Numerical Forecast Models For more info: www.meted.ucar.edu/nwp/pcu1/ic2/index.htm.

Slides:



Advertisements
Similar presentations
THE WATER CYCLE The water cycle — the continuous exchange of water between Earth's surface and atmosphere — is Earth's natural mechanism for recycling.
Advertisements

What Causes Changes in the Weather ?
A NUMERICAL PREDICTION OF LOCAL ATMOSPHERIC PROCESSES A.V.Starchenko Tomsk State University.
Jeopardy MatterClouds Water Cycle Weather Maps Q $100 Q $200 Q $300 Q $400 Q $500 Q $100 Q $200 Q $300 Q $400 Q $500 Final Jeopardy.
Discretizing the Sphere for Multi-Scale Air Quality Simulations using Variable-Resolution Finite-Volume Techniques Martin J. Otte U.S. EPA Robert Walko.
7. Radar Meteorology References Battan (1973) Atlas (1989)
The Problem of Parameterization in Numerical Models METEO 6030 Xuanli Li University of Utah Department of Meteorology Spring 2005.
SC.D CS The student knows that the water cycle is influenced by temperature, pressure, and the topography of the land. Content Limits: Items will.
NOAA/NWS Change to WRF 13 June What’s Happening? WRF replaces the eta as the NAM –NAM is the North American Mesoscale “timeslot” or “Model Run”
1 Use of Mesoscale and Ensemble Modeling for Predicting Heavy Rainfall Events Dave Ondrejik Warning Coordination Meteorologist
For the Lesson: Eta Characteristics, Biases, and Usage December 1998 ETA-32 MODEL CHARACTERISTICS.
UNIT THREE: Matter, Energy, and Earth  Chapter 8 Matter and Temperature  Chapter 9 Heat  Chapter 10 Properties of Matter  Chapter 11 Earth’s Atmosphere.
Earth’s Weather Weather Terms.
Chapter 8 Coordinate Systems.
Using 925 mb Temperatures to Improve Operational River Forecasts Ronald S. W. Horwood Meteorologist National Weather Service Northeast River Forecast Center.
Nesting. Eta Model Hybrid and Eta Coordinates ground MSL ground Pressure domain Sigma domain  = 0  = 1  = 1 Ptop  = 0.
Rapid Update Cycle Model William Sachman and Steven Earle ESC452 - Spring 2006.
Weather Research & Forecasting Model (WRF) Stacey Pensgen ESC 452 – Spring ’06.
GFS Deep and Shallow Cumulus Convection Schemes
Ensemble Post-Processing and it’s Potential Benefits for the Operational Forecaster Michael Erickson and Brian A. Colle School of Marine and Atmospheric.
Weather Forecasting - II. Review The forecasting of weather by high-speed computers is known as numerical weather prediction. Mathematical models that.
Lecture 4 Weather Maps and Models Chapters 3 and 4.
Basic Concepts of Numerical Weather Prediction 6 September 2012.
Learning About the Earth
Chapter 7 – Precipitation Processes
AOS 101 Weather and Climate Lisha M. Roubert University of Wisconsin-Madison Department of Atmospheric & Oceanic Sciences.
Numerical Forecast Models For more info:
Nesting. Eta Model Eta Coordinate And Step Mountains MSL ground  = 1 Ptop  = 0.
Chapter 2 Section 3 Winds.
Forecasting and Numerical Weather Prediction (NWP) NOWcasting Description of atmospheric models Specific Models Types of variables and how to determine.
Upper Air Charts By Tom Collow November 8, Reading Upper Air Charts Temperature (°C) Dewpoint Depression (°C) Height Wind direction and speed (knots)
A weather instrument that measures the wind speed.
The National Environmental Agency of Georgia L. Megrelidze, N. Kutaladze, Kh. Kokosadze NWP Local Area Models’ Failure in Simulation of Eastern Invasion.
Mesoscale Modeling Review the tutorial at: –In class.
NATS 101 Section 13: Lecture 24 Weather Forecasting Part I.
Chapter 3 The Changing Weather. Chapter 3 Terms Condensation Condensation Orographic Condensation Orographic Condensation Convectional Condensation Convectional.
Comparison of Different Approaches NCAR Earth System Laboratory National Center for Atmospheric Research NCAR is Sponsored by NSF and this work is partially.
Water and Weather Chapter Six: Weather and Climate 6.1 Introduction to Weather 6.2 Weather Patterns 6.3 Climates and Biomes.
Non-hydrostatic Numerical Model Study on Tropical Mesoscale System During SCOUT DARWIN Campaign Wuhu Feng 1 and M.P. Chipperfield 1 IAS, School of Earth.
Higher Resolution Operational Models. Operational Mesoscale Model History Early: LFM, NGM (history) Eta (mainly history) MM5: Still used by some, but.
Who Wants to be a Millionaire? A Weather Forecasting System Review Circle your answer as you go. Mark it right or wrong as you go.
Sensitivity Analysis of Mesoscale Forecasts from Large Ensembles of Randomly and Non-Randomly Perturbed Model Runs William Martin November 10, 2005.
Gouge – Navy slang for the bare essential knowledge to get by.
Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Section 3 Precipitation Chapter 23 Objectives Identify the four forms.
Water cycle and precipitation. Evaporation/Transpiration · Water enters the atmosphere as water vapor through evaporation and transpiration, plants releasing.
Higher Resolution Operational Models. Major U.S. High-Resolution Mesoscale Models (all non-hydrostatic ) WRF-ARW (developed at NCAR) NMM-B (developed.
Energy in the Atmosphere Energy from the sun travels to Earth as electromagnetic waves – mostly visible light, infrared radiation (longer wavelengths)
Have you ever just looked at clouds?  Why do we have clouds?  Why are there different shapes?  What can they tell us about the weather?
Lecture 5 Weather Maps and Models Chapters 5 and Chapter 6 Homework Due Friday, October 3, 2014 TYU Ch 6: 1,2,5,7,11,14,17,18,20; TYPSS Ch 6: 2 TYU Ch.
What is Weather? Wind Temperature Humidity (moisture in the air) Air Pressure The condition of the atmosphere in a certain place.
Surface Condensation Water vapor condensing on large surfaces is called dew. Dew Point is the temperature that saturation occurs and condensation begins.
Types of Clouds. Is that a space weapon you see in this photo? Not at all. This scientist in China is launching tiny crystals of silver iodide into the.
Vincent N. Sakwa RSMC, Nairobi
Brian Freitag 1 Udaysankar Nair 1 Yuling Wu – University of Alabama in Huntsville.
Higher Resolution Operational Models
Air Pressure & Wind Patterns. What is air pressure?  Air pressure is the force of molecules pushing on an area.  Air pressure pushes in all direction.
Water in the Atmosphere Section 3 Section 3: Precipitation Preview Key Ideas Forms of Precipitation Causes of Precipitation Measuring Precipitation Weather.
Numerical Weather Forecast Model (governing equations)
Weather and Climate.
Overview of Downscaling
Grid Point Models Surface Data.
Update on the Northwest Regional Modeling System 2013
  Robert Gibson1, Douglas Drob2 and David Norris1 1BBN Technologies
Overview of Deterministic Computer Models
How do models work? METR 2021: Spring 2009 Lab 10.
Better Forecasting Bureau
The Stone Age Prior to approximately 1960, forecasting was basically a subjective art, and not very skillful. Observations were sparse, with only a few.
Update on the Northwest Regional Modeling System 2017
Water and Weather. Water and Weather Chapter Six: Weather and Climate 6.1 Introduction to Weather 6.2 Weather Patterns 6.3 Climates and Biomes.
Numerical Forecast Models
Presentation transcript:

