500 1000 1500 2000 2500 3000 3500 Figure 1. 30-sec mean topography (m, shaded following scale at upper left) of the Intermountain West and adjoining regions,

Slides:



Advertisements
Similar presentations
Generation mechanism of strong winds in the left-rear quadrant of Typhoon MA-ON (2004) during its passage over the southern Kanto district, eastern Japan.
Advertisements

Chapter 6 Section 6.4 Goals: Look at vertical distribution of geostrophic wind. Identify thermal advection, and backing and veering winds. Look at an example.
Cold Fronts and their relationship to density currents: A case study and idealised modelling experiments Victoria Sinclair University of HelsinkI David.
Dynamical similarities and differences between cold fronts and density currents Victoria Sinclair University of Helsinki
By Megan and Slade. A topographic map is a map that shoes the surface features, or topography, of the Earth. Topographic maps show both natural features,
Analysis of Precipitation Distributions Associated with Two Cool-Season Cutoff Cyclones Melissa Payer, Lance F. Bosart, Daniel Keyser Department of Atmospheric.
An Overview of Environmental Conditions and Forecast Implications of the 3 May 1999 Tornado Outbreak Richard L. Thompson and Roger Edwards Presentation.
A WRF Simulation of the Genesis of Tropical Storm Eugene (2005) Associated With the ITCZ Breakdowns The UMD/NASA-GSFC Users' and Developers' Workshop,
Assimilating Sounding, Surface and Profiler Observations with a WRF-based EnKF for An MCV Case during BAMEX Zhiyong Meng & Fuqing Zhang Texas A&M University.
The Effect of the Terrain on Monsoon Convection in the Himalayan Region Socorro Medina 1, Robert Houze 1, Anil Kumar 2,3 and Dev Niyogi 3 Conference on.
The Effect of the Terrain on Monsoon Convection in the Himalayan Region Socorro Medina 1, Robert Houze 1, Anil Kumar 2,3 and Dev Niyogi 3 Cloud and Precipitation.
A M ULTISCALE A NALYSIS OF A H EAVY R AINFALL E VENT OVER L AKE M ICHIGAN Jason M. Cordeira D EPARTMENT OF A TMOSPHERIC AND E NVIRONMENTAL S CIENCES U.
Extreme Convection Near the Himalayas and Andes Gerald R. North Symposium, Texas A&M University, College Station, June 8, 2009 Robert A. Houze, Jr. Ulrike.
The effect of terrain and land surface on summer monsoon convection in the Himalayan region Socorro Medina, Robert Houze, Anil Kumar, and Dev Niyogi 13.
Hector simulation We found simulation largely depending on: Model initialization scheme Lateral boundary conditions Physical processes represented in the.
Figure 1. Topography (m, shaded following inset scale) of the Intermountain West and adjoining region
Some Preliminary Modeling Results on the Upper-Level Outflow of Hurricane Sandy (2012) JungHoon Shin and Da-Lin Zhang Department of Atmospheric & Oceanic.
 Z NO x Snow Cover VOCs O3O3 Fig. 1.1 Simplified schematic of typical situation leading to high ozone concentrations. Red line represent potential temperature.
A case book of the Double Trouble State Park Wildfire (2002) Joseph J. Charney USDA Forest Service, Northern Research Station, East Lansing, MI Daniel.
Multiscale Analyses of Tropical Cyclone-Midlatitude Jet Interactions: Camille (1969) and Danny (1997) Matthew S. Potter, Lance F. Bosart, and Daniel Keyser.
The National Environmental Agency of Georgia L. Megrelidze, N. Kutaladze, Kh. Kokosadze NWP Local Area Models’ Failure in Simulation of Eastern Invasion.
Prof. George Tai-Jen Chen Department of Atmospheric Sciences National Taiwan University ( May, 10, 2007 Beijing ) A case study of subtropical frontogenesis.
Fig. 1.1: Simplified schematic of typical situation leading to high wintertime ozone concentrations. Red line represent potential temperature profile with.
ADVENTURE IN SYNOPTIC DYNAMICS HISTORY
13th Cyclone Workshop 25 October 2005 Pacific Grove, CA1 A Study of the Effect of Horizontal Contrasts in Static Stability on Frontal Behavior Mark T.
The Linear and Non-linear Evolution Mechanism of Mesoscale Vortex Disturbances in Winter Over Western Japan Sea Yasumitsu MAEJIMA and Keita IGA (Ocean.
P1.7 The Real-Time Mesoscale Analysis (RTMA) An operational objective surface analysis for the continental United States at 5-km resolution developed by.
Meteo 1 Activity 6 Weather Map Activity
Dual-Aircraft Investigation of the inner Core of Hurricane Norbert. Part Ⅲ : Water Budget Gamache, J. F., R. A. Houze, Jr., and F. D. Marks, Jr., 1993:
