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Introduction to the NOAH Land Surface

Model

N: National Centers for Environmental Prediction (NCEP)

O: Oregon State University (Dept of Atmospheric Sciences)

A: Air Force (both AFWA and AFRL - formerly AFGL, PL)

H: Hydrologic Research Lab - NWS (now Office of Hydrologic Dev –

OHD)





Outline



1. What is an LSM?

2. What is the NOAH LSM?

3. NOAH @ UT



Zong-Liang Yang





Prepared for Surface Water Hydrology

February 24, 2005

Outline





1. What is an LSM? (29 slides)



2. What is the NOAH LSM? (13

slides)



3. NOAH @ UT (14 slides)

Computer Code to Model Land Surface

Processes

• Exchanges with the atmosphere

– Momentum

– Energy

– Vapor

– Trace gases/dust/aerosols

• Exchanges with the oceans

– Runoff

– Sediments / nitrogen

• Land-memory processes

– Topography

– Snow cover

– Soil moisture

– Vegetation

• Human activities

– Land use (agriculture, deforestation, urbanization…)

– Inland water pollution

Earth’s Radiation Budget









Shortwave: Earth reflects 30% directly back to space, absorbs about

20% in the atmosphere, and absorbs about 50% at the surface.

Longwave: Greenhouse effects keep the surface warm.

Turbulent heat fluxes: sensible and latent heat keeps the surface cool.

Land-atmosphere coupling strength (JJA)



Koster et al.,

2004

(Science)









Hot spots: initial soil moisture impacts

rainfall forecasts

Locations for the routine monitoring of

soil moisture

Interpretations

Rainfall in a region depends on atmospheric moisture transport

from upwind areas and local evapotranspiration.

 Moisture transport depends on large-scale circulations

 Evapotranspiration depends on vegetation, soil, and

weather conditions



L



Qa In Sa Qa Out







Pm Pa

E

Ql

Do Land Surface Processes Matter to

Climate Prediction?

What Are Land Surface Processes

• Land surface consists of

– urban areas, soil, vegetation, snow, topography, inland water (lake, river)











• Land surface processes describe

– exchanges of momentum, energy, water vapor, and other trace gases between

land surface and the overlying atmosphere

– states of land surface (e.g., soil moisture, soil temperature, canopy

temperature, snow water equivalent)

– characteristics of land surface (e.g., roughness, albedo, emissivity, soil

texture, vegetation type, cover extent, leaf area index, and seasonality)

What Are Land Surface Processes









• Land surface processes function as

– lower boundary condition in Atmospheric Models

• Atmospheric Boundary Layer Simulation Climate Simulation

• Numerical Weather Prediction 4-D Data Assimilation

– upper boundary condition in Hydrological Models

• Water Resources Estimation; Crop Water Use; Runoff Simulation

– interface for coupled Atmospheric/Hydrological/Ecological Models

Land Surface Models (LSMs)

• Computer code describing land surface processes (also called

LSSs, LSPs, SVATs)

– FORTRAN, C, C++, PASCAL, … ...

– Tens to thousands of lines

• There are a huge number of LSMs (100+ examples in literature)

– many are just “research models’’, local-scale oriented, with specific

process emphasis

– up to ~100 canopy, ~100 soil, ~100 snow, even ~100 atmosphere

layers!

• LSMs in GCMs and Hydrological Models are less diverse

– one dimensional, with 1-2 canopy, 1-10 soil, 1-10 snow layers

– three general classes

• “Bucket” Models (no vegetation canopy)

• “Micrometeorological” Models (detailed soil/snow/canopy

processes)

• “Intermediate” Models (some soil/snow/canopy features)

Land Surface Models (LSMs)

• Four basic requirements

– frequently-sampled (hourly or sub-hourly) weather “data” to

“drive” LSMs

• precipitation (rate; coverage, large-scale/convective in GCMs)

• radiation (shortwave, longwave)

• temperature

• wind components (u, v)

• specific humidity

• surface pressure

– initialization of state variables

• soil moisture (liquid, frozen) deep soil temperature

– specification of surface characteristics

• albedo roughness vegetation cover

– validation of simulations of state variables and fluxes

• soil moisture sensible/latent heat fluxes

Land Surface Models (LSMs)

• Minimum Requirement is to describe:

