Assignment #5: Cumulus Parameterization Sensitivity Due: 14 November 2017

Similar documents
National Scientific Library at Tbilisi State University

Impact of GPS RO Data on the Prediction of Tropical Cyclones

A Study of Convective Initiation Failure on 22 Oct 2004

Post Processing of Hurricane Model Forecasts

Description of. Jimy Dudhia Dave Gill. Bill Skamarock. WPS d1 output. WPS d2 output Real and WRF. real.exe General Functions.

IMPACT OF GROUND-BASED GPS PRECIPITABLE WATER VAPOR AND COSMIC GPS REFRACTIVITY PROFILE ON HURRICANE DEAN FORECAST. (a) (b) (c)

WRF MODEL STUDY OF TROPICAL INERTIA GRAVITY WAVES WITH COMPARISONS TO OBSERVATIONS. Stephanie Evan, Joan Alexander and Jimy Dudhia.

Projected future increase of tropical cyclones near Hawaii. Hiroyuki Murakami, Bin Wang, Tim Li, and Akio Kitoh University of Hawaii at Manoa, IPRC

ABSTRACT 2 DATA 1 INTRODUCTION

WRF Modeling System Overview

Numerical Simulation of a Severe Thunderstorm over Delhi Using WRF Model

P Hurricane Danielle Tropical Cyclogenesis Forecasting Study Using the NCAR Advanced Research WRF Model

608 SENSITIVITY OF TYPHOON PARMA TO VARIOUS WRF MODEL CONFIGURATIONS

Simulations with different convection parameterizations in the LM

Kelly Mahoney NOAA ESRL Physical Sciences Division

HWRF sensitivity to cumulus schemes

CHAPTER 8 NUMERICAL SIMULATIONS OF THE ITCZ OVER THE INDIAN OCEAN AND INDONESIA DURING A NORMAL YEAR AND DURING AN ENSO YEAR

Weather report 28 November 2017 Campinas/SP

Predicting Tropical Cyclone Formation and Structure Change

Tropical Cyclone Intensity and Structure Changes in relation to Tropical Cyclone Outflow

User's Guide for the NMM Core of the Weather Research and Forecast (WRF) Modeling System Version 3. Chapter 4: WRF-NMM Initialization

Q.1 The most abundant gas in the atmosphere among inert gases is (A) Helium (B) Argon (C) Neon (D) Krypton

11 days (00, 12 UTC) 132 hours (06, 18 UTC) One unperturbed control forecast and 26 perturbed ensemble members. --

Variational data assimilation of lightning with WRFDA system using nonlinear observation operators

Pacific Storm Track at Different Horizontal Resolutions Snap-shot of Column Liquid Water Content

SIMULATION OF ATMOSPHERIC STATES FOR THE CASE OF YEONG-GWANG STORM SURGE ON 31 MARCH 2007 : MODEL COMPARISON BETWEEN MM5, WRF AND COAMPS

Sensitivity of precipitation forecasts to cumulus parameterizations in Catalonia (NE Spain)

Tue 3/1/2016. Arakawa-Schubert, Grell, Tiedtke, Zhang-McFarlane Explicit convection Review for MT exam

A comparative study on the genesis of North Indian Ocean cyclone Madi (2013) and Atlantic Ocean cyclone Florence (2006)

WRF Modeling System Overview

Development of a Coupled Atmosphere-Ocean-Land General Circulation Model (GCM) at the Frontier Research Center for Global Change

The Role of Post Cold Frontal Cumulus Clouds in an Extratropical Cyclone Case Study

Preliminary results. Leonardo Calvetti, Rafael Toshio, Flávio Deppe and Cesar Beneti. Technological Institute SIMEPAR, Curitiba, Paraná, Brazil

Predicting Tropical Cyclone Formation and Structure Change

WRF Pre-Processing (WPS)

2012 AHW Stream 1.5 Retrospective Results

WRF Model Simulated Proxy Datasets Used for GOES-R Research Activities

The impact of rain on ocean wave evolution and its feedback to the atmosphere

2. Outline of the MRI-EPS

Unified Cloud and Mixing Parameterizations of the Marine Boundary Layer: EDMF and PDF-based cloud approaches

Upgrade of JMA s Typhoon Ensemble Prediction System

Project Summary 2015 DTC Task MM5: Test of an Expanded WRF-ARW Domain

Final Examination, MEA 443 Fall 2008, Lackmann

USING PROGRAM HURRICANE. Download all the files, including the (empty) output subdirectory into a new folder on your machine.

