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    International Journal of Applied Earth Observation and Geoinformation 17 (2012) 8593

    Contents lists available at SciVerse ScienceDirect

    InternationalJournal ofApplied Earth Observation andGeoinformation

    journal homepage: www.elsevier .com/ locate / jag

    Estimation ofevapotranspiration in an arid region by remote sensingA case

    study in the middle reaches ofthe Heihe River Basin

    Xingmin Li a,b,, Ling Lu a, Wenfeng Yang c, Guodong Cheng a

    a Cold andArid Regions Environmental and Engineering Research Institute, Chinese Academy of Sciences,730000 Lanzhou, Chinab Shaanxi Institute of Meteorological Sciences, 710014 Xian, Chinac Shaanxi Meteorological Observatory, 710014 Xian, China

    a r t i c l e i n f o

    Article history:

    Received 8 November 2010

    Accepted 7 September 2011

    Keywords:

    Heihe River Basin

    Evapotranspiration

    Remote sensing

    Evaporative fraction

    a b s t r a c t

    Estimating surface evapotranspiration is extremely important for the study of water resources in arid

    regions. Data from the National Oceanic and Atmospheric Administrations Advanced Very High Reso-

    lution Radiometer (NOAA/AVHRR), meteorological observations and data obtained from the Watershed

    Allied Telemetry Experimental Research (WATER) project in 2008 are applied to the evaporative frac-

    tion model to estimate evapotranspiration over the Heihe River Basin. The calculation method for the

    parameters used in the model and the evapotranspiration estimation results are analyzed and evaluated.

    The results observed within the oasis and the banks of the river suggest that more evapotranspiration

    occurs in the inland river basin in the arid region from May to September. Evapotranspiration values

    for the oasis, where the land surface types and vegetations are highly variable, are relatively small and

    heterogeneous. In the Gobi desert and other deserts with little vegetation, evapotranspiration remains

    at its lowest level during this period. These results reinforce the conclusion that rational utilization of

    water resources in the oasis is essential to manage the water resources in the inland river basin. In the

    remote sensing-based evapotranspiration model, the accuracy ofthe parameter estimate directly affects

    the accuracy ofthe evapotranspirationresults; more accurate parameter values yield more precise values

    for evapotranspiration. However, when using the evaporative fraction to estimate regional evapotranspi-

    ration, better calculation results can be achieved only ifevaporative fraction is constant in the daytime.

    2011 Elsevier B.V. All rights reserved.

    1. Introduction

    Evapotranspiration is both a heat balance component and a key

    component of the water budget. Because the inputs and outputs

    of surface heat and water primarily determine the components

    and evolution of the geographic environment, understanding evap-

    otranspiration can significantly improve the modeling of energy

    balance and water cycle. For research related to global climate

    change and land surface processes, evapotranspiration data are

    required to calculate water use efficiency, irrigation and water

    resource distribution; it is also important for the study of cli-mate change patterns, atmospheric circulation modes, carbon

    balance and related land surface processes and boundary condi-

    tions (Avissar, 1998; Verstraeten et al., 2005).

    For practical applications, it is typically necessary to know both

    the distribution of evapotranspiration and the general water con-

    sumption trend within the region. Therefore, estimating regional

    Corresponding author at: Shaanxi Institute of Meteorological Sciences, 710014

    Xian, China. Tel.: +86 29 81619291.

    E-mail address: [email protected](X.Li).

    evapotranspiration is a key issue. Traditional methods like refer-

    ence crop evapotranspiration assume homogeneous land coverage

    and structure, but these conditions are difficult to meet for large

    regions. In recent years, because of the rapid developments in

    remote sensing technology, the spatial, temporal and spectral

    resolution of satellite data is continuously improving. Surface

    characteristics, such as albedo, vegetation coverage, land surface

    temperature, and leaf area index, can be retrieved from visible,

    near-infrared, thermal infrared and other wave bands. These data

    provide a basis for estimating evapotranspiration from farmland

    and other regions and have attracted widespread attention for theuse of remotesensing technologies to study regional evapotranspi-

    ration (Li et al., 2009a).

