Lecture II-1: Data Assimilation Overview Lecture Outline: Objectives and methods of data assimilation Definitions and terminology Examples State-space.

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Lecture II-1: Data Assimilation Overview Lecture Outline: Objectives and methods of data assimilation Definitions and terminology Examples State-space formulation of the data assimilation problem State-space concepts Accounting for uncertainty Data assimilation and estimation theory The soil moisture data assimilation problem The importance of soil moisture The SGP97 field experiment Project goals and organization

What is Data Assimilation ? Data Assimilation: Data assimilation seeks to characterize the true state of an environmental system by combining information from measurements, models, and other sources. Typical measurements for hydrologic/earth science applications: Ground-based hydrologic and geological measurements (stream flow, soil moisture, soil properties, canopy properties, etc.) Ground-based meteorological measurements (precipitation, air temperature, humidity, wind speed, etc.) Remotely-sensed measurements (usually electromagnetic) which are sensitive to hydrologically relevant variables (e.g. water vapor, soil moisture, etc.) Mathematical models used for data assimilation: Models of the physical system of interest. Models of the measurement process. Probabilistic descriptions of uncertain model inputs and measurement errors. A description based on combined information should be better than one obtained from either measurements or model alone.

State estimation -- System is described in terms of state variables, which are characterized from available information Multiple data sources -- Estimates are often derived from different types of measurements (ground-based, remote sensing, etc.) measured over a range of time and space scales Spatially distributed dynamic systems -- Systems are often modeled with partial differential equations, usually nonlinear. Uncertainty -- The models used in data assimilation applications are inevitably imperfect approximations to reality, model inputs may be uncertain, and measurement errors may be important. All of these sources of uncertainty need to be considered in the data assimilation process. State variables may fluctuate over a wide range of time and space scales -- Different scales may interact (e.g. small scale variability can have large-scale consequences) The equations used to describe the system of interest are usually discretized over time and space -- Since discretization must capture a wide range of scales the resulting number of degrees of freedom (unknowns) can be very large. Key Features of Environmental Data Assimilation Problems

Real-time rainfall estimation: A Typical Environmental Data Assimilation Problem - 1 Instantaneous satellite antenna footprint Scattered metorological stations Ground radar pattern      Estimation pixels Objective: Characterize areally averaged 15 minute and hourly rainfall in each pixel of a regular grid (pixels ~10 km 2 ).

Data Sources: Multispectral satellite data provide indirect measure of rainfall over a reasonably large area (~ 100 km 2) Ground-based micro-meteorological data (~point data) Groundbased weather radar data provides another indirect measure of rainfall intensity Models: Numerical weather prediction (NWP) model which relates precipitation and other state variables to atmospheric and land surface boundary conditions Radiative transfer models used to relate satellite and radar measurements to NWP states Additional measurement models which relate micro-meteorological observations to NWP states. Probabilitistic descriptions of inputs and measurement errors A Typical Environmental Data Assimilation Problem - 2

In this problem we need to: Downscale satellite measurements (i.e. estimate rainfall at a finer spatial scale than the satellite radiobrightness measurements). Upscale radar measurements (i.e. estimate rainfall at a coarser spatial scale than the radar measurement pixels) Assimilate (or incorporate) all measurements into the NWP model (so that estimates derived from the model reflect measurements) Account for:  Subpixel variability  Model errors  Measurement errors All of this needs to be done in a systematic framework! A Typical Environmental Data Assimilation Problem - 3

State-Space Framework for Data Assimilation State-space concepts provide a convenient way to formulate data assimilation problems. Key idea is to describe system of interest in terms of following variables: Input variables -- variables which account for forcing from outside the system or system properties which do not depend on the system state. State variables -- dependent variables of differential equations used to describe the physical system of interest, also called prognostic variables. Output variables -- variables that are observed, depend on state and input variables, also called diagnostic variables. Classification of variables depends on system boundaries: Precip. Land Atmosphere Precip. Land Atmosphere System includes coupled land and atmosphere -- precipitation and evapo-transpiration are state variables System includes only land, precipitation and evapo- transpiration are input variables ET

