Downslope Winds Along the Wasatch Front

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Downslope Winds Along the Wasatch Front Lacey Holland

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Downslope Winds Along the Wasatch Front. Lacey Holland. Outline. Objectives A Climatology of Downslope Events at Hill AFB (HIF) Synoptic Overview of 7 Oct 2000 Mesoscale Overview Valley flows Tethersonde and lidar data ADAS analyses. Objectives. - PowerPoint PPT Presentation

Transcript of Downslope Winds Along the Wasatch Front

Page 1: Downslope Winds Along the Wasatch Front

Downslope Winds Along the Wasatch Front

Lacey Holland

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Outline

• Objectives• A Climatology of Downslope Events at Hill AFB

(HIF)• Synoptic Overview of 7 Oct 2000• Mesoscale Overview• Valley flows• Tethersonde and lidar data• ADAS analyses

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Objectives

• To what extent are strong winds on the east benches due to “canyon winds”?

• To what extent are the strong winds on the east benches due to cold air flowing down and across the slope (i.e. bora winds)?

• Why are the strongest winds confined to near the base of the Wasatch?

• Why do the windstorms occur further away from the base of the mountains so infrequently?

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Areas affected by Wasatch downslope windstorms

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Conditions favorable for downslope windstorms along the Wasatch Front

• Strong cross-barrier flow at crest-level (700 mb closed low to SSW)

• Pool of cold air to the ENE (relatively high pressure over Wyoming)

• Wind reversal above crest-level (presence of a critical level) and elevated stable layer

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Synoptic conditions favorable for downslope windstorms

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A Composite of Downslope Wind Events at HIF

• Most stations in valley of limited use– Records too short– Not in proximity of affected areas

• Top 0.5% events used to create composite

• NCEP Reanalysis

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Top 10 Downslope Windstorms at HIF (1949-1999)

• 4 Apr 1983 (46 m/s)• 16 May 1952 (42 m/s)• 20 Feb 1971 (38 m/s)• 22 Oct 1953 (38 m/s)• 18 Mar 1961 (37 m/s)

• 3 June 1949 (35 m/s)• 11 Nov 1978 (35 m/s)• 6 May 1949 (34 m/s)• 16 Nov 1964 (34 m/s)• 26 Jan 1957 (33 m/s)

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Wasatch Downslope Windstorms by Month

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A Composite of 700 mb Heights in strongest downslope events

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Vertical Transport and Mixing eXperiment (VTMX) IOP#2,

6-7 October 2000

• IOP#2: 2200 UTC 6 Oct – 1600 UTC 7 Oct

• Tethered balloon at Mt. Olivet Cemetery lost from its tether in strong winds

• URBAN2000 scientists report tracers stagnating downtown

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Synoptic OverviewRUC2 500 mb heights RUC2 700 mb heights

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Mesoscale Overview

2300 UTC 6 October 2000

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Chronology• Prior to 0700 UTC: Developing Stage

– progression of cold air across Wyoming

– drainage circulations in Salt Lake Valley (SLV)

• 0700 -1000 UTC: Initial development

– Initial penetration of cold air across Wasatch

– Gap flows through Parley’s Canyon

– Lidar

• After 1000 UTC- Downslope wind event into SLV

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Conceptual model of 7 Oct 2000 (0400 UTC)

SLCACS

VTMX9

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Cross-section Across Wyoming

EVW RKSRWL

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Surface plot

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Salt Lake Valley Flows

U42

WBB UT5

VPN10

VTMX9

VTMX6

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ASU Tethersondes

• Located at Mt. Olivet Cemetery• 3 sondes on one balloon• Each sonde separated by 50 m• Highest sonde 10 m below

balloon

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Sonde #2

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Tethersondes at 0400 UTC

__ = WF

__ = T2

__ = T3

__ = T4

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NOAA ETL Lidar

• Located at U42 (SLC Airport #2)

• Traverse Excitation Atmospheric pressure CO2 (TEACO2) lidar

• 10.6 m wavelength

• Detection range: 1-30 km

• Radial velocity accuracy: 0.3-1 ms-1

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lidar

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Description of ADAS Analyses

• Rawinsonde (PNL,NCAR,NWS), tethersonde (ASU), and surface station (PNL, Mesowest) data ingested into analyses

• 1 km resolution

• Adjustment made to analysis for dense data

• Further adjustments to be made

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Adas evening

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Conceptual Model at 0700 UTC

SLCACS

VTMX9

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sfc

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Tethersondes at 0530 UTC

__ = WF

__ = T2

__ = T3

__ = T4

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Conceptual Model at 0830 UTC

SLCACS

VTMX9

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SLC Special Sounding 0900 UTC

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Tethersondes at 1000 UTC

__ = WF

__ = T2

__ = T3

__ = T4

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Conceptual Model at 1030 UTC

SLC ACS

VTMX9

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Lidar ObservationsLidar graphics courtesy of Lisa Darby, NOAA ETL

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ADAS Analyses

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Summary• To what extent are strong winds on the east

benches due to “canyon winds”? – Lidar indicates jet out of canyon (gap flow) but spatial

extent is larger than simply the canyon opening ; Direction of flow out of the canyon determined by larger-scale flow

• To what extent are the strong winds on the east benches due to cold air flowing down and across the slope (i.e. bora winds)?– 7 Oct 2000 (and other times) are primarily bora events;

radiational inversions can erode and warm the surface, however.

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Summary (con’t)• Why do the windstorms occur further

away from the base of the mtns so infrequently?– East benches can stop mechanical penetration

of cold air into surface inversion in the valley– Radiatively cooled air in the valley is often

cooler than air crossing the barrier

• Why are the strongest winds confined to near the base of the Wasatch?– Need a mechanism to penetrate or to erode the

surface inversion

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Acknowledgments

• John Horel

• My committee (S. Lazarus, E. Zipser)

• Those who have contributed data (Sradik - ASU, Coulter - PNL, Darby - ETL)

• Many unnamed others who have provided support, help, and motivation

THANKS!