    Evapotranspiration with remote sensing technology has been

    studied thoroughly in China; for example, the Surface Energy

    Balance Algorithm for Land (SEBAL) model (Bastiaanssen et al.,

    1998a,b) and the Surface Energy Balance System (SEBS) model (Su,

    2002) are used to calculate evapotranspiration. Pang et al. (2007)

    developed evapotranspiration estimation models for vegetation

    coverage and for bare soil that are based on the SEBAL model.

    He et al. (2007) improved the parameters of the SEBS model and

    estimated surface energy flux from the topographical features of

    0303-2434/$ seefrontmatter 2011 Elsevier B.V. All rightsreserved.

    doi:10.1016/j.jag.2011.09.008

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    86 X. Li et al. / International Journal of Applied Earth Observation and Geoinformation 17 (2012) 8593

    the Huang-Huai region. Ma et al. (2010) studied energy flux on a

    heterogeneous land surface. Xin and Liu (2010) used assumptions

    to simplify the two-source model. Zhang et al. (2003) proposed an

    evaporation model based on differential thermal inertia by which

    evaporation (latent heat flux) can be determined forbare soil based

    on only remotely sensedinformation. This work inspired new ideas

    for estimating evapotranspiration by remote sensing techniques,

    and integrating these methods with soil-vegetation-atmosphere

    models (Liu et al., 2007) is also progressing.

    The Heihe River Basin, the second largest inland river basin of

    China, is commonly used as a case study area for estimating evap-

    otranspiration for a heterogeneous land surface in an arid region.

    Many studies have focused on evapotranspiration across the Heihe

    RiverBasin. Ma et al.(1997, 2004) implemented a parameterization

    scheme for regional energy flux on a heterogeneous land surface

    with Landsat TM data and then validated the scheme with obser-

    vations from the Heihe River Basin Field Experiment (HEIFE). Guo

    (2003) estimated evapotranspiration over the Heihe River Basin

    by using NOAA/AVHRR data to retrieve the typical surface parame-

    ters basedon PriestleyTaylor formula. Zhang et al.(2004) usedthe

    SEBAL model to deduce the spatial distributions of surface energy

    fluxesincludingevapotranspirationfrom TM images overthe Heihe

    River Basin. In addition, some researchers (Wu et al., 2007) inves-

    tigated the receipt and expenditure of radiation by farmland in the

    Heihe River Basin based on the reference crop evapotranspiration

    method. In contrast, this paper studies and estimates evapotran-

    spiration over the midstream of the Heihe River by the evaporative

    fraction method and verifies the calculated parameters and model

    results by comparing the results with data from the Watershed

    Allied Telemetry Experimental Research (WATER) (Li et al., 2009b,

    2011).

    2. Dataandmethod

    2.1. Study area

    The middle section of the Heihe River is selected as thestudy area in this paper to estimate evapotranspiration by the

    remote sensing model. With an area about 128,000 km2, the Heihe

    River Basin is the second largest inland river basin in north-

    western China; it is located in the middle of the Hexi Corridor

    between 964210200E and 37414242N. The oasis is pri-

    marily surrounded by the Gobi desert, but the landscape includes

    heterogeneously distributed farmland, forest and residential areas

    inside and on the margins of the oasis. The climate is a typical

    temperatearid environment with low precipitation andhigh evap-

    oration.

    2.2. Data

    2.2.1. NOAA/AVHRR dataThe Advanced Very High Resolution Radiometer (AVHRR) has

    five channels: one visible (VIS), one near-infrared (NIR), one

    infrared (IR) and two thermal infrared (TIR) channels. The tem-

    poral resolution is one day and the spatial resolution at nadir

    is 1.1 km. This paper uses NOAA/AVHRR data received by the

    Gausu Provincial Meteorological Bureau on May 5, June 3, August

    2 and 25, and September 30, 2008. The overpasses time of satel-

    lite NOAA-18 is between 14:00 pm and 16:00 pm local time.

    Polar Orbit Meteorological Satellite Receiving and Processing Sys-

    tem software, which was developed by the National Satellite

    Meteorological Center of the China Meteorological Administra-

    tion (CMA), was used to process the received real-time data.