New Zealand Heavy Rainfall and Floods

Tropical Cyclone Formation/Structure/Motion Studies

Francis O. 1, David H. Bromwich 1,2

3.4 THE IMPACT OF CONVECTIVE PARAMETERIZATION SCHEMES ON CLIMATE SENSITIVITY

the 2 past three decades

Comparison of Typhoon Track Forecast using Dynamical Initialization Schemeinstalled

Precipitation in climate modeling for the Mediterranean region

Motivation & Goal. We investigate a way to generate PDFs from a single deterministic run

Impact of different cumulus parameterizations on the numerical simulation of rain over southern China

Mesoscale atmospheric modeling of the San Francisco Bay Area using the Weather Research & Forecasting model (WRF)

Simulation studies for Lake Taihu effect on local meteorological environment. Ren Xia

2D.4 THE STRUCTURE AND SENSITIVITY OF SINGULAR VECTORS ASSOCIATED WITH EXTRATROPICAL TRANSITION OF TROPICAL CYCLONES

A review of VOCALS Hypothesis. VOCALS Science Meeting July 2009 Seattle Washington C. R. Mechoso, UCLA

Advanced Research WRF High Resolution Simulations of Hurricanes Katrina, Rita and Wilma (2005)

Track sensitivity to microphysics and radiation

Mesoscale and High Impact Weather in the South American Monsoon Leila M. V. Carvalho 1 and Maria A. F. Silva Dias 2 1

Assessment of the Noah LSM with Multi-parameterization Options (Noah-MP) within WRF

Maximization of Historical Severe Precipitation Events over American, Yuba and Feather River Basins

Quarterly numerical weather prediction model performance summaries April to June 2010 and July to September 2010

10B.2 THE ROLE OF THE OCCLUSION PROCESS IN THE EXTRATROPICAL-TO-TROPICAL TRANSITION OF ATLANTIC HURRICANE KAREN

Shu-Ya Chen 1, Tae-Kwon Wee 1, Ying-Hwa Kuo 1,2, and David H. Bromwich 3. University Corporation for Atmospheric Research, Boulder, Colorado 2

Have a better understanding of the Tropical Cyclone Products generated at ECMWF

Cloud parameterization and cloud prediction scheme in Eta numerical weather model

Hui-Ya Chuang. Presented by Matthew Pyle

Lecture 8. Monsoons and the seasonal variation of tropical circulation and rainfall

Lightning Data Assimilation using an Ensemble Kalman Filter

Three-dimensional Structure in Midlatitude Cyclones. ATMS 370 Due Friday, March 9, 2018

The 5th Research Meeting of Ultrahigh Precision Meso-scale Weather Prediction, Nagoya University, Higashiyama Campus, Nagoya, 9 March 2015

MOTIVATION. New view of Arctic cyclone activity from the Arctic System Reanalysis

MEA 716 Exercise, BMJ CP Scheme With acknowledgements to B. Rozumalski, M. Baldwin, and J. Kain Optional Review Assignment, distributed Th 2/18/2016

Boundary layer equilibrium [2005] over tropical oceans

Subtropical and Hybrid Systems IWTC VII Topic 1.6

MODEL TYPE (Adapted from COMET online NWP modules) 1. Introduction

SUPPLEMENTAL MATERIALS FOR:

Fernando Prates. Evaluation Section. Slide 1

Output Module (last updated 8/27/2015)