State, Output, and Measurement Equations State equations are intended to describe how state variables evolve over space and time. These equations are usually based on conservation laws: State Eq: Output equation relates output variables to state and input variables: Output Eq: y (  ), y ( t ) State vector (e.g. soil moisture at various locations) at times  (past) and t (current) y 0 (  ) Initial state (may depend on other inputs)  Time-invariant input vector (e.g soil conductivity at various locations) u(  ) Time-dependent input vector (e.g. precipitation at various locations) w(t i ) = w i Output vector at time t i (e.g. latent heat flux at various locations). z i Measurement of w ( t i )  i Measurement error at time t i Measurement equation relates measurements to output variables: Measurement Eq:

Example: A Simple Rainfall-Runoff Model State: Q(t i ) = Streamflow Inputs: P ( t i ) = Precipitation;  = [ 1,  2, 3, 4 ]= Parameter vector Output: S ( t i ) = S i = True stage Meas: Z i = Measured stage Error:  i = Measurement error In this example, the precipitation is assumed to be perfectly known. In reality, this input will be uncertain, although a reasonable range of values may be estimated from measurements. Consider AR(1) model of streamflow, forced by precipitation. Flow is not measured but stage is measured at selected times: State Eq: Output Eq: Meas. Eq:

Rainfall-Runoff Model Response Model response to measured precipitation near Boston, USA when measured precipitation is assumed to be perfect Precip., mm/d Flow, m3/sec Stage, m Input (precip): (no error!) State (flow): Output and measurements (stage): * * * * * * State Eq: Stage measurement Time

Deriving State-space Models for Spatially Distributed Problems - 1 Spatially distributed state-space models are typically derived by discretizing partial differential equations. Example: 1D Saturated Groundwater Flow: Start with PDE derived from mass balance and Darcy’s law: Define piecewise linear approximations for all variables (the state y and the inputs S, T, and u ). Approximations are expressed in terms of values at discrete points in time (i= 1,…,I ) and space ( k = 1,…,K ): boundary conditions initial condition Input (recharge) Net inflow Storage change t1t1 tItI t2t2 y(x, t) At x = x 1 y(x, t) x1x1 xKxK x2x2 At t = t 1

Deriving State-space Models for Spatially Distributed Problems - 2 Replace derivatives by finite difference approximations at each discrete time ( t i ) and location ( x i ): Result is a set of K scalar state equations, one at each discrete spatial location (node). These may be assembled in a single matrix state equation: Similar process applies when PDE is nonlinear. y (t i ) = [y (x 1, t i ), y (x 2, t i ), …, y(x K, t i )] T

Accounting for Uncertainties/Errors Uncertainties of interest in data assimilation tend to divide into: Structural (or “bias”) errors -- The model equations do not perfectly describe the true system (because of faulty assumptions, simplifications, approximations, omissions, etc.) Input uncertainties -- The model inputs are not perfectly known. Output uncertainties -- Output measurements differ from true outputs Structural errors can sometimes be detected by examining estimates generated by the data assimilation algorithm but there is no general method for correcting such errors. where is a known nominal (measured and or assumed) precip. and P’ ( t i ) is the unknown (random) difference between the true and nominal precip. values (i.e. the precip. input error). Input uncertainties can be accounted for if we assume that the relevant true variables are random. For example, we may assume that the true precipitation P ( t i ) driving the system is a random input variable given by: Output errors are normally accounted for by including a random measurement error in the measurement equation.

Measurement error can affect observations of both model inputs and model outputs. Sources of input and output measurement error: Instrument errors (measurement device does not perfectly record variable it is meant to measure). Scale-related errors (variable measured by device is not at the same time/space scale as corresponding model variable) Types of Measurement Errors When measurement error statistics are specified both error sources should be considered Large-scale trend described by model True value Measurement Instrument error Scale-related error * * * *

Types of Data Assimilation Problems - Temporal Aspects Z i = [ z 1, z 2, …, z i ] =Set of all measurements through time t i Smoothing: characterize system over time interval t  t i Use for reanalysis of historic data tt2t2 t1t1 titi Filtering/forecasting: characterize system over time interval t  t i Use for real-time forecasting titi t2t2 t1t1 t Interpolation: no time-dependence, characterize system only at time t = t i t=t i Use for interpolation of spatial data (e.g. kriging)