Numerical Forecast Models For more info:

The Models WRF (currently the NAM) US model output is at NCEP or NCAR-RAP GFS (NCEP) RUC (NCEP) ECMWF (Europe) NoGaps (Navy) MM5 GEM (Canada) Eta (formerly the NAM) Many more – individuals, universities, and government agencies have their own! You too can write a model.

Did Lorenz (famous theoretical meteorologist) really say that?

How do models work?

You only have observations at specific places (stations) Convert derivatives to finite differences

So, models work by approximating the equations using finite differences on a model “grid.” (exception: spectral models) ∆x is the grid interval in the west-east direction. ∆y is south-north. ∆t is time.

The NAM-WRF, sometimes called the NMM (Non-hydrostatic Mesoscale Model) has a new staggered grid and a 12-km resolution.

You solve the finite difference equations for the points on a map. Depending on your computer size, you may only get a limited number of grid points. The limited area where your model is defined is called the “Domain”

For a global model, the entire Earth is the Domain

The WRF model which is the basis for the North American Mesoscale model has a domain centered on - guess which continent. (March 2008)

If your domain is not global, you have artificial “boundaries”. Since these don’t exist in the real atmosphere, any effects from these boundaries are computational. The effects propagate into the interior as fast as air parcels move.

32-km Eta model terrain Once you define a domain, you need boundary conditions. The real Earth has topography. Your lower boundary must have mountains!

Here’s a closer look at the Southwest and Northeast U.S. terrain in the 22 km Eta (22 km horizontal grid spacing). What do you think? (Remember the butterfly!)

The latest NAM-WRF model terrain

“Box 47” view of eastern NY in the NAM-WRF

13km RUC Improvements expected from 13km RUC - Improved near-surface forecasts - Improved precipitation forecasts - Better cloud/icing depiction - Improved frontal/turbulence forecasts Terrain elevation m interval

Atmospheric models are three dimensional. You also need a vertical grid. Resolution in the vertical is much better than in the horizontal. But is it good enough?

The NAM-WRF has 60 vertical layers, as did the NAM-Eta. The top level in the NAM-WRF is 2 mb instead of the 25 mb Eta top level.

The NAM-WRF uses a vertical coordinate that is proportional to the surface pressure. So elevated terrain has very thin layers near the ground no matter how high it is. The old Eta had thin layers only near 1000 mb leading to errors in the western U.S. The vertical resolution is lowest near 500 mb and increases again near 250 mb for better depiction of jet stream shears.