Description of the ET of Super Typhoon Choi-Wan (2009) based on the YOTC-dataset

WRF Modeling System Overview

Dynamic Sensitivity Analysis of Tropical Cyclone Track and Extratropical Transition

Aerosol-Cloud-Precipitation-Climate (ACPC) Initiative: Deep Convective Cloud Group Roadmap Updated: October 2017

Why the Atlantic was surprisingly quiet in 2013

Tropical Storm Hermine: Heavy rainfall in western Gulf By Richard H. Grumm National Weather Service Office State College, PA 16803

Shear-Parallel Mesoscale Convective Systems in a Moist Low- Inhibition Mei-Yu Front Environment. Liu and Moncrieff (2017 JAS)

Numerical Weather Prediction: Data assimilation. Steven Cavallo

16D.4 Evaluating HWRF Forecasts of Tropical Cyclone Intensity and Structure in the North Atlantic Basin

Atmospheric Processes

8.3 A STUDY OF AIR-SEA INTERACTIONS AND ASSOCIATED TROPICAL HURRICANE ACTIVITY OVER GULF OF MEXICO USING SATELLITE DATA AND NUMERICAL MODELING

IOP Conference Series: Materials Science and Engineering. Related content PAPER OPEN ACCESS

WRF Derecho case. (Experiment 4 at end)

Examination of Tropical Cyclogenesis using the High Temporal and Spatial Resolution JRA-25 Dataset

Introduction of products for Climate System Monitoring

Chapter 1. Introduction

ESCI 241 Meteorology Lesson 19 Tropical Cyclones Dr. DeCaria

Ensemble Prediction Systems

1. Introduction. In following sections, a more detailed description of the methodology is provided, along with an overview of initial results.

CPTEC and NCEP Model Forecast Drift and South America during the Southern Hemisphere Summer

Transcription:

Assignment #5: Cumulus Parameterization Sensitivity Due: 14 November 2017 Objectives In this assignment, we use the WRF-ARW model to run two nearly-identical simulations in which only the cumulus parameterization varies to quantify, for this case, the extent to which varying the treatment of both deep and shallow cumulus clouds influences a three-day forecast over a tropical to subtropical model domain. This assignment is also designed to give you additional experience in configuring and running a state-of-the-art numerical model as well as with posing and testing robust hypotheses related to how numerical model configuration variation influences the forecast. As in the most recent assignment, we will use comet for this task. A Preliminary Task To complete the analysis portions of this assignment, we must modify the WRF-ARW model code so that it outputs four variables that are computed by but not typically output from the model. This involves modifying the WRF-ARW Registry, which documents all model variables and their input and output characteristics. 1. (5 pts) On comet, change into the Registry subdirectory of your WRFV3 directory. Open Registry.EM_COMMON with a text editor. Search (in nano, using Ctrl-W) for the entries for h_diabatic and qv_diabatic. Change the eighth column for each variable so that it reads rhdu. Search for the entries for RTHCUTEN and RQVCUTEN. Change the eighth column for each variable so that it reads rh. Save the file, then exit the text editor and return to your WRFV3 directory. Clean the earlier code installation by running./clean -a. Recompile the model following the steps from Assignment 1. Once this completes successfully, change into the test/em_real/ subdirectory and copy its contents to your WRF_run directory. After doing so, change into the WRF_run directory, use ls -al to list its contents, and include a screen capture with your completed assignment. Simulation Information: Domain and Model Configuration Both model simulations use the same 0.25 GFS analysis and forecast data as in Assignment 4 to specify the initial and lateral boundary conditions. Duration: 72 h (0000 UTC 19 September 2017 to 0000 UTC 22 September 2017) Lateral Boundary Data Frequency: 6 h (21,600 s) Domain Size (E-W x N-S x levels): 200 x 200 x 30 Horizontal Grid Spacing: 20 km (20,000 m) Assignment 5, Page 1