    After geometric and atmospheric corrections and other prepro-

    cessing such as data format conversion, the data were then

    been input into the Environment for Visualizing Images (ENVI)

    software (http://www.ittvis.com/ProductServices/ENVI.aspx) for

    further analysis.

    2.2.2. Meteorological data

    Estimating instantaneous evapotranspiration from the

    NOAA/AVHRR data requires several types of data, including

    air temperature, air pressure, water vapor pressure ( for the

    incoming long-wave radiation and short wave transmissivity).These data were obtained from the nine meteorological stations

    of Gansu Provincial Meteorological Bureau. The air temperature

    observations were interpolated into gridded data with a resolution

    of 1.1km, by considering the correlations with latitude, longitude

    and altitude. The cross-validation results showed that the interpo-

    lation error of temperature derived from the spatial distribution

    model is less than 0.7 C in terms of the absolute error. The spatial

    interpolation of air pressure was also performed by establishing

    a correlation equation between air pressure and altitude. The

    absolute error is less than 10Hpa. The water vapor pressure was

    interpolated using Kriging.

    Observation dataincluding surface albedo, land surface temper-

    ature (LST), net radiation, atmospheric long-wave radiation and

    eddy correlations were collected at two sites from the WATERexperiment in 2008 (Fig. 1) for validation of the model. One is the

    Yingke site and the other is the Huazhaizi site. The landscapes in

    thesetwo sitesare farmlandand desert steppe, respectively. Details

    of these sites can be found in Li et al. (2009b, 2011).

    2.2.3. Other data

    DEM data and the land use map of the Heihe River Basin were

    obtained from the Environmental and Ecological Science Data in

    western China (http://westdc.westgis.ac.cn).

    2.3. Evaporative fraction model

    The evaporative fraction is defined as follows:

    =E

    E+ H =

    E

    Rn G0(1)

    According to the surface energy balance equation,

    E=RnG0 H, Ecan be expressed as follows:

    E= (Rn G0) (2)

    where E is the latent heat flux (Wm2), Rn is the net radiation

    flux (net short and net long-wave) (Wm2), G0is the soil heat flux

    (W m2)andHisthesensibleheatflux(Wm2).Latentheatfluxcan

    be calculated from the net radiation, soil heat flux and evaporative

    fraction.

    Therefore, evapotranspiration can be assessed from remotesensing image by estimating the evaporative fraction, net surface

    radiation and the soil heat flux.

    2.3.1. Determining the net radiation

    Net radiation is determined by:

    Rn = (1 0)K +0 L 0 LST40 (3)

    where Rn is net radiation (Wm2), 0 is surface albedo (), K

    is incoming short wave radiation (Wm2), L is incoming long-

    wave radiation (Wm2), 0 is surface emissivity (), is the

    StefanBoltzmann constant as 5.67108 W m2 K4 and LST0 is

    land surface temperature (K). The estimation of these parameters

    is detailed below.

    http://www.ittvis.com/ProductServices/ENVI.aspxhttp://westdc.westgis.ac.cn/http://westdc.westgis.ac.cn/http://www.ittvis.com/ProductServices/ENVI.aspx
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    X. Li et al. / International Journal of Applied Earth Observation and Geoinformation 17 (2012) 8593 87

    Fig. 1. Observation sites in themiddle reaches of theHeiheRiverBasin.

    2.3.2. Solar short wave radiationThe instantaneous daily incoming short wave solar radiation on

    a surface for clear sky conditions is expressed as:

    K= I0E0 cos() (4)

    where I0 is the instantaneous extraterrestrial solar radiation

    (1367Wm2) (Iqbal, 1983), E0 is an eccentricity correction factor

    (Iqbal, 1983), is solar zenith angle (Wu et al., 1995), and is the

    transmittance in the short wave broadband range () (Iqbal, 1983).

    2.3.3. Surface albedo

    The broadband albedo is calculated from a simple linear combi-

    nation of data from channels one (red) and two (NIR) of the AVHRR

    sensor. Guo (2003) and Song and Gao (1999) introduced the fol-lowing formula to calculate the surface albedo:

    0 = 0.545vis+ 0.32nir+ 0.035 (5)

    where vis and nir are the visible and near-infrared reflectance

    from NOAA/AVHRR data, respectively.

