JACOBI SHAPE TRANSITIONS WITHIN THE LSD MODEL AND THE SKYRME-ETF APPROACH

2008 ◽  
Vol 17 (01) ◽  
pp. 100-109 ◽  
Author(s):  
JOHANN BARTEL ◽  
KRZYSZTOF POMORSKI

The "Modified Funny-Hills parametrisation" is used together with the Lublin-Strasbourg Drop Model to evaluate the stability of rotating nuclei. The Jacobi transition into triaxial shapes is studied. By a comparison with selfconsistent semiclassical calculations in the framework of the Extended Thomas-Fermi method, the validity of the present approach is demonstrated and possible improvements are indicated.

1977 ◽  
Vol 66 (1) ◽  
pp. 23-24 ◽  
Author(s):  
W. Stocker
Keyword(s):  

2009 ◽  
Vol 18 (04) ◽  
pp. 986-995 ◽  
Author(s):  
JOHANN BARTEL ◽  
BOZENA NERLO-POMORSKA ◽  
KRZYSZTOF POMORSKI

The "Modified Funny-Hills parametrisation" is used together with the Lublin-Strasbourg Drop Model and Strutinsky type shell corrections to determine the stability of hot rotating nuclei. Both the macroscopic and the microscopic part of the nuclear energy are evaluated by taking into account their dependence on the nuclear temperature and the rotational angular momentum. The Jacobi transition into triaxial shapes and the centrifugal-fission instability are studied.


2001 ◽  
Vol 687 (1-2) ◽  
pp. 206-211 ◽  
Author(s):  
A.L. Goodman

2011 ◽  
Vol 20 (10) ◽  
pp. 1995-2002 ◽  
Author(s):  
MICHAEL ROTONDO ◽  
REMO RUFFINI ◽  
SHE-SHENG XUE ◽  
VLADIMIR POPOV

In a unified treatment we extrapolate results for neutral atoms with heavy nuclei to nuclear matter cores of stellar dimensions with mass numbers A ≈ (m Planck /mn)3 ~ 1057. We give explicit analytic solutions for the relativistic Thomas–Fermi equation of Nn neutrons, Np protons and Ne electrons in beta equilibrium, fulfilling global charge neutrality, with Np = Ne. We give explicit expressions for the physical parameters including the Coulomb and the surface energies and we study as well the stability of such configurations. Analogous to heavy nuclei these macroscopic cores exhibit an overcritical electric field near their surface.


1991 ◽  
Vol 270 (1) ◽  
pp. 6-10 ◽  
Author(s):  
J. Gallego ◽  
S. Das Gupta
Keyword(s):  

Pramana ◽  
1980 ◽  
Vol 14 (1) ◽  
pp. 97-102
Author(s):  
K Andhradev ◽  
R G Kulkarni

1996 ◽  
Vol 74 (6) ◽  
pp. 965-968 ◽  
Author(s):  
Dennis P. Clougherty

The stability of He@C60 and Ne@C60 is discussed in the context of a spherical model where the carbon atoms are smeared out into a uniform shell. The electronic properties of the 60 π-electrons together with those of the central atom are treated in the Thomas–Fermi approximation. Simple electrostatic reasoning elucidates the nature of the radial stability of the complex. A method to include nonspherical corrections is outlined. Possible bonding topologies of the central atom and the C60 cage are discussed, as well as the relevance of these topologies to incipient central atom distortions. Key words: fullerenes, Thomas–Fermi, dopeyball, He@C60, Ne@C60.


2004 ◽  
Vol 10 (3) ◽  
pp. 227-232 ◽  
Author(s):  
Jerzy T. Sawicki ◽  
T. V. V. L. N. Rao

A computational procedure for the mechanism of shear between the liquid sublayer and air cavity in the cavitation zone of a submerged journal bearing is presented here. Using the mass conservation principle, Elrod's universal equation is modified to take into consideration the shear of the air cavity in the cavitation region. Results of steady state and transient response for the submerged journal bearing using the present approach are compared with the universal equation based on the striated flow in the cavitation region. At steady state, the angular extent of cavitation region predicted by the present approach is higher than that predicted by Elrod's model and the limit cycle journal transient response using the present approach predicts higher eccentricity ratios.


1995 ◽  
Vol 300 ◽  
pp. 117-147 ◽  
Author(s):  
Rama Govindarajan ◽  
R. Narasimha

A new formulation of the stability of boundary-layer flows in pressure gradients is presented, taking into account the spatial development of the flow and utilizing a special coordinate transformation. The formulation assumes that disturbance wavelength and eigenfunction vary downstream no more rapidly than the boundary-layer thickness, and includes all terms nominally of orderR−1in the boundary-layer Reynolds numberR. In Blasius flow, the present approach is consistent with that of Bertolottiet al.(1992) toO(R−1) but simpler (i.e. has fewer terms), and may best be seen as providing a parametric differential equation which can be solved without having to march in space. The computed neutral boundaries depend strongly on distance from the surface, but the one corresponding to the inner maximum of the streamwise velocity perturbation happens to be close to the parallel flow (Orr-Sommerfeld) boundary. For this quantity, solutions for the Falkner-Skan flows show the effects of spatial growth to be striking only in the presence of strong adverse pressure gradients. As a rational analysis toO(R−1) demands inclusion of higher-order corrections on the mean flow, an illustrative calculation of one such correction, due to the displacement effect of the boundary layer, is made, and shown to have a significant destabilizing influence on the stability boundary in strong adverse pressure gradients. The effect of non-parallelism on the growth of relatively high frequencies can be significant at low Reynolds numbers, but is marginal in other cases. As an extension of the present approach, a method of dealing with non-similar flows is also presented and illustrated.However, inherent in the transformation underlying the present approach is a lower-order non-parallel theory, which is obtained by dropping all terms of nominal orderR−1except those required for obtaining the lowest-order solution in the critical and wall layers. It is shown that a reduced Orr-Sommerfeld equation (in transformed coordinates) already contains the major effects of non-parallelism.


2014 ◽  
Vol 750 ◽  
pp. 144-190 ◽  
Author(s):  
Vivek Narsimhan ◽  
Andrew P. Spann ◽  
Eric S. G. Shaqfeh

AbstractWhen a flexible vesicle is placed in an extensional flow (planar or uniaxial), it undergoes two unique sets of shape transitions that to the best of the authors’ knowledge have not been observed for droplets. At intermediate reduced volumes (i.e. intermediate particle aspect ratio) and high extension rates, the vesicle stretches into an asymmetric dumbbell separated by a long, cylindrical thread. At low reduced volumes (i.e. high particle aspect ratio), the vesicle extends symmetrically without bound, in a manner similar to the breakup of liquid droplets. During this ‘burst’ phase, ‘pearling’ occasionally occurs, where the vesicle develops a series of periodic beads in its central neck. In this paper, we describe the physical mechanisms behind these seemingly unrelated instabilities by solving the Stokes flow equations around a single, fluid-filled particle whose interfacial dynamics is governed by a Helfrich energy (i.e. the membranes are inextensible with bending resistance). By examining the linear stability of the steady-state shapes, we determine that vesicles are destabilized by curvature changes on its interface, similar to the Rayleigh–Plateau phenomenon. This result suggests that the vesicle’s initial geometry plays a large role in its shape transitions under tension. The stability criteria calculated by our simulations and scaling analyses agree well with available experiments. We hope that this work will lend insight into the stretching dynamics of other types of biological particles with nearly incompressible membranes, such as cells.


Sign in / Sign up

Export Citation Format

Share Document