Map Information: usgs_lakes+2m geographic data; Mercator map projection, center point of 25.0 N, 75.0 W; tangent latitude: 0.0 N, standard longitude: 97.0 W. History Interval: 3 h (180 min) Time Step: 5 * Δx, where Δx is in km num_metgrid_levels: 32 Physics Suite: the standard CONUS suite for simulation #2 and the standard CONUS suite with a new cu_physics = 1, -1, -1, entry for simulation #1. The standard CONUS suite uses the Tiedtke cumulus parameterization, whereas cu_physics = 1 specifies the Kain-Fritsch cumulus parameterization. Both are low-level control parameterizations that parameterize both deep and shallow cumulus clouds but differ in how they determine if, when, and where both types of clouds exist (e.g., in their trigger functions). Physics Time Steps: 0 for boundary layer, equal to Δx (in km) for radiation and convection num_land_cat: 28 Gravity Wave Drag Option: off (0) 2. (5 pts) Edit namelist.wps in your WPS directory and namelist.input in your WRF_run directory to account for this information. Include copies of each file with your assignment. Use plotgrids_new.ncl in the WPS/util/ subdirectory to create a plot of the model domain, and include a copy of this plot with your assignment. 3. (5 pts) Complete and run both simulations. This includes running geogrid.exe, ungrib.exe, metgrid.exe, real.exe, and wrf.exe (the latter three all by job submission script), as you did for Assignment 4. Rename the output from your first simulation as wrfout_kf_2017-09- 19_00:00:00 before running the second simulation. Rename the output from your second simulation as wrfout_tiedtke_2017-09-19_00:00:00. After both simulations are complete, run ls -al in your WRF_run directory and include a screen capture of the output with your assignment. 4. (5 pts) As in Assignment 4, use ARWpost to post-process both simulations. The ARWpost namelist is configured similarly to in Assignment 4, except the output variable list should have H_DIABATIC, QV_DIABATIC, RTHCUTEN, RQVCUTEN, and QVAPOR added before post-processing each simulation. Include a copy of the final namelist.arwpost file with your assignment. Change into the directory where you directed ARWpost to save its output. Run ls -al in this directory and include a screen capture of the output with your assignment. Simulation Analysis and Diagnosis As in Assignment 4, we will use GrADS to visualize the post-processed model output to be able to gain insight into forecast sensitivity to the chosen cumulus parameterization. Assignment 5, Page 2

5. (16 pts) Create plots, every 3 h from 0300 UTC 19 September to 0300 UTC 20 September, of the difference (Kain-Fritsch minus Tiedtke) in 700 hpa temperature (contours at ±4, 3, 2, and 1 C). Title each plot with the time of the analysis, and include each with your assignment. In the analysis to come, focus on three regions: within +/- 5 of tropical cyclones Jose (35.2 N, 71.3 W) and Maria (15.5 N, 61.4 W) over the western Atlantic Ocean between, but more than 5 away from, Jose and Maria over the southeastern United States excluding the Florida peninsula Describe the sign, magnitude, and temporal variation in the 700 hpa temperature difference in each area. In particular, discuss similarities and differences, and advance a physicallybased hypothesis as to why they exist, in the temporal variation between the second and third regions listed above. 6. (16 pts) Create three time-height cross-sections, each as separate images, from 0300 UTC 19 September to 0000 UTC 22 September between 1000-300 hpa (with a logarithmic vertical axis): area-averaged (between 30-35 N, 89-81 W; over the southeast United States) temperature difference (Kain-Fritsch minus Tiedtke; contours at ±2.5, 2, 1.5, 1, and 0.5 C) area-averaged (again between 30-35 N, 89-81 W) difference (Kain-Fritsch minus Tiedtke) in the potential temperature tendency due to the cumulus parameterization (RTHCUTEN, which is in K s -1 ; plot with contours at ±5, 4, 3, 2, and 1 K day -1 ) area-averaged (again between 30-35 N, 89-81 W) difference (Kain-Fritsch minus Tiedtke) in the water vapor mixing ratio tendency due to the cumulus parameterization (RQVCUTEN, which is in g g -1 s -1 ; plot with contours at ±3, 2, and 1 g kg -1 day -1 ) Title each image appropriately and include copies with your assignment. Discuss the sign/magnitude, vertical structure, and temporal evolution of the differences indicated by each plot. Given the altitude(s) at which they are predominantly found, do you believe each to result primarily from shallow or deep cumulus parameterization? Why? Given this answer and what you know about the physical role(s) of shallow or deep cumulus in the atmosphere, hypothesize as to what physical process(es) are parameterized differently between the Kain-Fritsch and Tiedtke parameterizations to result in these differences. Note: ARWpost post-processes the longitude information for Mercator projections relative to E, such that 90 W = 270 E and 60 W = 300 E. Further, as the requested plot varies in the z and t dimensions, the x and y dimensions must be fixed to a single x-y/lon-lat point to create the desired plot. It does not matter which single point is chosen. Assignment 5, Page 3