– bulk momentum exchange (roughness length, zero displacement height)

– exchange of radiation for:

• solar radiation (0-3 micrometers): albedo

• long-wave (3-100 micrometers): surface emissivity

– partition of radiant energy between soil heat, latent heat and sensible heat, along with its

relationship to water availability

• Micrometeorological Models typically

– have 20-50+ parameters

– require to prescribe or predefine them before running the models

• Research Issues

– Obtaining and applying relevant “pure biome” data to test or calibrate LSMs

– Dealing with spatial/temporal heterogeneity

• defining area-average parameters; scaling up surface parameters from local to regional

• defining space-time structure of atmospheric inputs

– Making best use of remote sensing data for initialization, specification and validation

– Improving key processes

• Snow/Frozen soil

• Runoff generation/routing

• “Greening” of LSMs (carbon balance and vegetation dynamics)

Land Surface Models (LSMs)

• Project for Intercomparison of Land-surface Parameterization Schemes (PILPS)

– is helping define needs, understanding processes, from sensitivity tests and

field data to coupled modeling

– ongoing project (4 phases, starting from 1992, 20-30 LSMs participating)

• Phase 1: GCM-generated forcing data for three “biomes”:

– models’ response time to initialization of soil moisture

– sensitivity experiments with albedo, canopy/soil water storage,

aerodynamic resistances

• Phase 2 : observed data

– 2(a) Cabauw, Netherlands (grass; 1-year)

– 2(b) HAPEX-MOBILHY, France (crop; 1-year)

– 2(c ) Red-Arkansas River Basin, USA (mixed land covers; 10-year)

– 2(d) Valdai, Russia (snow/frozen soil; 18-year)

– 2(e) Sweden Torne/Kalix Basins, 58000 sq. km, 218 grids, 1979-98

• Phase 3: joint with Atmospheric Model Intercomparison Project -AMIP

• Phase 4: selected LSMs coupled to one host model

– Regional Model Global Model Coupling Strategy

Simple “Bucket” LSMs

• “Bucket” Models” first in hydrological models, later in GCMs

– “Bucket” is filled by precipitation, and emptied by evaporation

– Runoff occurs when “Bucket” is full (soil water level exceeds the field capacity)

– Evaporation is based on soil-water limited “Potential Evaporation”

– The limiting factor is a linear function of soil moisture

• In original “bare soil” form, e.g., Manabe (1969) include no vegetation so

specify (fixed) parameter values for

– albedo (Solar radiation)

– surface emissivity (Longwave radiation)

– roughness length (Momentum exchange)

– soil thermal properties (Soil heat storage)

– field capacity (15 cm) for all land points (Soil hydrology)

– snow areal coverage (covers 100% gridbox) (Snow energy/water budgets)

• Some variants of “Bucket” Models

– allowing leakage by implicit transpiration or gravitational drainage

– including surface resistance in evaporation formula

– extending to 2 connected “Buckets”: Deardorff (1977) includes a thin surface layer

and a deep bulk layer

Micrometeorological Model-Based LSMs

• Micrometeorological Model-Based LSMs are

– more complex than bucket models

– less complex than “multi-layer” or “second order closure” canopy models





• Best known examples:

– “Biosphere-Atmosphere Transfer Scheme (BATS)”

– “Simple Biosphere Model (SiB)”

– SiB more complex (not at run time) some whole-canopy parameters from “pre-

processing”, one calculation, prior to actual model run





• Five components of radiation exchange considered in BATS and SiB

– Direct beam photosynthetically active radiation (PAR) (4.0 micrometers)

Micrometeorological Model-Based LSMs

Biosphere-Atmosphere

BATS Transfer Scheme

Micrometeorological Model-Based LSMs

• “Two-Stream Approximation” are used to calculate solar radiation exchange

in SiB for both PAR and NIR, diffuse and direct beam components from

dI 

  [1  (1  )  ]I       I       K   0  e  KL

dL

dI 

  [1  (1  )  ]I       I       K  (1   0 )  e  KL

dL

divergence forward scatter back scatter direct beam scatter

I , I  normalized upward / downward diffuse beam components

,  0 diffuse / direct " on scatter"parameters for beam

 ts

scattering coefficien for " photoelements"

