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    Objectives of the Atmospheric

    Dynamics Mission

    The prim ary aim of the Earth Explorer

    Atm ospheric D ynam ics M ission (AD M )

    is to p rovide im proved analyses of the

    global three-dim ensional w ind field, by

    dem onstrating the ability to correct the

    m ajor deficiency in w ind-profiling of

    the G lob al C lim ate O bserving System

    (G C O S) and the current G lobal

    O bserving System (G O S). The A eolus-

    A D M w ill provide the w ind-profile

    m easurem ents required to ad vance

    atm osp heric m od elling and analyses.

    N ew insights into the atm osphere,

    through the provision of w ind profiles,

    are required, not only for clim ate

    research, but also for num erical

    w eather pred iction (N W P). The A eolus-

    AD M w ill address one of the m ain

    areas discussed under Them e 2Physical C lim ateof the ESA Living

    Planet Program m e [ESA 1998;ESA

    1999b]. A lthough there are several

    w ays of m easuring w ind from a

    satellite, the active D oppler w ind lidar

    (D W L) is the only candidate, so far

    identified, that can provide direct

    observations of w ind profiles, and thus

    has the potential to provide the

    requisite data globally. In addition, the

    D W L also has the potential to p rovide

    ancillary inform ation about cloud topheights, vertical distribution of cloud,

    aerosol properties, and w ind variability.

    These w ould be b y-products.

    The Need for Atmospheric Wind

    Fields for Climate Studies and

    Numerical Weather Prediction

    (NWP)

    C lim ate-change issues have received

    substantial attention in recent yearsdue to the increasing aw areness that

    hum an activities m ay substantially

    m odify the future clim ate of the Earth.

    The glob ally averag ed tem perature

    has increased by ab out 0.6C over the

    past hundred years and 1998 w as the

    w arm est year recorded in the

    instrum ental tem perature d ata

    covering the last 150 years. These

    facts, and other pieces of evidence,

    suggest that an increase in the

    greenhouse effect, due to hum anactivities, is starting to influence the

    global clim ate system . A very

    im portant question is, thus, to assess

    how any future increase in

    greenhouse g ases m ay affect this

    system .

    R eliab le instantaneous analyses and

    longer term clim atologies of w inds areneeded to im prove our understanding

    of atm ospheric d ynam ics and the

    glob al atm ospheric transport and of

    the cycling of energy, w ater, aerosols,

    chem icals and other airborne

    m aterials. H ow ever, im provem ents in

    analysing global clim ate, its variability,

    predictability and change, require

    m easurem ents of w inds throug hout

    the atm osp here.

    The m ost effective tools available toansw er such q uestions are g lob al and

    regional clim ate m odels, w hich to a

    very large extent resem ble the

    Earth Explorer Missions 12

    The Atmospheric Dynamics Mission

    P. Ingmann and J. Fuchs (1), J. Pailleux (2) and A. Stoffelen (3)

    (1) ESA/ESTEC , P.O . Box 299, 2200 AG N oordw ijk, The N etherlands

    (2) M to-France, 42 avenue C oriolis, 31057 Toulouse C edex, France

    (3) Royal N etherlands M eteorological Institute (KN M I), PO Box 201, 3730 AE D e B ilt, The N etherlands

    The quality of m odels used in clim ate research and num erical w eather prediction (N W P) relies m uch on the availability of

    observations. M odels have im proved m uch over the last decade. Better param ersiation schem es are used in clim ate

    m odels; advanced data assim ilation techniques are now being used for the analysis in N W P. H ow ever, conventional w ind

    profile data lack coverage and uniform distribution over the globe. Thus, there is a need for w ind profilers in order to

    im prove the G lobal (C lim ate) O bserving System .

    In the context of the Earth Explorer C ore M issions, ESA is preparing a m ission aim ing at the observation of the atm ospheric

    w ind profile, nam ely the Atm ospheric D ynam ics M ission (AD M ). Its m ain com ponent w ill be a D oppler w ind lidar..

    Fig. 1: The intim ate links betw een num erical w eather prediction (N W P) and

    clim ate studies.

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    corresponding N W P m odels. A ll the

    benefits of w ind data related to

    circulation m odels used for clim ate

    stud ies are also relevant to N W P

    m odels, as b oth m odel types are

    based on the sam e physical and

    num erical principles. The intim acy of

    the links betw een N W P and clim ate

    studies is d epicted in Fig.1: there is a

    continuous transition betw een N W P

    and clim ate stud ies on a prog ressive

    tim e scale. A ny im provem ent in N W P

    w ill result in an im provem ent in clim ate

    m odels. This w as d em onstrated

    recently w ith the ER A -15 data set (i.e.the re-analysis of the w hole 15 year

    period 1979 to 1994 carried out at

    EC M W F and N C EP). A s an exam ple,

    for the zonal w ind com ponent, a

    com parison of the N C EP and EC M W F

    m od els w as carried out, w hich

    show ed m ajor differences in the

    tropics and in the low er stratosphere

    (Fig. 2).

