] Bajer, K. & Moffatt, H. K. (1997). On the effect of a central vortex on a stretched

magnetic flux tube. J. Fluid Mech. 339, 121–142.

[2] Bajer, K. (1998). Flux expulsion by a point vortex. Eur. J. Mech. B – Fluids,

17 (4), 653–664.

[3] Bajer, K. & Moffatt, H. K. (1998). Theory of non-axisymmetric Burgers vor-

tex with arbitrary Reynolds number. In Dynamics of Slender Vortices, Eds. E.

Krause & K. Gersten  Proceedings of the IUTAM Symposium held in Aachen,Germany, 31 August – 3 September 1997, pp. 193–202, Kluwer.

2