 average inverse optical depth / unit leaf area

K direct beam optical depth / unit leaf area

• Can obtain single-scattering albedo, diffuse fluxes within canopy (for stomatal

resistances) and at soil surface, and total albedo of the vegetated surface

• Vegetation albedo depends on specifications of

– leaf area index scattering coefficients of leaves and soil

– leaf angle distribution function angle of the direct-beam incident radiation

– proportion of different components of the incident radiation

• Not suitable for application over heterogeneous or ‘clumpy’ canopies

(coniferous forests); require three-dimensional radiation models

• BATS prescribes vegetation albedo; 4-layer model for stomata

Micrometeorological Model-Based LSMs

• Thermal Radiation from surface is computed from “Stefan-Boltzmann” law:



L out    Ts4

where Ts is an " appropriat ely defined" surface temperature





• Whole-canopy turbulent transfer is important for exchange of momentum,

heat and mass (water vapor, trace gases)

– is a complex process

– requires higher-order closure models, Markov-chain numerical simulations, or

eddy simulation techniques

– simpler treatments in LSMs because of

• computational expense and storage requirements

• aerodynamic resistance roughly an order of magnitude smaller than aerodynamic

resistance

– z 0 and d : prescribed for BATS (and most other models); aerodynamic resistances

from curve-fitting functions, iteration for nonneutral corrections

– z 0 and d : calculated in SiB: pre-processed from canopy morphology using a “K-

Theory” equivalent of Shaw-Pereira (1982); aerodynamic resistances from canopy

morphology using “K-Theory”, iteration for nonneutral corrections

Micrometeorological Model-Based LSMs

• Canopy interactions described by a “big leaf” model in BATS and SiB and

others [SiB allows an “understorey”; SiB2 allows only one layer]

• Dry canopy parameterized through surface resistance based on the model of

Jarvis (1976). For a single leaf:

1

 gs  g0 gC g R g D gT g M

rs

rs - leaf stomatal resistance, sm-1

g s - leaf stomatal conductance, ms -1

g 0 - constant depending on vegetat ion type

g C - canopy cover factor

g R - radiation " stress function"

g D - vapor pressure deficit " stress function"

g T - temperature " stress function"

g M - soil moisture " stress function"



• Canopy surface resistance is obtained by integrating above equation over leaf

angle and canopy depth. This integration and those dependencies are “coded”

in different forms in BATS and SiB and many other models.

Micrometeorological Model-Based LSMs

• Different forms of coding for the integration:

– In SiB, an analytical integration is performed by using the Goudriaan formulation

for some regular leaf angle distribution

– In BATS, the integration is done by using a 4-layer numerical scheme for canopy





• Different forms of coding for the stress factors:

– primarily determined from curves fits to data (e.g. Jarvis, 1976), but

– g M in SiB was a linear function of the leaf water potential, which, in turn, was

determined by a catenary model of water flow from root zone to leaf

– g M in BATS, was introduced only when the atmospheric demand exceeds the water

supply from the soil through roots

– gT in SiB taken as a smooth curve varying from zero at some minimum

temperature around freezing to unity at an optimum temperature between 25

degree C and 35 degree C, depending on species, and dropping sharply down to

zero at 45 degree C to 55 degree C

– gT in BATS parameterized as a quadratic function of canopy temperature,

varying from 0 at freezing point to unity at 25 degree C, and remaining at unity

when temperature is greater than 25 degree C

Micrometeorological Model-Based LSMs

• Calibration of stomatal resistance largely speculative: guessed from single leaf

data, but occasional “Calibration Data Sets” available e.g. for forest,

Shuttleworth (1989); Gash et al. (1996)

• Wet Canopy Description is a simplified “Rutter” Model: S, proportional to

Leaf Area Index ~[(0.1-0.25) x LAI] (mm)

• Both BATS and SiB allow partially wet canopy



E  E  E

Total Transpirat ion Intercepted Rain

 [1  f (C / S)] E rST  finite

PM  f(C/S) E rST  0

PM







dC

 g(F, LAI ) P  f (C / S) E rST  0  D

PM canopy wat er balance equation

dt

D  0, when C  S whe re D is canopy drainage rate

D  P, when C  S where P is precipitation rate

a c p D

 (R n  G ) 

ra

E  (whole - canopy) Penman - Monteith Equation

  rST 

 r 

   1   

  a 

Micrometeorological Model-Based LSMs

• “Plot-scale” calibration of interception models adequate, given tuning of S

against LAI

• BATS/SiB have simple “vertical hydrology”: soil water diffuses vertically

through 2-3 layers, but is ultimately inaccessible by draining from lowest layer

• Global Distributions of different land classes required, BATS has 15, SiB has

12, with parameters defined for each class:

Calibration of these Parameters Remains Speculative

“Intermediate” LSMs

• “Intermediate” LSMs trade process detail for simplicity, justified by still

speculative need for more complete process models, and their poor calibration

• Often have distributed vegetation class, but simpler physics: e.g.