Mesoscale Simulation of a Convective Frontal Passage Travis Swaggerty, Dorothea Ivanova and Melanie Wetzel Department of Applied Aviation Sciences Embry-Riddle.
Tropical Transition in the Eastern North Pacific: Sensitivity to Microphysics Alicia M. Bentley ATM May 2012.
Research on the HWRF Model: Intensification and Uncertainties in Model Physics Research on the HWRF Model: Intensification and Uncertainties in Model Physics.
Validation of the Simulated Microphysical Structure within the Midlevel Inflow Region of a Tropical, Oceanic Squall Line Hannah C. Barnes, Robert A. Houze.
Meng, Z., F. Zhang, P. Markoswki, D. Wu, and K. Zhao, 2012: A modeling study on the development of a bowing structure and associated rear inflow within.
Figure 1. Map of study area. Heavy solid polygon defines “Cascade Mountains” for the purposes of this study. The thin solid line divides the Cascade Mountains.
Figure 1. Schematic of factors contributing to high ozone concentrations. Potential temperature profile (red line) with stable layer trapping ozone precursors.
Acceleration of high winds in idealised simulations of extratropical cyclones. Tim P. Slater Prof. David M. Schultz Prof. Geraint Vaughan 3 Jan 2012 UTC.
Fig Decadal averages of the seasonal and annual mean anomalies for (a) temperature at Faraday/Vernadsky, (b) temperature at Marambio, and (c) SAM.
Ship-board Flux Measurements made during CalNex 2010 C.W. Fairall, D.E. Wolfe, S. Pezoa, L. Bariteau, B. Blomquist, C. Sweeney Air-Sea flux measurements.
Numerical Simulation and Prediction of Supercell Tornadoes Ming Xue School of Meteorology and Center for Analysis and Prediction of Storms University of.
Unit 2 Measuring the Earth Mapping. Size and Shape Almost a perfect sphere- slight flattening in the polar regions and a slight bulging at the equatorial.
A Subtropical Cyclonic Gyre of Midlatitude Origin John Molinari and David Vollaro.
An Investigation of Model-Simulated Band Placement and Evolution in the 25 December 2002 Northeast U.S. Banded Snowstorm David Novak NOAA/ NWS Eastern.
Cheng-Zhong Zhang and Hiroshi Uyeda Hydroshperic Atmospheric Research Center, Nagoya University 1 November 2006 in Boulder, Colorado Possible Mechanism.
Topographic & Geologic Maps Plus: Latitude and Longitude!
Forces and accelerations in a fluid: (a) acceleration, (b) advection, (c) pressure gradient force, (d) gravity, and (e) acceleration associated with viscosity.
Forecast Pressure. Pressure Observations ASOS is the best…the gold standard Ships generally the worst.
X 10 km Model Bathymetry (A)Temperature (B) Alongshore Velocity Cross-shore Velocity Figure 1: Panel (A) model grid and bathymetry. The model has closed.
Meteorología sinóptica Lección 05 Un ejemplo de análisis sinóptico aplicado a un estudio de caso.
Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. Spectral response functions (SRF) for the ABI IR bands (blue curves with band numbers.
Implementation of Terrain Resolving Capability for The Variational Doppler Radar Analysis System (VDRAS) Tai, Sheng-Lun 1, Yu-Chieng Liou 1,3, Juanzhen.
Figure 1. NASA Blue Marble (i.e., true color) image of (a) the Intermountain West and (b) the Wasatch Front and adjoining region. Geographic features discussed.
(a)(b) (c)(d) FIG. 1. Climatological precipitation (color, mm day -1 ) and SST (contour interval is 2 o C with 10 o C and 20 o C thickened) in June (left)
Heavy Rain Climatology of Upper Michigan Jonathan Banitt National Weather Service Marquette MI.
Matt Vaughan Class Project ATM 621
Model Simulations of Extreme Orographic Precipitation in the Sierra Nevada during the New Year's Holiday Flood of Phillip J. Marzette, Michael.
Mapping.
SO254 Extratropical cyclones
Daniel M. Alrick 14th Cyclone Workshop Monday, September 22, 2008
Low level Jet.
Water Budget of Typhoon Nari(2001)
The May 24 Shamrock cold front
Cold Frontal Zone N E Reproduced from Synoptic-Dynamic Meteorology in Midlatitudes, Vol. II.
Upper air Meteorological charts
Nonlinear modulation of O3 and CO induced by mountain waves in the UTLS region during TREX Mohamed Moustaoui(1), Alex Mahalov(1), Hector Teitelbaum(2)
Figure11.2 Air mass source regions and their paths.
Daniel M. Alrick 14th Cyclone Workshop Monday, September 22, 2008
Guy Dagan, Ilan Koren, Orit Altaratz, Yoav Lehahn  iScience 
FIGURE 6.7 The top diagram (a) shows four cities (A, B, C, and D) at varying elevations above sea level, all with different station pressures. The middle.
Scott A. Braun, 2002: Mon. Wea. Rev.,130,
Presentation transcript:

