MULTICELL SQUALL-LINE STRUCTURE AS A MANIFESTATION OF VERTICALLY TRAPPED GRAVITY-WAVES

Authors
Citation
Mj. Yang et Ra. Houze, MULTICELL SQUALL-LINE STRUCTURE AS A MANIFESTATION OF VERTICALLY TRAPPED GRAVITY-WAVES, Monthly weather review, 123(3), 1995, pp. 641-661
Citations number
50
Categorie Soggetti
Metereology & Atmospheric Sciences
Journal title
ISSN journal
00270644
Volume
123
Issue
3
Year of publication
1995
Pages
641 - 661
Database
ISI
SICI code
0027-0644(1995)123:3<641:MSSAAM>2.0.ZU;2-0
Abstract
Two-dimensional and three-dimensional simulations of a midlatitude squ all fine with a high-resolution nonhydrostatic model suggest that the multicellular structure of the storm may be associated with gravity wa ves generated by convection. Time-lapse display of model output demons trates that the commonly described ''cutoff'' process is actually a gr avity wave phenomenon. The convective cells arise as gravity waves, wh ich are forced by continuous strong low-level convergence at the storm 's gust front. The waves propagate to both sides of the gust front. Th e stronger westward (front to rear) mode dominates at the mature stage of the squall line. Continuous low-level updraft is generated at the nose of the cold pool, which propagates at the speed of a density curr ent. Updraft cells periodically break away from this persistent low-le vel gust-front updraft and move at phase speeds of their associated gr avity waves, not at the surrounding airflow speeds as implied by the t raditional multicell model. Linear theory shows that the multicellular structure is associated with vertically trapped gravity waves in the troposphere. The waves become trapped in the mid- to upper troposphere because of the strong decrease of Scorer parameter with height as a r esult of strong vertical wind shear and the reduced static stability a loft. Waves are trapped in lower Levels because of the rigid ground. T he basic characteristics of these trapped tropospheric gravity waves a re wavelengths of 16-20 km, storm-relative phase speeds of 20-25 m s(- 1), and periods of 11-17 min, which are consistent with the generation periods of precipitation cells at the mature stage in the leading por tion of the storm. In the trailing stratiform region, these tropospher ic gravity waves become more diffuse with weaker amplitudes, and their wavelengths become longer (25-35 lan) with greater storm-relative pha se speeds (30-40 m s(-1)), as described by the dispersion relationship of internal gravity waves. The tropospheric gravity waves differ from disturbances above the tropopause. which are mechanically forced by c onvective cells impinging on the tropopause. These waves in the lower stratosphere have the structure of vertically propagating (rather than trapped) gravity waves.