1,821 research outputs found
A compact design for a magnetic synchrotron to store beams of hydrogen atoms
We present a design for an atomic synchrotron consisting of 40 hybrid
magnetic hexapole lenses arranged in a circle. We show that for realistic
parameters, hydrogen atoms with a velocity up to 600 m/s can be stored in a
1-meter diameter ring, which implies that the atoms can be injected in the ring
directly from a pulsed supersonic beam source. This ring can be used to study
collisions between stored hydrogen atoms and molecular beams of many different
atoms and molecules. The advantage of using a synchrotron is two-fold: (i) the
collision partners move in the same direction as the stored atoms, resulting in
a small relative velocity and thus a low collision energy, and (ii) by storing
atoms for many round-trips, the sensitivity to collisions is enhanced by a
factor of 100-1000. In the proposed ring, the cross-sections for collisions
between hydrogen, the most abundant atom in the universe, with any atom or
molecule that can be put in a beam, including He, H, CO, ammonia and OH can
be measured at energies below 100 K. We discuss the possibility to use optical
transitions to load hydrogen atoms into the ring without influencing the atoms
that are already stored. In this way it will be possible to reach high
densities of stored hydrogen atoms.Comment: 9 pages, 3 figure
A pencil distributed finite difference code for strongly turbulent wall-bounded flows
We present a numerical scheme geared for high performance computation of
wall-bounded turbulent flows. The number of all-to-all communications is
decreased to only six instances by using a two-dimensional (pencil) domain
decomposition and utilizing the favourable scaling of the CFL time-step
constraint as compared to the diffusive time-step constraint. As the CFL
condition is more restrictive at high driving, implicit time integration of the
viscous terms in the wall-parallel directions is no longer required. This
avoids the communication of non-local information to a process for the
computation of implicit derivatives in these directions. We explain in detail
the numerical scheme used for the integration of the equations, and the
underlying parallelization. The code is shown to have very good strong and weak
scaling to at least 64K cores
Mixed insulating and conducting thermal boundary conditions in Rayleigh-B\'enard convection
A series of direct numerical simulations of Rayleigh-B\'enard convection, the
flow in a fluid layer heated from below and cooled from above, were conducted
to investigate the effect of mixed insulating and conducting boundary
conditions on convective flows. Rayleigh numbers between and
were considered, for Prandtl numbers and
. The bottom plate was divided into patterns of conducting and
insulating stripes. The size ratio between these stripes was fixed to unity and
the total number of stripes was varied. Global quantities such as the heat
transport and average bulk temperature and local quantities such as the
temperature just below the insulating boundary wall were investigated. For the
case with the top boundary divided into two halves, one conducting and one
insulating, the heat transfer was found to be approximately two thirds of the
fully conducting case. Increasing the pattern frequency increased the heat
transfer which asymptotically approached the fully conducting case, even if
only half of the surface is conducting. Fourier analysis of the temperature
field revealed that the imprinted pattern of the plates is diffused in the
thermal boundary layers, and cannot be detected in the bulk. With
conducting-insulating patterns on both plates, the trends previously described
were similar, however, the half-and-half division led to a heat transfer of
about a half of the fully conducting case instead of two-thirds. The effect of
the ratio of conducting and insulating areas was also analyzed, and it was
found that even for systems with a top plate with only conducting
surface, heat-transport of of the fully conducting case can be seen.
Changing the 1D stripe pattern to 2D checkerboard tessellations does not result
in a significantly different response of the system.Comment: Submitted to JF
Boundary layer dynamics at the transition between the classical and the ultimate regime of Taylor-Couette flow
Direct numerical simulations of turbulent Taylor-Couette flow are performed
up to inner cylinder Reynolds numbers of {Re_i=10^5} for a radius ratio of
{\eta=r_i/r_o=0.714} between the inner and outer cylinder. With increasing
{Re_i}, the flow undergoes transitions between three different regimes: (i) a
flow dominated by large coherent structures, (ii) an intermediate transitional
regime, and (iii) a flow with developed turbulence. In the first regime the
large--scale rolls completely drive the meridional flow while in the second one
the coherent structures recover only on average. The presence of a mean flow
allows for the coexistence of laminar and turbulent boundary layer dynamics. In
the third regime the mean flow effects fade away and the flow becomes dominated
by plumes. The effect of the local driving on the azimuthal and angular
velocity profiles is quantified, in particular we show when and where those
profiles develop.Comment: 22 pages, submitted to Po
Logarithmic mean temperature profiles and their connection to plume emissions in turbulent Rayleigh-B\'enard convection
Two-dimensional simulations of Rayleigh-B\'enard convection at show that vertical logarithmic mean temperature profiles can be
observed in regions of the boundary layer where thermal plumes are emitted. The
profile is logarithmic only in these regions and not in the rest of the
boundary layer where it is sheared by the large scale wind and impacted by
plumes. In addition, the logarithmic behavior is not visible in the horizontal
average. The findings reveal that the temperature profiles are strongly
connected to thermal plume emission and support a perception that parts of the
boundary layer can be turbulent, while others are not. The transition to the
ultimate regime, in which the boundary layers are considered to be fully
turbulent, can therefore be understood as a gradual increases in fraction of
the plume-emitting ('turbulent') regions of the boundary layer.Comment: 6 page
Geostrophic convective turbulence: The effect of boundary layers
Rayleigh--B\'enard (RB) convection, the flow in a fluid layer heated from
below and cooled from above, is used to analyze the transition to the
geostrophic regime of thermal convection. In the geostrophic regime, which is
of direct relevance to most geo- and astrophysical flows, the system is
strongly rotated while maintaining a sufficiently large thermal driving to
generate turbulence. We directly simulate the Navier--Stokes equations for two
values of the thermal forcing, i.e. and , a
constant Prandtl number~, and vary the Ekman number in the range
to which satisfies both requirements of
super-criticality and strong rotation. We focus on the differences between the
application of no-slip vs. stress-free boundary conditions on the horizontal
plates. The transition is found at roughly the same parameter values for both
boundary conditions, i.e. at~ for~ and at~ for~. However,
the transition is gradual and it does not exactly coincide in~ for
different flow indicators. In particular, we report the characteristics of the
transitions in the heat transfer scaling laws, the boundary-layer thicknesses,
the bulk/boundary-layer distribution of dissipations and the mean temperature
gradient in the bulk. The flow phenomenology in the geostrophic regime evolves
differently for no-slip and stress-free plates. For stress-free conditions the
formation of a large-scale barotropic vortex with associated inverse energy
cascade is apparent. For no-slip plates, a turbulent state without large-scale
coherent structures is found; the absence of large-scale structure formation is
reflected in the energy transfer in the sense that the inverse cascade, present
for stress-free boundary conditions, vanishes.Comment: Submitted to JF
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