    2.3.4. Incoming long-wave radiation

    The approach implemented here estimates instantaneous

    incoming long-wave radiation by the method describedby Iziomon

    et al. (2003):

    L =

    1 a exp

    b

    e0T

    air

    T4air (6)

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    88 X. Li et al. / International Journal of Applied Earth Observation and Geoinformation 17 (2012) 8593

    wherea= 0.35,b=10.0KhPa1, is the StefanBoltzmann constant

    and Tairis the air temperature (K).

    2.3.5. Outgoing long-wave radiation

    The StefanBoltzmann law is used to calculate the long-wave

    radiation from land surface:

    L0 = 0 LST40 (7)

    2.3.6. Surface emissivity

    Surface emissivity is estimatedby themethod of thenormalized

    differencevegetation index(NDVI) threshold,which is describedby

    Sobrino and Raissouni (2000).

    2.3.7. Land Surface temperature

    Land surface temperature is extracted from the brightness tem-

    peratures recorded by channels four and five of the NOAA/AVHRR

    instrument using the split window technique described by Ulivieri

    et al. (1994):

    LST0 = 2.8T4 1.8T5+ 48(1 0) 75 (8)

    where T4 and T5 are the brightness temperatures in channels fourand five, respectively. is the difference between the surface

    emissivity in channel four and the surface emissivity in channel

    five.

    2.3.8. Determination of soil heat flux

    Bastiaanssen et al. (1998a) utilizes a proportionality factor that

    describes conductive heat transfer in the soil using LST0, albedo

    (0) and an extinction factor that describes the reflection of radia-

    tion through vegetation canopies based on NDVI according to the

    following formula:

    G0 = Rn

    LST0 273.15

    0(0.0032C10+ 0.0062C

    21

    20)(1

    0.978NDVI4)

    (9)

    where C1is a conversion factor to obtain the daily average surface

    albedo from instantaneous values (default= 1.1) ().

    2.3.9. Determination of the evaporative fraction

    The major assumption in the NOAA/AVHRR data set is that

    the evaporative fraction remains constant for all overpass times

    associated with a daily satellite image (Crago, 1996; Franks and

    Beven, 1997). This assumption holds for environmental conditions

    under which soil moisture does not change significantly. Changes

    in weather conditions or cloud cover and surface discontinuities

    can induce significant variability of the evaporative fraction.

    A simple method to approximate the evaporative fraction is

    to combine albedo with land surface temperature as described by

    Su and Menenti (1999), Su et al. (1999), Roerink et al. (2000) and

    Verstraeten et al. (2005).

    =E

    E+ H

    LSTH LST0LSTH LSTE

    H 0 + bH LST0

    (H E)0 + (bH bE) (10)

    where LSTHis the land surface temperature for drypixels (K); LSTEisthe land surface temperaturefor wetpixels(K); Hand Earethe

    slopesof thehigh andlow surface temperature,respectively, which

    are functions of surface albedo (K); bHand bEare the intercepts of

    the high and low temperature, respectively, which are functions of

    surface albedo (K). By fitting the linear equations for the upper and

    lower boundaries ofLST0 0, the slope and intercept of Eq. (10)

    can be obtained.

    Fig. 2. The scatter plot of NDVI andevapotranspirationat themiddle reaches of the

    Heihe River Basin on June 3, 2008.

    3. Evaluation

    3.1. Evaluation of surface physical parameters

    3.1.1. Evaluation of surface albedo

    Table 1 compares the observed surface albedo at the Yingke andHuazhaizievaluation siteswith the surface albedo calculatedby Eq.

    (5). With the exception of the surface albedo at the Yingke oasis on

    June 3, 2008, the maximum absolute error is 0.037, and the mini-

    mum absolute error is 0.009.These results suggest that themethod

    for estimating the surface albedo has small errors.

    3.1.2. Evaluation of outgoing long-wave radiation

    Table 2 compares the observed outgoing long-wave radiation at

    the Yingke andHuazhaizi sites to theoutgoinglong-waveradiation

    calculated by Eq. (7). The maximum absolute error of the outgoing

    long-wave radiation is 39.2 W m2 (relative error of 7.9%), and the

    minimum absolute error is only 1.3W m2 (relative error of 0.38%).

