2,514 research outputs found
Experimental Basis and First Application of CLinical Lymphvessel-Transplantation of Secondary Lamphedema
Mathematical Models of Influenza A Virus Infection: Multiplicity of Infection and its Impact on Co-Infection and Virus Production
Parity properties of an advection-dominated solar \alpha^2\Om-dynamo
We have developed a high-precision code which solves the kinematic dynamo
problem both for given rotation law and meridional flow in the case of a low
eddy diffusivity of the order of cm/s known from the sunspot
decay. All our models work with an \alf-effect which is positive (negative) in
the northern (southern) hemisphere. It is concentrated in radial layers located
either at the top or at the bottom of the convection zone. We have also
considered an \alf-effect uniformly distributed in all the convection zone. In
the present paper the main attention is focused on i) the parity of the
solution, ii) the form of the butterfly diagram and iii) the phase relation of
the resulting field components. If the helioseismologically derived internal
solar rotation law is considered, a model without meridional flow of high
magnetic Reynolds number (corresponding to low eddy diffusivity) fails in all
the three issues in comparison with the observations. However, a meridional
flow with equatorial drift at the bottom of the convection zone of few meters
by second can indeed enforce the equatorward migration of the toroidal magnetic
field belts similar to the observed butterfly diagram but, the solution has
only a dipolar parity if the (positive) \alf-effect is located at the base of
the convection zone rather than at the top. We can, therefore, confirm the main
results of a similar study by Dikpati & Gilman (2001).Comment: 9 pages, 16 figures, to appear on Astronomy and Astrophysic
Bistability and hysteresis of dipolar dynamos generated by turbulent convection in rotating spherical shells
Bistability and hysteresis of magnetohydrodynamic dipolar dynamos generated by turbulent convection in rotating spherical fluid shells is demonstrated. Hysteresis appears as a transition between two distinct regimes of dipolar dynamos with rather different properties including a pronounced difference in the amplitude of the axisymmetric poloidal field component and in the form of the differential rotation. The bistability occurs from the onset of dynamo action up to about 9 times the critical value of the Rayleigh number for onset of convection and over a wide range of values of the ordinary and the magnetic Prandtl numbers including the value unity
Magnetoresistance, Micromagnetism and Domain Wall Effects in Epitaxial Fe and Co Structures with Stripe Domains
We review our recent magnetotransport and micromagnetic studies of
lithographically defined epitaxial thin film structures of bcc Fe and hcp Co
with stripe domains. Micromagnetic structure and resistivity anisotropy are
shown to be the predominant sources of low field magnetoresistance (MR) in
these microstructures, with domain wall (DW) effects smaller but observable
(DW-MR ). In Fe, at low temperature, in a regime in which fields
have a significant effect on electron trajectories, a novel negative DW
contribution to the resistivity is observed. In hcp Co microstructures,
temperature dependent transport measurements for current perpendicular and
parallel to walls show that any additional resistivity due to DW scattering is
very small.Comment: 7 pages, 8 figures, to appear in Journal of Applied Physics 199
Stability of density-stratified viscous Taylor-Couette flows
The stability of density-stratified viscous Taylor-Couette flows is
considered using the Boussinesq approximation but without any use of the
short-wave approximation. The flows which are unstable after the Rayleigh
criterion (\hat \mu<\hat \eta^2, with \hat \mu=\Omega_{out}/\Omega_{in} and
\hat \eta= R_{in}/R_{out}) now develop overstable axisymmetric Taylor vortices.
For the considered wide-gap container we find the nonaxisymmetric modes as the
most unstable ones. The nonaxisymmetric modes are unstable also beyond the
Rayleigh line. For such modes the instability condition seems simply to be
\hat\mu<1 as stressed by Yavneh, McWilliams & Molemaker (2001). However, we
never found unstable modes for too flat rotation laws fulfilling the condition
\hat \mu >\hat \eta. The Reynolds numbers rapidly grow to very high values if
this limit is approached (see Figs. 3 and 4).
Also striking is that the marginal stability lines for the higher do less
and less enter the region beyond the Rayleigh line so that we might have to
consider the stratorotational instability as a 'low- instability'. The
applicability of these results to the stability problem of accretion disks with
their strong stratification and fast rotation is shortly discussed.Comment: 7 pages, 7 figures, Astron. Astrophys. (subm.
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