    This reflects m ajor deficiencies in

    m od el param eterisations, w hich needto be resolved.

    The different types of w ind

    observations currently available and

    constituting the G lobal O bserving

    System (G O S), are d ocum ented in full

    detail in [ESA 1996]. They can be

    classified in the follow ing w ay:

    Surface d ata the synoptic reports

    from land stations and ships, data

    from m oored and drifting buoys as

    w ell as scatterom eter w ind s from

    satellites (such as ER S). A ll these

    are single level data and do not

    provide any inform ation on

    atm ospheric profiles.

    Single-level upper-air data m ainlyaircraft reports and cloud m otion

    w inds derived from geostationary

    satellite im ag ery. M ore and m ore

    aircraft observations (w ind and

    tem perature) are b eing m ade

    during ascent and d escent phases,

    thus tending to b ecom e m ulti-

    level. Their m ain deficiency is the

    poor geographic data coverage,

    especially over the oceans and in

    the S outhern H em isphere.

    M ulti-level upper-air data radiosondes are the only current

    observing system providing vertical

    profiles of the w ind field, but they

    are confined m ainly to the

    continents in the N orthern

    H em isphere (Fig. 3).

    C om plem entary observations are

    provided by the sound er instrum ents

    on board low -Earth orbiting satellites.

    Satellite sounders p rovide global

    coverag e w ith rad iance data, but

    these can only be used indirectly for

    the definition of the m ass field

    (tem perature and hum idity). From

    these observations, synoptic scale

    w ind fields at higher latitudes can be

    derived. This does not w ork at sm allerscales or at low latitudes.

    The W orld M eteorolog ical

    O rganisation (W M O ) states in its

    recent evaluation of user

    requirem ents and satellite capabilities

    that, for global m eteorological

    analyses, m easurem ent of w ind

    profiles rem ains m ost challenging and

    m ost im portant [W M O, 1998]. The

    W M O recognises the p rim e need for

    w ind-profile d ata [W M O, 1998] andhas d efined a set of w ind- profile

    m easurem ent requirem ents [W M O,

    1996]. The W M O (e.g. [W M O, 1996])

    ADM13

    Fig. 2: C om parison of N C EP (N ational C entre for Environm ental prediction) and ERA (EC M W F R e-Analysis) derived zonal

    w inds. M ajor differences are found m ainly in the tropics and in the low er stratosphere (courtesy K N M I)

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    attaches great im portance to w ind -

    profile m easurem ents. The realisation

    of these req uirem ents w ould rep resent

    a m ajor step forw ard in im proving the

    quality of atm ospheric flow analyses.

    There is a clear requirem ent for a

    high-resolution system observing

    atm osp heric w ind profiles directly.

    The Observational Requirements of

    the Atmospheric Dynamics Mission

    Existing system s cannot m eet the

    requirem ents for better w ind profiles.

    In order to m eet the needs of N W P,

    clim ate and atm osp heric research

    ob jectives, an ob serving system has

    to be set up that provides three-

    dim ensional w ind data over the glob e.This m eans that it is essential to

    devote significant effort to the

    developm ent of space-based

    system s.

    For a m ission intended to dem onstrate

    the feasibility of a full-scale sp ace-

    borne w ind ob serving system to

    im prove glob al atm osp heric analyses,

    the req uirem ents on data quality and

    vertical resolution are very stringent

    and difficult to achieve. The horizontaldensity of observations is of low er

    priority. The derivation of the coverage

    specification is supported by w eather-

    forecast-im pact experim ents, w hich

    included the inputs from the

    conventional w ind-profile netw ork, that

    provides poor geographic coverage

    and is irregular in tim e but

    nevertheless is of key im portance. The

    use of variational assim ilation

    techniques im plies that only line-of-

    sight (LO S) w inds are required; vector

    w ind s are not necessary. Table 1

    specifies the principal param eters for

    w ind-profile observations that have

    been extracted from the previously

    m entioned W M O requirem ents and

    capab ilities docum ents.