    Therefore, the methods used to estimate land surface temperature

    and outgoing long-wave radiation show effective.

    3.1.3. Evaluation of incoming long-wave radiation

    Table 3 compares the observed incoming long-wave radiation

    at Yingke and Huazhaizi to the incoming long-wave radiation cal-

    culated from Eq. (6). As shown in this table, the maximum absolute

    error between theobservedand calculated values is 16.2 W m2 (at

    Yingke), andthe corresponding relative error is 5.2%; theminimum

    absolute error is 4.1W m2 (at Huazhaizi), and the correspond-

    ing relative error is only 1.2%. Therefore, the calculated results

    for incoming long-wave radiation show a high accuracy for both

    farmland and grassland sites.

    3.1.4. Evaluation of net radiationTable 4 compares the observed net surface radiation at Yingke

    and Huazhaizi to the estimated net surface radiation from Eq. (3).

    Themaximum absolute error is 87W m2 atYingkeon June 3,2008,

    andits relative error is 14.1%. Based on the results in Tables 1 and 2,

    errors in the estimated surface albedo and outgoing long-wave

    radiationlead to erroneousnet radiationvaluesfor thatday because

    reflected radiation and outgoing long-wave radiation are used to

    estimate net radiation. At Yingke, the relative errors are less than

    10% on August 2 and September 30.

    At Huazhaizi, the relative errorin net radiationis 12.1% (absolute

    error of 42.6W m2) on June 3, 2008. Previous results suggest that

    this error may have been due to errors in the estimated outgoing

    long-wave radiation and incoming long-wave radiation. On August

    25, 2008, the relative error in the net radiation of 11.2% may have

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    X. Li et al. / International Journal of Applied Earth Observation and Geoinformation 17 (2012) 8593 89

    Table 1

    Comparison between the measurements and the calculated results of land surface albedo.

    Date Observation sites Measured value Calculated value Absolute error Relative error (%)

    May 5 Huazhaizi

    Yingke 0.219 0.229 0.010 4.6

    June 3 Huazhaizi 0.274 0.265 0.009 3.3

    Yingke 0.109 0.188 0.078 71.5

    August 2 Huazhaizi 0.249 0.239 0.010 4.0

    Yingke 0.148 0.128 0.021 14.2

    August 25 Huazhaizi 0.265 0.228 0.037 14.0Yingke

    September 30 Huazhaizi 0.166 0.174 0.008 4.8

    Yingke 0.147 0.157 0.010 6.8

    Table 2

    Comparison between the measurements and the calculated results of outgoing long-wave radiation.

    Date Yingke Huazhaizi

    Measured

    value(W m2)

    Calculated

    value(W m2)

    Absolute error

    (W m2)

    Relative

    error (%)

    Measured

    value(W m2)

    Calculated

    value(W m2)

    Absolute error

    (W m2)

    Relative

    error (%)

    May 5 N/A 465.5

    June 3 495.7 535.0 39.2 7.9 613.5 595.6 17.9 2.9

    August 2 466.3 477.6 11.3 2.4 550.5 544.0 6.5 1.2

    August 25 573.2 564.2 9.0 1.6

    September 30 474.0 454.8 19.2 4.1 460.1 461.4 1.3 0.4

    Table 3

    Comparison between the measurements and the calculated results of incoming long-wave radiation.

    Date Yingke Huazhaizi

    Measured

    value(W m2)

    Calculated

    value(W m2)

    Absolute error

    (W m2)

    Relative

    error (%)

    Measured

    value(W m2)

    Calculated

    value(W m2)

    Absolute error

    (W m2)

    Relative

    error (%)

    June 3 351.4 346.4 5.0 1.4 332.5 336.6 4.1 1.2

    August 2 353.2 364.0 10.8 3.1 339.8 352.4 12.6 3.7

    August 25 346.3 336.2 10.1 2.9

    September 30 311.1 327.3 16.2 5.2 313.5 318.3 4.8 1.5

    been due to errors in estimated surface albedo. The relative error

    is less than 10% on the other two days.