Types of Data Assimilation Problems - Spatial Aspects Downscaling: Estimation area smaller than measurement area Upscaling: Estimation area larger than measurement area Estimation areas ( y 1 … y 4 ) Measurement area ( z 1 ) Measurement areas ( z 1...z 4 ) Estimation area ( y 1 ) Downscaling and upscaling are handled automatically if measurement equation is defined approriately

Characterizing System States In order to understand how each approach works we must introduce some basic concepts from probability theory. Then we can consider specific data assimilation techniques. The basic objective of data assimilation is to characterize the true state of an environmental system (at specified times, locations, and scales). How this should be done when the states are uncertain? There are two related approaches to characterization: Derive a point estimate of the true state y from available information (measurements, model, error statistics) This estimate should be “representative” of true conditions. In practice, some additional information should be provided on the range of likely values around the point estimate. Derive a range of possible values for the true state from available information. This could be conveyed in the form of a probability distribution. This approach explicitly recognizes that we cannot perfectly identify the true state. If desired, we can select a point estimate within this range (e.g. the median).

Importance of Soil Moisture Soil moisture is important because it controls the partitioning of water and energy fluxes at the land surface. This effects runoff (flooding), vegetation, chemical cycles (e.g. carbon and nitrogen), and climate. Precipitation Runoff Infiltration Evapotranspiration Soil moisture Soil moisture varies greatly over time and space. Measurements are sparse and apply only over very small scales. Soil moisture Solar Radiation Ground Heat Flux Sensible and Latent Heat Fluxes

Microwave Measurement of Soil Moisture L-band (1.4 GHz) microwave emissivity is sensitive to soil saturation in upper 5 cm. Brightness temperature decreases for wetter soils. Objective is to map soil moisture in real time by combining microwave meas. and other data with model predictions (data assimilation) saturation [-] microwave emissivity [-] sand silt clay

Case Study Area Aircraft microwave measurements SGP97 Experiment - Soil Moisture Campaign

SGP97 Experiment - Precipitation Records Julian Day 169 =18th June mm/s Precipitation at OK Mesonet Station ACME mm/s Precipitation at OK Mesonet Station ELRE mm/s Julian Day Precipitation at OK Mesonet Station MEDF

Relevant Time and Space Scales Vertical Section Soil layers differ in thickness Note large horizontal-to-vertical scale disparity 5 cm 10 cm Typical precipitation events For problems of continental scale we have ~ 10 5 est. pixels, 10 5 meas, 10 6 states, 0.8 km 4.0 km Plan View Estimation pixels (large) Microwave pixels (small) 170 = 6/19/ mm/s *** ** ****** * *** * = ESTAR observation

SGP97 Experiment - Typical ESTAR Brightness Temperature Distributions UTM, N July 9730 June June June July TBTB

Observing System Simulation Experiment (OSSE) “True” radiobrightness “Measured” radiobrightness “True” soil moisture and temperature Mean soil properties and land use Land surface model (NOAH) Mean initial conditions Mean land-atmosphere boundary fluxes Radiative transfer model (RTM) Random forcing error Random initial condition errors Random meas. error Data assimilation algorithm (EnKF) Estimated microwave radiobrightness and soil moisture Soil properties and land use, mean fluxes and initial conditions, error covariances Estimation error OSSE generates synthetic measurements which are then processed by the data assimilation algorithm. These measurements reflect the effect of random model and measurement errors. Performance can be measured in terms of estimation error. Random property errors

SGP97 Project Task Summaries The summer school project uses an OSSE to investigate a particular data assimilation algorithm (an ensemble Kalman filter) and to evaluate tradeoffs for a soil moisture satellite mission. The OSSE relies on data from the SGP97 experiment. The following three problems will be examined: Algorithm convergence properties -- How is convergence affected by the number of uncertain variables (error sources) included in the data assimilation algorithm? Identification of error statistics -- Is it possible to identify the statistical properties of model and measurement errors by observing the performance of the data assimilation algorithm? Mission design -- What are the best choices for satellite mission specifications such as revisit time, resolution, coverage, and accuracy? Would performance be improved by augmenting L-band microwave measurements with measurements of skin temperature?