7. (16 pts) Create the same three plots as in the previous question, except for the area-average between 27-33 N, 75-65 W, or over the western Atlantic Ocean, between 1200 UTC 19 September and 0000 UTC 22 September. Title each image appropriately and include copies with your assignment. Describe how the altitude(s) of and temporal variability in the differences vary between in this analysis and that in the previous question. Hypothesize as to physically why the altitude(s) and temporal variability varies between over land in the previous question and over water in this question. 8. (16 pts) Create a plot at 0600 UTC 19 September of the 1000-100 hpa (with a logarithmic vertical axis), area-averaged (between 14.25-17.25 N, 63-59.5 W; centered on tropical cyclone Maria) potential temperature tendency due to the cumulus parameterization (RTHCUTEN; convert from K s -1 to K day -1 ) for the Kain-Fritsch simulation (default black line) and Tiedtke simulation (default green line). Title the plot appropriately and include a copy with your assignment. Discuss similarities and differences in the vertical structure of this diabatic heating term between the two simulations. As both parameterizations trigger deep, moist convection in an attempt to locally eliminate CAPE over a specified time interval, based on this analysis which parameterization will be more effective at doing so whether physically or nonphysically over a short time interval? Why? Tropical cyclone intensification is theorized to result from surface latent heat fluxes, with deep, moist convection acting as a conduit for lofting this heat, which is released primarily upon condensation, into the middle to upper troposphere. If the diabatic heating profiles at this time are representative of those at other times, in which simulation do you believe the simulated Maria will become the strongest? Why? Create a plot of sea level pressure from each simulation (contours every 4 hpa; Kain-Fritsch in rainbow colors, Tiedtke in blacks) at 0000 UTC 22 September over the domain 15-27 N, 77-62 W. Title this image appropriately and include a copy with your assignment. Does this plot support your answer? If not, hypothesize why. 9. (16 pts) To first order, tropical cyclones are steered by the synoptic-scale wind averaged between the lower and middle/upper troposphere (e.g., 850-300 hpa). Consider the areaaveraged, time-height cross-section of temperature difference that you created in Question 6. From this analysis, would you expect the area-averaged horizontal wind in the 850-300 hpa layer to be more anticyclonic, more cyclonic, or about the same in the Kain-Fritsch simulation versus the Tiedtke simulation? Why? Create a plot at 0000 UTC 22 September of vertically-averaged (from 850-300 hpa) Assignment 5, Page 4

horizontal wind difference (Kain-Fritsch minus Tiedtke; barbs every fifth grid point in kt, noting that u and v are provided in m s-1) between 24-33 N, 80-60 W. Title this image appropriately and include a copy with your assignment. What does this analysis indicate? Does it support your original answer? Consider again the sea level pressure analysis at 0000 UTC 22 September from the previous question. Given your answers to this question, discuss why the simulated Maria position differences exist between the two simulations. Assignment 5, Page 5