    The evaluation of retrieval results of the surface parametersdemonstrates that errors in the estimated physical surface param-

    eters are small in the evaporative fraction model. The results

    therefore reasonably reflect the characteristics of the regional

    energy balance and the distribution of biophysical parameters.

    3.2. Evaluation of evapotranspiration

    The observed evapotranspiration at Yingke is compared to the

    estimated evapotranspiration by evaporative fraction model and

    displayedhere (Table 5). The maximum relative errorbetween June

    andAugust, when vegetative cover is high, ranges from 1% to 13.2%.

    Because the evapotranspiration estimation model involves many

    parameters, errors in each estimated parameter can affect the final

    evapotranspiration result. For August 2, errors in the estimated val-

    ues for surface albedo, land surface temperature (LST), outgoing

    long-wave radiation and incoming long-wave radiation were rel-

    atively small; thus, the error in the estimated evapotranspiration

    was also small. Therefore, the best evapotranspiration results can

    be achieved by applying the best possible methods to obtain

    each parameter in the evaporative fraction model. More accurateestimated parameters yield more accurate estimates of evapotran-

    spiration.

    In early May and late September, estimates of evapotranspira-

    tion tend to have larger errors due to sparse vegetation or a lack

    of contrast between vegetative coverage inside and outside of the

    oasis. In this case, the evapotranspiration model is less able to pro-

    duce meaningful results.

    4. Results and analysis

    4.1. Spatial variation of evapotranspiration in themiddle reaches

    of the Heihe River Basin

    A comparison of the calculated results of evapotranspiration

    with the NDVI indicates a strong relationship over the study area.

    Fig. 2 is a scatter plot of NDVI and latent heat flux at the middle

    reaches of the Heihe River Basin on June 3, 2008, showing almost a

    Table 4

    Comparison between the measurements and the calculated results of net radiation.

    Date Yingke Huazhaizi

    Measured

    value(W m2)

    Calculated

    value(W m2)

    Absolute error

    (W m2)

    Relative

    error (%)

    Measured

    value(W m2)

    Calculated

    value(W m2)

    Absolute error

    (W m2)

    Relative

    error (%)

    June 3 617.2 530.0 87.2 14.1 351.4 394.0 42.6 12.1

    August 2 659.2 646.0 13.2 2.0 480.0 498.0 18.0 3.8

    August 25 398.5 443.0 44.5 11.2

    September 30 438.5 473.0 34.5 7.8 458.7 451.6 7.1 1.5

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    90 X. Li et al. / International Journal of Applied Earth Observation and Geoinformation 17 (2012) 8593

    Fig. 3. Distribution of latent heat flux over central Heihe River Basin in 2008 (a, May 5; b, June 3; c, August 2; d, September 30).

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    X. Li et al. / International Journal of Applied Earth Observation and Geoinformation 17 (2012) 8593 91

    Table 5

    Comparison between themeasurements and thecalculated results of latentheat flux at Yingke.

    Date Measured value (W m2) Calculated value (W m2) Absolute error (W m2) Relative error (%)

    May 5 158.6 209.0 50.4 31.8

    June 3 372.8 323.0 49.8 13.3

    August 2 437.0 485.0 48.0 11.0

    August 25 523.9 519.0 4.9 0.9

    September 30 150.8 265.0 114.2 75.7

    linear positive correlation between NDVI and evapotranspiration.

    But it is also clear that at low NDVI values there are a lot of outliers.

    On May 5,2008 (Fig. 3a), the maximum value of latent heat flux

    (300350W m2) occurs in parts of Gaotai, which is located on the

    bank of the Heihe River bank and scattered across some areas of

    Jiuquan oasis. The next highest values, 200300W m2, are found

    in Zhangye, Linze, Gaotai, most part of the Jiuquan oasis and on

    the banks of the Heihe River. Evapotranspiration values in the Gobi

    desert are obviously low, typically less than 50W m2. Areas along

    the moisture river banks with more vegetation coverage get more

    evapotranspiration than other regions. In many artificial oases of

    the middle reaches of the Heihe River in early May, spring wheat

    is just in the tiller or jointing stage and spring corn is in the trefoil

    stage. Because the vegetation index is relatively low at this point,

    there is no pronounced difference in evapotranspiration between

    the oases and the surrounding desert areas.

