Authors

David C. Fritts, GATS, Inc.
Ronald B. Smith, Yale University
Michael J. Taylor, Utah State UniversityFollow
James D. Doyle, Naval Research Laboratory, Monterey, California
Stephen D. Eckermann, Naval Research Laboratory, Washington, DC
Andreas Dörnbrack, German Aerospace Center (DLR), Munich, Germany
Markus Rapp, German Aerospace Center (DLR), Munich, Germany
Bifford P. Williams, GATS, Inc.
Pierre-Dominique Pautet, Utah State UniversityFollow
Katrina Bossert, GATS, Inc.
Neal R. Criddle, Utah State UniversityFollow
Carolyn A. Reynolds, Naval Research Laboratory, Monterey, California
P. Alex Reineke, Naval Research Laboratory, Monterey, California
Michael Uddstrom, NIWA, Newmarket, Auckland, New Zealand
Michael J. Revell, NIWA, Newmarket, Auckland, New Zealand
Richard Turner, NIWA, Newmarket, Auckland, New Zealand
Bernd Kaifler, German Aerospace Center (DLR), Munich, Germany
Johannes S. Wagner, German Aerospace Center (DLR), Munich, Germany
Tyler Mixa, GATS, Inc.
Christopher G. Kruse, Yale University
Alison D. Nugent, Yale University
Campbell D. Watson, Yale University
Sonja Gisinger, German Aerospace Center (DLR), Munich, Germany
Steven M. Smith, Boston University
James J. Moore, Earth Observing Laboratory, National Center for Atmospheric Research, Boulder, Colorado
William O. Brown, Earth Observing Laboratory, National Center for Atmospheric Research, Boulder, Colorado
Julie A. Haggerty, Earth Observing Laboratory, National Center for Atmospheric Research, Boulder, Colorado
Alison Rockwell, Earth Observing Laboratory, National Center for Atmospheric Research, Boulder, Colorado
Gregory J. Stossmeister, Earth Observing Laboratory, National Center for Atmospheric Research, Boulder, Colorado
Et al. Et al.

Document Type

Article

Journal/Book Title/Conference

Bulletin of the American Meteorological Society

Volume

97

Issue

3

Publisher

American Meteorological Society

Publication Date

4-8-2016

First Page

425

Last Page

453

Abstract

The Deep Propagating Gravity Wave Experiment (DEEPWAVE) was designed to quantify gravity wave (GW) dynamics and effects from orographic and other sources to regions of dissipation at high altitudes. The core DEEPWAVE field phase took place from May through July 2014 using a comprehensive suite of airborne and ground-based instruments providing measurements from Earth’s surface to ∼100 km. Austral winter was chosen to observe deep GW propagation to high altitudes. DEEPWAVE was based on South Island, New Zealand, to provide access to the New Zealand and Tasmanian “hotspots” of GW activity and additional GW sources over the Southern Ocean and Tasman Sea. To observe GWs up to ∼100 km, DEEPWAVE utilized three new instruments built specifically for the National Science Foundation (NSF)/National Center for Atmospheric Research (NCAR) Gulfstream V (GV): a Rayleigh lidar, a sodium resonance lidar, and an advanced mesosphere temperature mapper. These measurements were supplemented by in situ probes, dropsondes, and a microwave temperature profiler on the GV and by in situ probes and a Doppler lidar aboard the German DLR Falcon. Extensive ground-based instrumentation and radiosondes were deployed on South Island, Tasmania, and Southern Ocean islands. Deep orographic GWs were a primary target but multiple flights also observed deep GWs arising from deep convection, jet streams, and frontal systems. Highlights include the following: 1) strong orographic GW forcing accompanying strong cross-mountain flows, 2) strong high-altitude responses even when orographic forcing was weak, 3) large-scale GWs at high altitudes arising from jet stream sources, and 4) significant flight-level energy fluxes and often very large momentum fluxes at high altitudes.

Comments

Publisher: http://journals.ametsoc.org/doi/pdf/10.1175/BAMS-D-14-00269.1

Share

COinS