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Advanced multi-purpose numerical
models (top)
Anelastic model for geophysical flows: dynamic grid deformation
Joseph Prusa (Iowa State University) and Smolarkiewicz
continued the development of an adaptive grid-refinement
approach, embedded in the framework of a nonhydrostatic anelastic
model, for simulating a broad range of geophysical flows using
Eulerian/semi-Lagrangian nonoscillatory forward-in-time (NFT)
numerical methods. The key prerequisite of the adaptive grid
is a continuous time-dependent curvilinear-coordinate remapping
that enables mesh refinement indirectly, via dynamic change
of the metric coefficients, while retaining advantages of
Cartesian mesh calculations (speed, low memory requirements,
and accuracy), conducted fully in the computational domain.
The focus of the past year has been an advective grid adaptation
technique. Compared to more traditional elliptic grid generators,
the advective approach proposed is faster and more straightforward
in its implementation for time dependent grids. These properties
follow from the use of MPDATA to integrate a posited, prognostic
equation for grid increments. Also, the NFT properties of
MPDATA mimicked nested grids by propagating step changes in
grid resolution. Test results that simulate a traveling stratospheric
inertio-gravity wave packet (Movie 4) demonstrate the potential
and the efficacy of the approach for tracing targeted flow
features, and dynamically adjusting to prescribed undulations
of model boundaries.

Use links at right to see a larger sized version of
this movie.
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To view
the movie, place mouse over image. Alternately, for
slower connections, you may use the links below to download
the movie.
Gravity
wave movie
(animated GIF)
Gravity
wave movie
(AVI format)
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| Movie 4. Traveling
gravity-wave packet. Left panel shows contours of vertical
velocity, with 1000 km region of high grid resolution
only in immediate neighborhood of the traveling disturbance.
Right panel shows normalized grid stretching factor (solid
line) and physical coordinate (dashed line) as a function
of normalized transformed coordinate. |
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A nonhydrostatic NFT model for oceanic research
Smolarkiewicz, Frank Bryan
(NCAR/CGD), and Matthew Hecht (Los Alamos National Laboratory)
developed a nonoscillatory forward-in-time (NFT) nonhydrostatic
model for simulating a broad range of oceanic circulations.
The model employs the Boussinesq approximation and linearized
constitutive equation for seawater. These two assumptions,
common in the simulation of oceanic flows, facilitated the
design of a fully second-order-accurate NFT numerics with
implicit treatment of internal gravity waves. The latter enhances
the computational stability and accuracy of the model. Since
the model has been cloned from the all-scale atmospheric model
EULAG, it inherits all the benefits of the NFT approach, and
most of the technical advancements, including: accurate representation
of rapidly-rotating strongly-stratified flows past complex
bathymetry, explicit/implicit turbulence modeling, optionality
of the semi-Lagrangian (trajectory wise) and Eulerian (control-volume
wise) transport schemes, mesh refinement capability via deformable
coordinates, and high-performance computer programming. Smolarkiewicz,
and a Naval Research Laboratory (NRL) team lead by Alex Warn-Varnass,
have collaborated on research projects which demonstrate the
efficacy of the model, including: the western-boundary-current
separation (DNS scenario mimicking laboratory experiments,
Movie 5 and the evolution of coastal solitons (LES of mesoscale
circulations in the Messina Straits.
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To view the movie, place mouse over image. Alternately,
for slower connections, you may use the links below
to download the movie.
Dye
tracer movie
(animated GIF)
Dye
tracer movie
(AVI format)
Dye
tracer movie
(MPEG format)
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| Movie 5. Animation
of the simulated flow of a dye tracer, injected into the
rotating, flat-bottomed domain along with inflowing water
at the bottom left and flowing out at the upper right.
Frames are separated in time by about 3 seconds, with
the total length of the simulation spanning about 5 minutes. |
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Upper boundary conditions for nonhydrostatic
models
Nils Wedi of the European Center for Medium Range Weather
Forecasts (ECMWF) and Smolarkiewicz
continued development of a novel class of upper boundary conditions
for nonhydrostatic models of atmospheres and oceans. Typically,
nonhydrostatic atmospheric models attempt to mimic an infinite
atmosphere, whereas nonhydrostatic oceanic models incorporate
rigid-lid approximation. Either condition assumes simplistic
mathematical representation of the true conditions, and over-constrains
admissible atmospheric/oceanic circulations. Wedi and Smolarkiewicz
relaxed the standard assumptions to allow for undulating smooth
material boundaries, an approximation that is sound in the
long-wave limit. The key technical prerequisite of their development
is the extension of the classical terrain-following coordinate
transformation of Gal-Chen and Somerville (1975) onto time-dependent
curvilinear upper boundaries, and its efficient numerical
coding in a generic Eulerian/semi-Lagrangian NFT nonhydrostatic
model format. A series of simulations with the finite-amplitude
undulations of the upper boundary predicted from the shallow-water
equations - a physical scenario relevant to ocean models (see
Movie 6) - and the validation against corresponding simulations
of ''real shallow water'' (incompressible non-Boussinesq fluid
with a 1/1000 density jump) clearly demonstrate the utility
of the approach.