Figure sec mean topography (m, shaded following scale at upper left) of the Intermountain West and adjoining regions, with the height of Sierra Nevada crest between points N and S at lower left (position of Lake Tahoe indicated by vertical line). Abbreviations used for Lake Tahoe (LT) and the lower Colorado River Basin (LCRB) Sierra Nevada Cascade Mountains N S Elevation (m) N LT S LT High Sierra Intermountain West Nevada Utah Idaho Oregon California Arizona Pacific Ocean LCRB High Sierra

L SFC: 0000 UTC 26 Mar UTC 26 Mar L L SFC: 1200 UTC 25 Mar hPa: 1200 UTC 25 Mar Figure 2. Synoptic structure of the 25 Mar 2006 cold front at 1200 UTC 25 Mar (left panels) and 0000 UTC 26 Mar 2006 (right panels). Manual surface analyses (top) include conventional frontal symbols, sea level contours (every 2 hPa), and surface wind observations (full and half barb denote 5 and 2.5 m s -1, respectively). NAM 700- hPa analyses (bottom) include temperature contours (every 2°C), wind (full and half barb denote 5 and 2.5 m s -1, respectively), and 800–500-mb mean relative humidity (shaded following scale at lower left). Adapted from Steenburgh et al. (2009).

a) FULLTER b) NOSIERRA Figure 3. WRF topography [m, shaded following scale in (a)] for a subset of the (a) FULLTER and (b) NOSIERRA 12-km nested domain.

