@@ -18,20 +18,19 @@ again, 16 processors are needed, etc. However, in the altitude/radial direction,
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the number of points that are specified in the aether.json is unchanged, as it
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does not rely on the number of processors used.
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- - [ Grids in Aether] ( #grids-in-aether )
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- - [ Grid Types Explained] ( #grid-types-explained )
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- - [ Grid Shapes Explained] ( #grid-shapes-explained )
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- - [ TL;DR] ( #tldr )
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- - [ The Sphere Grid] ( #the-sphere-grid )
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- - [ The Cubesphere Grid] ( #the-cubesphere-grid )
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- - [ The Dipole Grid] ( #the-dipole-grid )
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- - [ Root Nodes] ( #root-nodes )
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- - [ Sphere] ( #sphere )
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- - [ Cubesphere] ( #cubesphere )
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- - [ Specifying Root Nodes] ( #specifying-root-nodes )
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- - [ Specifying the Grid] ( #specifying-the-grid )
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- - [ Horizontal Resolution] ( #horizontal-resolution )
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- - [ Vertical Resolution] ( #vertical-resolution )
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+ - [ Grid Types Explained] ( #grid-types-explained )
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+ - [ Grid Shapes Explained] ( #grid-shapes-explained )
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+ - [ TL;DR] ( #tldr )
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+ - [ The Sphere Grid] ( #the-sphere-grid )
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+ - [ The Cubesphere Grid] ( #the-cubesphere-grid )
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+ - [ The Dipole Grid] ( #the-dipole-grid )
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+ - [ Root Nodes] ( #root-nodes )
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+ - [ Sphere] ( #sphere )
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+ - [ Cubesphere] ( #cubesphere )
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+ - [ Specifying Root Nodes] ( #specifying-root-nodes )
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+ - [ Specifying the Grid] ( #specifying-the-grid )
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+ - [ Horizontal Resolution] ( #horizontal-resolution )
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+ - [ Vertical Resolution] ( #vertical-resolution )
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## Grid Types Explained
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@@ -115,24 +114,24 @@ bottom of the field-line. Each fieldline starts at the lowest modeled altitude
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and curves towards the equator. In the northern hemisphere, this means that the
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fieldlines curve south, while in the southern hemisphere they curve north.
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- The latitudinal spacing is such that there is a dependence on the L-shell (i.e.,
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- the equatorial radial extent of the field-line). Along the ` k ` dimension,
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- field-lines either terminate when they reach the equatorial plane, forming half
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- of a full field-line, or they terminate at the highest point specified in the
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- aether.json file, forming an open field line. Any grid point with an L-shell
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- less than the peak altitude will terminate in the equatorial plane, while any
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- field-line that has an L-shell above the peak altitude will simply terminate.
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- Field-lines that terminate in the equatorial plane have corresponding
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- field-lines in the other hemisphere, so ghostcells are used to pass information
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- back and forth. Field-lines that terminate at the maximum altitude have
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- vertical boundary conditions set in the ghost cells.
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-
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- The transition from the "closed" field-line region to the "open" field-line
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- region is a natural break point in the grid. The transition between these
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- regions can be handled with ghostcells in the "latitudinal" direction.
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- Therefore it makes the most sense to have have 4 distinct regions in "latitude":
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- south open, south closed, north closed, north open. The message passing is
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- treated differently at the boundaries between each of these regions .
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+ The latitudinal spacing is determined by the ` LatStretch ` factor in the settings.
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+ The base latitudes are then scaled in such a way that ** higher ** ` LatStretch ` leads to
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+ more points near the equator, 1.0 is roughly linear, and then values less than 1.0 will
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+ distribute more points near the poles. The exact spacing is calculated where the
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+ difference between successive values is proportional to:
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+ ` cos(lat_max)^(1/LatStretch) ` . Using an even number of latitudes is required.
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+
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+ Along the ` k ` dimension, field lines terminate after a specified number of points.
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+ When using the Dipole grid option, there is not an option to set the maximum altitude.
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+ Rather, points are laid down from the pole towards the equator, stopping when the field
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+ line reaches the equator. Ghost cells are then used to pass information across the
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+ equator. The spacing of points along each field line is the same as
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+ [ (Huba, Joyce & Fedder, 2000) ] ( https://doi.org/10.1029/2000JA000035 ) .
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+ Using an even number of points along the ` k ` dimension ( ` nAlts ` ) means that no points
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+ will lie on the magnetic equator and thus the field lines from the high latitude
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+ regions will not reach beyond the plasmasphere. See
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+ [ the dipole script in edu/examples ] ( ../../edu/examples/Dipole/dipole.py ) to
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+ experiment with the available options .
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### Root Nodes
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