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|
To view
the movie, place mouse over image. Alternately, for
slower connections, you may use the links below to download
the movie.
Simulated
flow movie
(animated GIF)
Simulated
flow movie
(AVI format)
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| Movie 6. Simulated
flow (contours of vertical velocity) of a homogeneous
nonhydrostatic Boussinesq fluid with the free-surface
upper boundary conditions. The height of the surface is
predicted by integrating shallow-water equations, and
it is incorporated into a nonhydrostatic model via time-dependent
curvilinear coordinate transformation. |
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Spectral preconditioners for nonhydrostatic
atmospheric models
The elliptic problems in semi-implicit nonhydrostatic atmospheric
models are difficult. Typically, they are poorly conditioned,
nonseparable, contain cross derivative terms, and often are
nonsymmetric. Collaboration between NCAR researchers Steven
Thomas (NCAR/SCD), Joshua Hacker,
Smolarkiewicz, and Roland
Stull (University of British Columbia) has led to a class
of effective Krylov methods - a conjugate residual (GCR) algorithm
preconditioned with a 3D direct solver (using standard tridiagonal
inversion in the vertical). They have developed a horizontal
spectral preconditioner as an alternative to a more standard,
and simpler, line-Jacobi relaxation scheme. However, the efficacy
of the spectral preconditioner requires neglecting the cross
derivative terms, and homogenization (e.g., averaging) metric
coefficients over the computational domain. Because such a
compromise causes a substantial departure of the preconditioner
from the original elliptic operator, it is not obvious whether
it leads to a competitive solver a priori. They evaluated
the robustness of the proposed approach over a broad range
of representative meteorological applications (see Movie 7)
and they documented its superior performance in the context
of a three-time-level, semi-implicit, semi-Lagrangian, all-scale
weather-prediction/research model.
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|
To view
the movie, place mouse over image. Alternately, for
slower connections, you may use the links below to download
the movie.
Isotherms movie
(animated GIF)
Isotherms movie
(AVI format)
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| Movie
7. Isotherms of a 3D convective thermal. The loop
covers 450 s in 30 s intervals. GCR solver performance
with both the DCT and line Jacobi preconditioners are
shown as running totals of iterations and CPU seconds.
The contour interval is 0.1 K. |
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Correction algorithms for Vaisala radiosondes
Vaisala radiosonde relative humidity measurements are known
to be inaccurate at cold temperatures in the upper troposphere,
yet these measurements are fundamentally important to a wide
range of research activities, including: initializing numerical
models or evaluating model results; performing radiative transfer
calculations; validating ground-based or satellite water vapor
retrievals; and developing water vapor and cloud parameterizations.
Larry Miloshevich developed
a numerical inversion algorithm to correct for the time-lag
error that results from slow sensor response at cold temperatures,
based on laboratory measurements of the temperature-dependence
of the sensor time-constant. Miloshevich applied a correction
algorithm for time-lag known bias errors to a dataset of 40
humidity profiles, measured simultaneously by Vaisala radiosondes
and the reference-quality NOAA/Climate Monitoring Diagnostics
Library cryogenic hygrometer (Fig. 32), demonstrating that
the corrections largely remove the temperature-dependent dry
bias, and reduce the variability. The example corrected humidity
profile in Figure 33 (red) shows that the time-lag correction
recovers vertical structure in the profile at cold temperatures,
showing what appears to be a tropopause cirrus layer, approximately
1 km thick, that is undetectable in the original measurements
(blue).
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| Figure 32. Statistical analysis
of 40 Vaisala RS80-H humidity profiles as compared to
simultaneous measurements by the reference-quality NOAA/CMDL
cryogenic hygrometer. The mean and standard deviation
(red curves) of the difference between the hygrometer
measurements and the corresponding uncorrected (left)
or corrected (right) radiosonde measurements are shown
in %RH as a function of temperature. |
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| Figure 33. Vaisala
RS80-H humidity sounding after correction for sensor time-lag
error and known bias errors (red), showing a probable
tropopause cirrus layer that is not readily apparent in
the original data (blue). The dashed curve is ice-saturation,
and an asterisk indicates the tropopause. |
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