Esrange Sweden Simulation - Winter Conditions

This page describes a numerical simulation of gravity waves due to wintertime winds blowing over the Scandinavian Mountain ranges in Norway and Sweden.

Computational Domain

The layout of the of the simulation is shown in the figure below. Note that the boundaries of the computation domain (shown by the thin white line) has been rotated by 26 degrees with respect to lines of constant latitude.
domain

Just the computational domain is shown in the figure below. In this plot, the surface has been interpolated to rectangular coordinates.

surface

The mesh is uniform at 500 m spacing from the Norwegian coastline to a point 50 km east-southeast of Esrange, Sweden. Gentle stretching is used upstream and downstream of these points. The mesh is also uniformly spaced at 500 m in the lateral direction over the central regon +/- 50 km N-NE and S-SW of Esrange. Gentle stretching is once again used from this region to the outer boundaries. The mesh is uniformly spaced at 250 m for all altitudes in the z direction. In total the mesh contains 650 x 274 x 576 points and sponge layers are used on all external boundaries in order to absorb outgoing waves.

Wind and Thermodynamic Profiles

The wind and temperature profiles were based on radiosonde mesurements taken over Nome Alaska on Jan 5 2017 at 12:00 UTC. The radiosonde measurements were smoothed somewhat and the data was extended between 30 and 113 km using climatology. Polynomial extrapolation was used above 113 km.

winds

magnitude

direction

direction

temperature

N_sq

N_sq

Initial Wind Condition

Here the winds are initially set to zero from the surface to an altitude of about 20 km. At this point the wind transitions to the profiles shown in the plots above. Forcing terms then gradually introduce winds near the surface with the objective of achieving the profile shown above within a two hour period. A hyperbolic tangent function is used in order to produce gentle acceleration of the wind near the beginning and end of the forcing period. The maximum forcing rate is equivalent to that of a linear ramp with a duration of 30 minutes.

Movies

Shortened animation of u' in the xz plane at the position y = 0 km






Shortened animation of vorticity magnitude in the xz plane at the position y = 0 km








Animation of u' in the xz plane at the position y = 0 km






Animation of w' in the xz plane at the position y = 0 km






Animation of potential temperature perturbation in the xz plane at the position y = 0 km






Animation of vorticity magnitude in the xz plane at the position y = 0 km






Animation of w' in the xy plane at an altitlde of 35 km






Animation of vorticity magnitude in the xy plane at an altitlde of 35 km overlayed on the computational domain






Animation of w' in the xy plane at an altitlde of 40 km






Animation of vorticity magnitude in the xy plane at an altitlde of 40 km overlayed on the computational domain






Animation of w' in the xy plane at an altitlde of 45 km






Animation of vorticity magnitude in the xy plane at an altitlde of 45 km overlayed on the computational domain






Animation of w' in the xy plane at an altitlde of 60 km






Animation of vorticity magnitude in the xy plane at an altitlde of 60 km overlayed on the computational domain






Animation of w' in the xy plane at an altitlde of 90 km






Animation of vorticity magnitude in the xy plane at an altitlde of 90 km overlayed on the computational domain






Animation of temperature fluxuation in the xy plane at an altitlde of 90 km