– UKMO simple canopy model

– French ISBA simple soil model

– Simple SiB Simplified empirical parameterization fitted to time

consuming, SiB-calculated functions

– “Super Bucket” basic bucket, with “reference crop” estimates instead of

“potential” rate(+Several others)

• Permissible, practical alternative, pending evidence of need for more complex

micrometeorological models

LSMs Calibration Issues

• Primary LSM short-coming is lack of reliable calibration: 3 needs

– Obtaining and applying relevant “pure biome” data

– Understanding how to define area-average parameters

– Making best use of Remote Sensing Data

• Single Biome Calibration

– Needs:

• sets of continuous “driving variables” for whole years

(frequently-sampled, near-surface, equivalent to GCM)

• some substantial periods with measured exchanged fluxes

(preferably for several seasons, all exchanges, time scales)

– Some biomes done or in-hand

• Rain forest (ARME, ABRACOS)

• Prairie grass (FIFE)

• Boreal forest (BOREAS)

• Sonora Desert, Tucson, Arizona (Example of multi-objective

calibration)

LSMs Calibration Issues: Area-average

• Defining Area-average LSM parameters is active research which involves data collection,

analysis and coupled models for mixed land covers, and for selected regions

– mixed vegetation cover and/or soils uneven precipitation sloping terrain

• Examples:

– Hydrologic-Atmospheric Pilot Experiment (HAPEX) - S.W. France, 1986, (mixed temperate;

agriculture, forest)

– First ISLSCP Field Experiment (FIFE) - Kansas, 1987,9 (tall prairie grass)

– HAPEX-Sahel - Niger, 1992, (semi-arid Sahelian savannah-across rainfall gradient)

– BOREAS - Canada, 1993,4, Boreal Forest

– AMAZONIA (LBA) - S. America, 1997,8 - Amazonian land covers

– GEWEX

LSMs Calibration Issues: Atmospheric Data

• Calibration or model development depends on atmospheric input data

• Runoff estimation error is determined by the accuracy of the precipitation

forcing as measured by the density of rain gauge

Micrometeorological Model-Based LSMs

• New developments: The Greening of LSMs (improved canopy physiology)

– enzyme kinetics-electron transport model (Farquhar et al., 1980), relating leaf

photosynthetic rate to PAR, leaf temperature, leaf internal carbon dioxide

concentration, and leaf carboxylase concentration

– photosynthesis modeled as the minimum of three potential capacities to fix carbon

A g  min (J e , J c , J s )

A g - gross photosynthesis rate per unit leaf, mol CO 2 m - 2 s -1

J e - light - limited rate of photosynthesis per unit leaf, mol CO 2 m - 2 s -1

J c - Rubisco - limited rate of photosynthesis per unit leaf, mol CO 2 m - 2 s -1

J s - triose phosphate utilization - limited rate of photosynthesis per unit leaf, mol CO 2 m - 2 s -1

g s, H 2 O

A n  A g  R leaf  (C a  Cs ) g b, CO 2  (Cs  Ci )

1.6

A n - net leaf assimilation rate, mol CO 2 m - 2 s -1

R leaf - leaf maintenanc e respiration, mol CO 2 m - 2 s -1

C a - CO 2 concentration (mol/mol)in the atmosphere

Cs - CO 2 concentration (mol/mol)at the leaf surface

Ci - CO 2 concentration (mol/mol)in the intercellular air spaces of the leaf

g b, CO 2 - boundary layer conductance for CO 2 (mol CO 2 m - 2 s -1 )

1.6 - factor to account for different diffusivities of CO 2 and H 2 O

Micrometeorological Model-Based LSMs

• New developments: The Greening of LSMs (improved canopy physiology)