Figure 4. WRF-model analyses for 1500 UTC 25 Mar (a) FULLTER radar reflectivity [dBZ, color shaded according to scale in (a)], cloud-top temperature (°C, grey shaded according to scale in (b)], and 850-hPa geopotential height (solid contours every 10 m). (b) Same as (a) but for NOSIERRA. (c) FULLTER lowest half-η level potential temperature (every 2 K), wind (vector scale at left), and kinematic frontogenesis [K (100 km h) −1, shaded following scale at left]. (d) Same as (c), but for NOSIERRA. (e) Same as (c), but with diabatic frontogenesis. (f) As in (e) but for NOSIERRA. c) FULLTER Kinematic (F w ) 1500 UTC e) FULLTER Diabatic (F D ) 1500 UTC d) NOSIERRA Kinematic (F w ) 1500 UTC f) NOSIERRA Diabatic (F D ) 1500 UTC ms a) FULLTER Cloud/Radar 1500 UTC b) NOSIERRA Cloud/Radar 1500 UTC X Y X Y

a) FULLTER-NOSIERRA 1500 UTC c) FULLTER-NOSIERRA 2100 UTC b) FULLTER-NOSIERRA 1800 UTC d) FULLTER-NOSIERRA 0000 UTC ms Figure 5. FULLTER lowest half-η level potential temperature (every 2 K), FULLTER- NOSIERRA lowest half-η level potential temperature difference [K, shaded according to scale in (a)], and FULLTER-NOSIERRA lowest half-η level vector wind difference [scale in (a)] at (a) 1500 UTC 25 Mar, (b) 1800 UTC 25 Mar, (c) 2100 UTC 25 Mar, and (d) 0000 UTC 26 Mar X Y X Y X Y X Y A

a) FULLTER UTC Group X Group Y Group Z b) NOSIERRA UTC Figure 6. Three-dimensional 15-h (0000−1500 UTC 25 Mar 2006) trajectories from (a) FULLTER and (b) NOSIERRA. Group X forward trajectories (brown) begin at 850 hPa upstream of the Sierra Nevada. Group Y and Z backwards trajectories (green and light green, respectively) terminate at 850 hPa or the half-η level, whichever is higher. FULLTER-NOSIERRA lowest half-η level potential temperature difference (color filled as in Fig. 5) and terrain difference (0–1000m gray, >1000m black). Trajectory layering based on plotting order and does not indicate relative altitude. Trajectories discussed in text and presented in Fig. 7 labeled to left of start position and right of ending arrow Group X Group Y Group Z

Figure 7. Pressure and potential temperature along (a) trajectories 1 and 2 and (b) trajectories 3 and 4 of Fig. 6. a) Trajectories 1 & 2b) Trajectories 3 & 4

Pressure (hPa) a) FULLTER 1500 UTC Figure 8. Cross sections along line XY (see Fig. 4 and other figures for locations) at 1500 UTC 25 Mar (a) FULLTER potential temperature (contours every 2K), total cloud water and ice mixing ratio (gray shaded at.0001,.1, and.2 g kg -1 intervals), total diabatic heating rate produced by the explicit moisture scheme and cumulus parameterization (K hr -1, shaded following inset scale), and vectors of along-section wind and pressure vertical velocity (following inset scale). (b) Same as (a) except for NOSIERRA. (c) FULLTER potential temperature [as in (a)] and FULLTER- NOSIERRA potential temperature difference (K, shaded following inset scale). Shading over Sierra Nevada indicates region where differences in the height of the half-η surfaces contribute to the anomaly and introduce a false positive bias. X Y Pressure (hPa) b) NOSIERRA 1500 UTC X Y 35 m s hPa s -1 Pressure (hPa) c) FULLTER w/ Anomaly 1500 UTC X Y

Figure 9. Same as Fig. 4 except for 1800 UTC 25 Mar c) FULLTER Kinematic (F w ) 1800 UTC d) NOSIERRA Kinematic (F w ) 1800 UTC ms -1 e) FULLTER Diabatic (F D ) 1800 UTC f) NOSIERRA Diabatic (F D ) 1800 UTC a) FULLTER Cloud/Radar 1800 UTC b) NOSIERRA Cloud/Radar 1800 UTC X Y X Y