    On June 3, 2008 (Fig. 3b), the maximum value of latent heat

    flux is seen within the oases at Zhangye, Linze, Gaotai and Jiuquan,

    where it reaches from 450 to 500 W m2; the latent heat flux

    and NDVI in most other parts of the oases are between 350 and

    450Wm2 and between 0.3 and 0.4, respectively. At the edge of

    the oases, where vegetation is sparse, the latent heat flux ranges

    from about 350400W m2. The NDVIof the Jinta oasis isless than

    0.2, and its latent heat flux is also smaller (200300W m2).In the

    Gobi desert, just outside the oases, the latent heat flux is below

    150Wm2. Because almost no plants grow in the desert, the latent

    heat flux sharply decreases to a dozen W m2 in some places.

    With vegetationgrowth in August, themaximum value of latent

    heat flux(500550 W m2) occurson August2, 2008at theZhangyeoasis and Linze oasis, which lies on the Heihe River banks (Fig. 3c).

    In Gaotai, Linze and the northern part of the Zhangye, the latent

    heat flux is between 400 and 500 W m2. The latent heat flux

    is 350400W m2 across most of the Jiuquan oasis and is about

    200400W m2 in Jinta oasis and NDVI is about 0.10.4; these

    values indicate thatthe landscapewithin the Jintaoasis is heteroge-

    neous and that the vegetation distribution varies greatly. However,

    the latent heat flux in the Gobi desert area varies much less in

    August than in June.

    On September 30, 2008 (Fig. 3d), the green of the NDVI image

    rapidly declines, which corresponds to crop maturity and harvest.

    The maximum value of latent heat flux is again found in Zhangye

    oasis with a value between 300 and 350W m2. In this oasis, the

    large value of the NDVI (0.30.4) indicates that some plants arestillgrowing. Higher values of the latent heat flux are also scattered

    across some areas of Linze, Gaotai and Jiuquan at this time, but the

    latent heat flux in most parts of the oases drops to between 250

    and 300Wm2 from more than 350W m2 in August. In the Gobi

    desert, which has little vegetation, evapotranspiration remains at

    a steady low level.

    4.2. Temporal variation of evapotranspiration in the central

    Heihe River

    Based on the distribution of evapotranspiration values on May

    5, June 3, August 2 and September 30, during all of these months

    evapotranspirationis very lowin theGobi desert, where vegetation

    issparse.Withtheexceptionofafewplacesneartheoasesthathave

    slightly more evapotranspiration, the latent heat flux is typically

    less than 10Wm2 in some places. This condition is the result of

    the surface energy balancing process, in which sensible heat flux

    and soil heat flux are major parameters, whereas latent heat flux

    has minimal influence.

    Evapotranspiration variation in the middle reaches of the Heihe

    River Basin is closely related to crop growth. In early May, when

    springwheatis in thetiller or jointing stage andcorn is in thetrefoil

    stage, the ground has limited vegetation cover, and evapotranspi-

    ration values are similar for the oasis and the surrounding desert.

    On August 2, when spring wheat, maize and other crops are expe-

    riencing vigorous growth, oasis evapotranspiration increases to a

    maximum value. Harvesting at the end of September causes oasis

    evapotranspirationto become lower than that in August. Both river

    banks are distinguished from the surrounding desert by their rel-

    atively moist conditions and high evapotranspiration values on all

    of the studied dates. Changes in the evapotranspiration in desert

    areas are consistently small.

    Evapotranspirationvariations in the middle reaches of the Heihe

    River Basin are closely related to crop growth and it has a strong

    relationship with the NDVI. This suggests that according to the

    characteristics of spatial and temporal variation of evapotranspira-

    tion, rational utilization of water resources in the oasis is essential

    to manage the water resources in the inland river basin.