– Ball-Berry model of stomatal conductance (Ball et al., 1986): robust semi-empirical

method, relating leaf stomatal conductance to photosynthetic rate and

environmental parameters

m An

gs  hs  b

Cs

m, b - constants 9 and 0.01, respectively

h s - relative humidity on leaf surface

A n - net leaf assimilation rate, mol CO 2 m - 2 s -1

p CO 2 [Pa]

Cs - CO 2 concentration (mol/mol)at the leaf surface, or

p [Pa]

– Other forms: Leuning (1995), Foley et al. (1996), Dickinson et al. (1998): using

vapor pressure deficit instead of relative humidity



m An

gs  b

D

(Cs  * )(1  s )

Do

Ds - water vap or mole fraction difference between the leaf and the air (mol/mol)

D o - referencevalue (mol/mol)

Ds / D o - written as (1  0.05 VPD) as in Dickinson et al. (1998);VPD in Pa

Micrometeorological Model-Based LSMs

• New developments: The Greening of LSMs (improved

canopy physiology)



– C3 (all trees and many herbaceous) and C4 (warm

grasses) plants are similarly modeled as the minimum

of three potential capacities to fix carbon, but

– The three potential capacities are defined differently for

C3 and C4 plants

– The parameters are different for both types of plants

– The Ball-Berry model of stomatal conductance replaces

all the terms in the Jarvis model except for the soil

water stress term

Micrometeorological Model-Based LSMs

• New developments: The Greening of LSMs (improved vegetation phenology)

– Traditionally, annual cycle in areal vegetation coverage and leaf area index

prescribed as a quadratic function of deep soil temperature

– Some recent attempts: relating vegetation to climate using empirical rules

involving monthly or annual mean temperature and precipitation

– New developments:

• simple rule-based formulation to describe behavior of winter-deciduous

and drought-deciduous plants (Foley et al., 1996), using

– daily average temperature, yearly carbon balance

– competition between trees and grasses (through allocation/shading)

• interactive canopy model (Dickinson et al., 1998)

– short time-scale leaf dynamics

– consistent treatment of stomatal conductance and assimilation

– assimilated carbon allocated into leaf, fine root and wood

– soil carbon model

» fast pool: leaf/root turnover (senescence, herbivory or

mechanical), leaf loss (cold and drought stress), soil respiration

» slow pool: inert for seasonal variations

Recent LSM Developments

• Improved understanding in physical hydrology

– Snow hydrology

– Topographic controls on soil moisture/runoff

• Enhanced linkage with biogeochemistry/ecology

– Carbon and nitrogen

– Vegetation growth/competition

• Closed water cycle through river routing

• Advanced techniques for using remotely-sensed

land parameters

• Extended field datasets and model calibration

Outline





1. What is an LSM? (29 slides)



2. What is the NOAH LSM? (13

slides)



3. NOAH @ UT (14 slides)

Land-Atmosphere Interaction

NOAH LSM Development Team

NCEP/EMC: NCEP Environmental Modeling Center (EMC)

(Mitchell, Chen, Ek, Lin, Marshall, Janjic, Manikin,

Lohmann, Grunmann, Pan)



OSU: Oregon State University

(Mahrt, Pan, Ek, Kim, Rusher)



HL: NWS Hydrology Lab - formerly Office of Hydrology

(Schaake, Koren, Duan)



AFWA: Air Force Weather Agency - formerly AFGWC

(Moore, Mitchell, Gayno)



AFRL: Air Force Research Lab - formerly AFGL and PL

(Mitchell, Hahn, Chang, Yang)

NOAH LSM Evaluation Team

E.H. Berbery and Rasmusson: U. Maryland (ARM/CART)



C. Marshall and Crawford U. Oklahoma (OU Mesonet)



I. Yucel and Shuttleworth: U. Arizona (ARM/CART,

AZNET)

A.K. Betts: Atmospheric Res Inc (ISLSCP/FIFE)



C.D. Peters-Lidard, Wood Princeton U. (TOPLATS

extensions)

L. Hinkelman and Ackerman: Penn State U. (ARM/CART)



T.H. Chen, W. Qu,

Henderson-Sellers, et al. RMIT (PILPS-2a)



E. Wood, Lettenmaier,

Liang, Lohmann: Princeton U. (PILPS-2c)



A. Schlosser, A.G. Slater,

A. Robock, et al. U. Maryland (PILPS-2d)



R. Angevine NOAA/AL (Flatland Exp)

References

1. User’s Guide, Public Release Version 2.2, Last Updated 25 June 2001,

filename README_2.2.doc at

ftp://ftp.ncep.noaa.gov/pub/gcp/ldas/noahlsm/ver_2.2



2. Author / Point of Contact: Kenneth.Mitchell@noaa.gov (NCEP/EMC), phone

301-763-8000



3.