Models have top and bottom boundaries. The real atmosphere doesn’t so how you program these affects model performance. Many models use nondimensional (sigma) coordinates (P/P ref )

The Stepwise Eta Coordinate System (Eta model)

At each grid point, you have seven finite difference equations, each with multiple mathematical operations. If your horizontal grid resolution is 12 km, how many 12 x 12 km boxes would you need for the entire world? A: Earth’s radius ~ 6370 km, Area of a sphere = 4  r 2 so the Earth’s area is approximately 5.1 x 10 8 km 2 12km x 12km = 144 km 2 so you need 3,541,003 boxes! You also have 60 levels of grid points so multiply that answer by 60 to get 2.12 x 10 8 boxes!!! But you only need that kind of resolution in a limited area, like North America. One solution is to use a wider spacing for most of the world, but a very fine spacing in your area of interest. That’s called Nesting Grid Modeling. The NAM-WRF is a nested grid model

Here are the NAM-WRF model’s nested grid domains

The first nested grid model was the NGM (nested grid model!) It had three grids, A, B, and C. The A grid was the entire world. A B C

When you nest a model, you run the model equations for each grid, with different grid spacings. It takes at least three times as much computer time.

Two-way interaction is now the standard

Nested Grid modeling allows the forecaster to “zoom in” on the local forecast region How far in can we zoom? What are the modeling considerations? With more calculations come more errors. Smaller grids need more calculations.

A neat feature of the WRF is the “moving nest”

Initialization. How do we start the model? A: Somehow we need to assess the atmosphere’s true initial state. Right down to each butterfly. Any butterflies missed?

The models are 3-dimensional so you need data from above the surface. This is the most dense upper air network in the world.

Every Model operates on a “framework” or procedure. The NAM would be like this: This part would be the WRF 

Spectral Models Instead of solving for the variables (u,v,w, etc.) at grid points, some models solve for wave solutions. The GFS is a spectral model The complete description of the GFS spectral model is at

Good wave example. How many are around the 45°N latitude circle? (very approximately shown in black)

Question: To resolve the equivalent of today’s waves, how fine a resolution would a grid point model need? To resolve a single wave, you need, at a minimum, 5 grid points.

What is the wavelength of the waves in the example shown before? Take the circumference of the 45°N latitude circle. C = 2πr where r is the radius of that circle. In this case r = a sin 45° where a is the Earth’s radius. So, a ~ 4500 km and C ~ km. With 7 waves today, the average wavelength is around 4000 km (2500 miles). So your points must be a minimum of 800 km or 500 miles apart. Question: Suppose you wanted to resolve smaller features, say 20 km in width? How many waves would you need? 28,000 km/20 = 1400 waves Would you ever want to resolve more?

This is the simulated radar from the NAM-WRF It looks like individual thunderstorm cells can be forecast.

Parameterization If the weather element you are trying to forecast is smaller than a grid box or one wave in a spectral model, your model can’t handle it. Even with a grid spacing of 12 km, your model won’t predict individual cumulus clouds. Real weather depends on very small-scale (called sub-grid scale) processes such as cloud or even raindrop formation. Models must forecast these processes correctly. Do you have to forecast each raindrop? To include sub-grid scale processes, we build in computer subroutines called parameterization schemes.

Clouds in the WRF model consist of liquid droplets or ice particles (depending on temperature of cloud and cloud top)

Condensation in the Eta Model  Grid-point condensation occurs in model at two different RH thresholds –Over land, when RH exceeds 75% –Over water, when RH exceeds 80%

Precipitation in the Eta Model Continued Parameterization of precipitation includes six major microphysical processes 1Autoconversion of cloud water to rain 2Collection of cloud droplets by the falling rain drops 3Autoconversion of ice particles to snow 4Collection of ice particles by the falling snow 5Melting of snow below the freezing line 6Evaporation of precipitation below cloud bases

An example of how tricky parameterization can be.

Sub-grid scale processes requiring parameterization: Friction (includes turbulence and ground ) Convection Deep convection = thunderstorms Shallow convection = cumulus clouds Ice crystal formation Raindrop formation Cloud droplet formation Cloud electrification Atmospheric aerosols

Ensemble Forecasting Where to find products: (environmental modeling center) (short range) (Canada) Tutorial:

Basic Terminology for ensemble forecasts ENSEMBLE forecast - A collection of individual forecasts valid at the same time. MEMBER - An individual solution in the Ensemble. CONTROL - The member of the ensemble obtained from the best initial analysis (the Control is usually what is perturbed to produce the remaining members in the ensemble). ENSEMBLE MEAN (or MEAN) - The average of the members. SPREAD (or “uncertainty”) - The standard deviation about the mean (also known as the "envelope of solutions").

. Typical ensemble forecast of MSLP from SPC/SREF. You get the mean and standard deviation (shaded)

“Spaghetti Plots” Take two 500 mb contours and show all the ensemble members. At 48 hours there’s not much spread. At 360 hours it’s spaghetti!

So what good is it? If you take the ensemble mean, that forecast beats all individual member forecasts over the long term.