26 September Start/Stop Times

 

Flight 1

 

Start                Stop                Maneuver

15:12:11         15:20:48         A to B; Descent to 500’

15:20:48         15:38:43         B to C; 500’

15:38:53         15:51:05         C to E’; 500’

15:53:53         16:05:31         E’ to C; 3K’

16:07:14         16:21:39         C to E’; 1.5K’

16:23:49         16:39:20         E’ to C; 1K’

16:40:45         16:48:30         C to F’; 500’

16:49:24         17:22:18         F’ to G’; 500’

17:23:18         17:33:15         G’ to C; 500’

17:34:19         17:54:27         C to D’; 500’

17:54:27         17:56:37         D’ to D, Ascent to 4K’

 

Flight 2

 

Start                Stop                Maneuver

21:02:46         21:06:23         D” to D’; Descent 7K’ to 500’

21:06:23         21:35:31         D’ to C; 500’

21:35:31         21:42:42         C; Spiral Ascent to 7 K’

21:44:10         21:48:00         C; Descent to 3K’

21:48:51         22:04:50         C to E’, 3K’

22:08:04         22:19:08         E’ to C, 1K’

22:21:48         22:37:30         C to E’; 1.5K’

22:39:54         22:52:34         E’ to C; 500’

22:53:58         23:26:55         C to B’; 500’

23:26:55         23:37:59         B’ to A, 500’

23:37:59         23:48:39         A; Ascent to 11K’

 

Initial Impressions: Barrier effects seem more prominent on the 1st flight.  Clear enhancement of the alongshore flow, and more of an offshore component proximal to the higher terrain inland of Cape Fairweather.  This enhancement extended barely up to 3K’.  The second flight indicated less of a barrier jet along the coast. Modest increases in v and decreases in u were found near the coast in the 500’ leg and weakly in the 1000’ just near point C.  But the terrain effects here may have been at least a bit obscured by the mesoscale variability.  The 3K’ leg from C to E’ indicated somewhat stronger southerlies offshore, presumably unrelated to terrain effects.  If this level reflects the overall low-level pressure gradients due to the storm itself, the effect of the terrain on the flow at 500’ is greater than it might first appear.  A quick glance at the thermodynamics suggests that it was slightly statically stable at low-levels at least in terms of the vertical gradient in thetae.