Pressure (hPa) a) FULLTER 1800 UTC X Y Pressure (hPa) b) NOSIERRA 1800 UTC X Y 35 m s hPa s -1 Figure 10. Same as Fig. 8 except for 1800 UTC 25 Mar Pressure (hPa) c) FULLTER w/ Anomaly 1800 UTC X Y

b) FULLTER-NOSIERRA 2100 UTC X Y X Y a) FULLTER-NOSIERRA 1800 UTC Figure 11. FULLTER lowest half-η level potential temperature (every 2 K) and FULLTER- NOSIERRA surface heat flux difference [W m -2, shaded according to scale in (a)] at (a) 1800 UTC 25 Mar and (b) 2100 UTC 25 Mar 2006.

Figure 12. Same as Fig. 4 except for 2100 UTC 25 Mar c) FULLTER Kinematic (F w ) 2100 UTC d) NOSIERRA Kinematic (F w ) 2100 UTC ms -1 e) FULLTER Diabatic (F D ) 2100 UTC f) NOSIERRA Diabatic (F D ) 2100 UTC a) FULLTER Cloud/Radar 2100 UTC b) NOSIERRA Cloud/Radar 2100 UTC X Y X Y A A

Pressure (hPa) a) FULLTER 2100 UTC X Y Pressure (hPa) b) NOSIERRA 2100 UTC X Y 35 m s hPa s -1 Pressure (hPa) c) FULLTER w/ Anomaly 2100 UTC X Y Figure 13. Same as Fig. 8 except for 2100 UTC 25 Mar

Pressure (hPa) Figure 14. FULLTER (red) and NOSIERRA (blue) skew T–log p diagram (temperature and dewpoint) for point A (see Figs. 5c and 12c,d for location) at 2100 UTC 25 Mar 2006.

Group A Group B Group C Group D Group E Group A Group B Group C Group D Group E a) FULLTER b) NOSIERRA Figure 15. Three-dimensional nine-hour trajectories ending at 2100 UTC. (a) FULLTER and (b) NOSIERRA. Trajectory number indicated to right of trajectory ending arrow. FULLTER-NOSIERRA lowest half-η level potential temperature difference (color filled following inset scale) and terrain difference shaded (0–1000m gray, >1000m black). Update w/ Same color Scale as Fig. 5 Update Fig. Cap following Fig. 6

c) FULLTER Kinematic (F w ) 0000 UTC d) NOSIERRA Kinematic (F w ) 0000 UTC ms -1 c) FULLTER Diabatic (F D ) 0000 UTC d) NOSIERRA Diabatic (F D ) 0000 UTC Figure 16. Same as Fig. 4 except for 0000 UTC 26 Mar a) FULLTER Cloud/Radar 0000 UTC b) NOSIERRA Cloud/Radar 0000 UTC e) FULLTER Diabatic (F D ) 0000 UTC f) NOSIERRA Diabatic (F D ) 0000 UTC X Y X Y

a) FULLTER b) NOSIERRA c) FULLTER-FKDRYd) NOSIERRA-FKDRY Figure 17. Lowest half-η level potential temperature (thin contours every 2 K), potential temperature gradient magnitude [thick contours every 5 K (100 km) -1 beginning with 10 K (100 km) -1 ], wind [vector scale at upper left of (a)], and kinematic frontogenesis [K (100 km h) −1, shaded following scale in Fig. 4c] from (a) FULLTER, (b) NOSIERRA, (c) FULLTER-FKDRY, and (d) NOSIERRA-FKDRY at 0000 UTC 26 Mar ms -1

Pressure (hPa) a) FULLTER 0000 UTC X Y Pressure (hPa) b) NOSIERRA 0000 UTC X Y 35 m s hPa s -1 Pressure (hPa) c) FULLTER w/ Anomaly 0000 UTC X Y Figure 18. Same as Fig. 8 except for 0000 UTC 26 Mar