PROGRAM HISTORY LOG



01 Mar 99: Ver_1.0

08 Mar 99: Ver_1.1

27 Jul 99: Ver_2.0

23 Oct 00: Ver_2.1

25 Mar 01: Ver_2.2

Timeline of NOAH LSM Evolution

Atmospheric Forcing Variables



Air temperature at height Z above ground

Air humidity at height Z above ground

Surface pressure at height Z above ground

Wind speed at height Z above ground

Surface downward longwave radiation

Surface downward solar radiation

Precipitation

Initial Conditions



1. SMC: total volumetric soil moisture (liquid & frozen) in each soil

layer



2. SH2O: liquid volumetric soil moisture in each soil layer



3. STC: temperature in each soil layer



4. T1: skin temperature



5. CMC: canopy water content



6. SNOWH: snow depth



7. SNEQV: water-equivalent snow depth

Model Parameters

There are five kinds of land-surface parameters, reviewed in order below.



a) single universal values



b) values dependent on the soil class index (default categories are 1–9)



c) values dependent on the vegetation class index (default categories are 1–

13)



d) values dependent on the surface slope index (default categories are 1–7)



e) parameters specifying the numbers of vegetation, soil, and slope classes

Model Soil Parameters

SMCMAX: maximum volumetric soil moisture (porosity)



SMCREF: soil moisture threshold for onset of some transpiration stress



SMCWLT: soil moisture wilting point at which transpiration ceases



SMCDRY: top layer soil moisture threshold at which direct evaporation

from soil ceases



DKSAT: saturated soil hydraulic conductivity



PSISAT: saturated soil matric potential



B: the “b” parameter in hydraulic functions



DWSAT: saturated soil water diffusivity



QUARTZ: quartz content, used to compute soil thermal diffusivity



FRZFACT: a parameter used with FRZK to compute the value of

parameter FRZX

Model Vegetation Parameters

Z0 (m): roughness length

RCMIN (s/m) : minimal stomatal resistance used in canopy resistance

of routine CANRES

RGL: radiation stress parameter used in F1 term in canopy

resistance of routine CANRES

HS: coefficient used in vapor pressure deficit term F2 in

canopy resistance of routine CANRES

LAI: presently set to universal value of 3.0 across all

vegetation classes

Note: seasonality of vegetation greenness carried by fraction of green

vegetation (SHDFAC)



NROOT: number of soil layers from top down reached by roots



SNUP: the water-equivalent snowdepth upper threshold at

which

1) 100 percent snow cover is achieved for given veg class

2) maximum snow albedo is achieved for given veg class

Forecasts of Dew Point Temperature



Old version









New version

Forecasts of Dew Point Temperature

Outline





1. What is an LSM? (29 slides)



2. What is the NOAH LSM? (13

slides)



3. NOAH @ UT (14 slides)

NOAH @ UT



• To put a dynamic vegetation component in the NOAH

LSM

– understand the feedback mechanisms between precipitation,

soil moisture, and vegetation dynamics

– To improve weather and climate forecasts on time scales

from hourly to seasonal

– To interpret and transfer weather and climate forecasts for

water resources management applications





• To put a biogenic VOC emission component in the

NOAH LSM

– understand the impacts of climate change and land use/land

cover change on BVOC emissions and the formation of near

ground ozone

The Modeling Domains: Multiple interactive nesting grids:

Weather Research and Forecast

(WRF) Model, version 2.02

(http://www.wrf-model.org/) 30 km grid; 31 Levels

Temperature, wind, humidity,

The model is developed by NCAR,

pressure predicted

NCEP and Universities.