    5. Discussion

    Estimated evapotranspiration values are evaluated by compari-

    son to surface flux observations from WATER. During months with

    greater vegetative cover (June, July and August), the relative error

    in the results of the evaporative fraction model ranges from 13.2%

    to as little as 1%. For a pixel range of 1.1km, this result is accept-

    able. However, when vegetation cover in the middle reaches of the

    Heihe River Basin is sparse (May and September), the evapotran-

    spiration estimation error is relatively large, which indicates that

    the method is not effective for the condition with less vegetative

    coverage.

    Changes in the evaporative fraction at Yingke are evaluated

    based on data from May 5, September 30, June 3 and August 2 and

    25, 2008 (Fig. 4). In the early stage of crop growth (May 5) when

    Fig. 4. Daily variations of the evaporative fraction at Yingke site.

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    vegetative coverage is low and the NDVI is 0.06, the change in the

    evaporative fraction is obvious. In the late stage of crop growth

    (September 30), the NDVI is 0.21, and the evaporative fraction also

    changes clearly during the day. During the vigorous growth stage

    (June 3, August 2 and 25), the NDVI is above 0.30, and the evap-

    orative fraction changes little during the day. Therefore, changes

    in the evaporative fraction likely contribute to the errors in esti-

    mated evapotranspiration. In addition, satellite passing time and

    observation time are not completely consistent, which generates

    the difference between the observed and estimated values. For

    instance, on May 5, at the satellite passing time of 15:40 (local

    time), the estimated latent heat flux was 209W m2; the latent

    heat flux values observed on the ground were 203.3 W m2 at

    15:15 and 158.6 Wm2 at 15:45. On September 30, at the satel-

    lite passing time of 15:00, the estimated latent heat flux was

    265Wm2; observed latent heat flux values were 150.9 W m2 at

    15:15 and 167.7 Wm2 at 15:45. Therefore, the evaporative frac-

    tion changes during the early and late crop growth stages, and the

    timeassociatedwith satellite and ground-based measurements are

    not completely consistent. These factors contribute greatly to the

    large estimation errors on May 5 and September 30.

    Two major error sources should be discussed here. One is the

    error related with the temporal scale. The estimated evapotran-

    spiration extracted from remote sensing data is an instantaneous

    value, while the evapotranspiration measured by the Eddy Covari-

    ance system(EC) is generallya mean value withina certain average

    period (normally 30min). Therefore, the difference in the tempo-

    ral scale might make some contribution to the errors between the

    estimated and measured evapotranspiration.

    The other is the error related with the spatial scale. EC at the

    Yingke station is set up at 28m high to observe evapotranspiration

    of cropland. Its footprint is about 250m of radius in circle range

    according to the study ofShang et al. (2009). When comparing the

    latent heat flux value measured by EC with the estimated value

    from NOAA/AVHRR data with 1.1 km resolution, the difference in

    spatial scale may bring errors (Song, 2011). However, how to take

    account the scale issue into validation is a very challenge issue and

    it needs further investigation. It believes that higher spatial resolu-tion remote sensing data can play an important role in solving this

    problem.

    The model is also sensitive to theerrors in the input parameters,

    to quantify these errors is also of great importance. To incorporate

    the remote sensing model of evapotranspiration into a land data

    assimilation system for better estimation of ET and quantification

    related errors will be our future research priority.

    6. Conclusion

    This paper uses the remote sensing data and WATER observa-

    tions to estimate the evapotranspiration over the middle reaches

    of the Heihe River Basin based on the evaporative fraction method.The evaluation of the obtained parameters and modeling results

    suggest that the method produces only small errors and is able

    to achieve the goals of a good ET estimation. When estimating

    regional evapotranspiration from the evaporative fraction, vege-

    tative growth conditions must be considered. Good results can be

    obtained only if the evaporative fraction remains constant during

    the day. Generally, during peak crop growth (June to August), the

    evaporative fraction model can yield accurate results for evapo-

    transpiration.

    Evapotranspiration and NDVI distribution are strongly corre-

    lated. The oases and river banks, which have higher NDVI, typically

    have greater evapotranspiration, whereas areas with sparse or no

    vegetation coverage normally have very low evapotranspiration.

    There are also some exceptions in Fig. 2. We found that most of the

    points apart from the linear correlation line are distributed near

    the river. They have little vegetation cover, with NDVI value

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