3-10 km grid; 31

Levels

Temperature, wind,

humidity, pressure

predicted

90 km grid; 31 Levels

Temperature, wind, humidity, pressure prescribed

from large-scale analyses

Vegetation Distribution in the Model

Other Land Data:

Vegetation

LAI

Albedo

Roughness length

Stomatal parameters

Soil

Topography



Validation:

Weather stations

Hydrologic stations

Remote sensing

Field data

Stomatal Conductance in NOAH

• Transpiration 1

 gs  g0 gC g R g D gT g M

parameterized through rs

surface conductance

based on the model of rs - leaf stomatal resistance, sm-1

Jarvis (1976). For a

g s - leaf stomatal conductance, ms -1

single leaf:

g 0 - constant depending on vegetat ion type

g C - canopy cover factor

g R - radiation " stress function"

g D - vapor pressure deficit " stress function"

g T - temperature " stress function"

g M - soil moisture " stress function"

NOAH with Modifications (1)

The ability of roots to uptake soil water depends on the availability

of soil water.



In NOAH, this is a linear function, which may work if soil is near

saturated.



We make it a step-function, guided by observations.



We call the experiment NOAH SWF (soil water factor).

Role of Land Surface Processes in Modulating NAMS Rainfall



OBS WRF/SLAB WRF/NOAH WRF/NOAH SWF





JUN









JUL









AUG









WRF/SLAB fails to WRF/NOAH fails to WRF/NOAH-SWF

produce rainfall for capture rainfall in captures rainfall in

June thru August. August. August.

NOAH with Modifications (2)



NOAH prescribes fractional green vegetation.



In the real world, vegetation growth depends on

precipitation, temperature, nutrients, and others.



This can be modeled by



1) Relating stomatal conductance to photosynthesis &

environmental conditions, and

2) Allocating assimilated carbon to leaves, stem, wood,

and roots.

Leaf Anatomy









Stomate

(pl. stomata)

Carbon and Water



• Plants eat CO2 for

a living

• They open their

stomata to let

CO2 in

• Water gets out as

an (unfortunate?)

consequence

• For every CO2

molecule fixed

about 400 H2O

molecules are lost

Photosynthesis and Conductance

Stomatal conductance is linearly related to photosynthesis:



(The “Ball-Berry-Collatz” parameterization)



photosynthesis RH at leaf sfc



stomatal An hs

conductance gs  m pb

cs

CO2 at leaf sfc







Photosynthesis is controlled by three limitations

(The Farquahar-Berry model):



An  min( AC , AL , AS )  Rd



Enzyme kinetics Light Starch

(“rubisco”)

Photosynthesis and Carbon Allocation

Comparison of Observed & Simulated Rainfall

OBS WRF/NOAH SWF WRF/NOAH DV



JUN









JUL









AUG

Conclusions

1) Strong sensitivity to land surface processes

1) SLAB (without vegetation) fails to simulate the monsoon

rainfall in all months

2) NOAH (with prescribed vegetation) is better, but under-

estimates the August rainfall

3) NOAH (with improved root water uptake and response) is even

better

4) NOAH (with improved carbon and water coupling and leaf’s

dynamic response to rainfall) gives the best overall simulation

of the warm season rainfall

1) In the southern monsoon regions

2) In the southern Great Plains.



2) Dynamic vegetation has the largest impacts on the simulation of

rainfall in the SGP, which is the area that shows the largest

memory to soil moisture conditions.

PHYSICAL CLIMATOLOGY

GEO 387H

TTh 9:30-11:00 Fall 2005

www.geo.utexas.edu/courses/

387h/indexPHY.htm

Taught by

Dr. Liang Yang

Department of Geological Sciences









This course will cover the basics of a broad range of physical processes having an impact on precipitation and

evapotranspiration at the earth's surface. Local processes include thermodynamics, cloud microphysics, net

radiation at the surface, fluxes of heat and moisture into the soil and the atmospheric boundary layer, and the

effects of a vegetation canopy. Large-scale interactions between atmosphere, ocean, soil moisture, snow, ice,

biosphere, and lithosphere are reviewed in the context of potential local/large-scale transports. Methods for

measuring and estimating precipitation and evapotranspiration are described, including the sophisticated

models known as GCMs (General Circulation Models) and SVATS (Soil-Vegetation-Atmosphere Transfer

Schemes). Some basic programming/modeling techniques will be covered.

For both Geoscience and non-Geoscience graduate students.



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