    The Technical Concept of theAtmospheric Dynamics Mission

    The m easurem ent concep t is

    illustrated in Fig. 4: the heart of the

    m ission is a space-borne D oppler

    w ind lidar w hich em its ultraviolet

    pulses tow ards the Earth. These are

    reflected by the atm osp here and by

    Earth Explorer Missions 14

    O bservational R eq uirem ents

    PB L Troposph. Stratosph.

    Vertical D om ain [km ] 0-2 2-16 16-20

    Vertical R esolution [km ] 0.5 1.0 2.0

    H orizontal D om ain global

    N u m b er of P rofiles [hour-1] 100

    Profile Separation [km ] > 200

    Tem poral Sam pling [hour] 12

    Accuracy (C om ponent) [m s-1] 2 2-3 3

    H orizontal Integration [km ] 50

    Tim eliness [hour] 3

    Leng th of O bservational

    D ata Set [yr] 3

    Table 1: O bservational requirem ents for the Atm ospheric D ynam ics M ission

    (PBL = planetary boundary layer).

    Fig. 3: The radiosonde netw ork radiosonde/pilot ascents containing w ind profile inform ation that w ere available for the 6-

    hour tim e w indow centred around 12 U TC on 28 April 1999. W ind profile inform ation is generally m issing over all ocean

    areas.

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    M ean O rbit Param eters

    O rbit Type Sun-synchronous orbit

    at 18:00 LTAN

    M ean A ltitude 408 km

    Inclination 96.99

    the Earths surface. These back-

    scattered signals are p rocessed to

    provide quantitative inform ation on

    vertical w ind profiles. The lidar

    exploits the D oppler shifts induced by

    the w ind on the received signal back-

    scattered from aerosols or m olecules.

    In addition, inform ation can be

    derived ab out other param eters

    (e.g. cloud cover or aerosol content).

    Electrom agnetic radiation in the

    ultraviolet is heavily attenuated by

    cloud. A com plete profile can thusonly be derived in a cloud-free or

    partly cloud-free atm osphere, through

    gap s betw een clouds. H ow ever, it has

    been dem onstrated that in about 50 %

    of the cloudy cases it is still possible

    to retrieve w ind profiles w ith high

    quality [ESA 1999a]. If a scene is

    overcast, w ind profiles can be derived

    for the layers above the clouds.

    Furtherm ore, sim ulations have show n

    that cloud-free observations alone

    w ould still have a significant im pact.

    The m ission requires the m easurem ent

    of horizontal w ind velocity

    com ponents from the low er part of thetroposphere to the low er part of the

    stratosphere (up to 20 km altitude). A s

    the ob servation of a sing le com ponent

    of the horizontal w ind velocity has

    been show n to be adequate to m eet

    the m ission ob jectives of A eolus-A D M ,

    this has been b aselined to ease

    instrum ent design.

    For the satellite, a sun-synchronous

    daw n-dusk orbit has been selected .

    This p rovides quasi-glob al coverag eand corresp onds to a low er cloud

    coverage w hile, in turn, it w ill also

    im prove p erform ance. It also

    facilitates som e asp ects of the satellite

    design.

    The LO S of the instrum ent w ill be 35

    off nadir, to ensure optim al instrum ent

    perform ance. and 90 across the flight

    direction to avoid a contribution from

    the satellite velocity to the D oppler-

    frequency shift. To dim inish

    background radiation effects, the LO S

    of the instrum ent w ill point in the anti-

    Sun direction. The equator crossing

    tim e has b een chosen to p rovide lowcloud-cover conditions. The orbit w ill

    provide a slightly b etter coverage over

    the N orth Pole than over the South

    Pole. A baseline altitude of 400 km

    has been selected . The orbit

    param eters are sum m arised in Table 2.

    The instrum ents orientation is

    depicted in Fig. 5. The sam pling

    schem e foresees one m easurem ent

    being m ade every 200 km and an

    integration length of 50 km .

    The req uired instrum ental accuracy

    for any horizontal LO S w ind

    ADM15

    Fig. 4: D oppler W ind Lidar principle: the lidar em its a laser pulse tow ards the atm osphere, then collects, sam ples, and

    retrieves the frequency of the back-scattered signal. The received signal frequency is D oppler-shifted from that em itted by

    the laser, due to the spacecraft, Earth, and w ind velocities. The lidar m easures the w ind projection along the laser line-of-

    sight (LO S), using a slant angle relative to nadir.

    Table 2. M ain param eters of selected

    baseline orbit.

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    sea) echo w ill be d etected tocalibrate distance (height).

    In order to transform raw data into

    w ind m easurem ents, processing has

    to be perform ed for both the aerosol

    and the m olecular channels. This

    requires taking into account

    background radiances and the

    spectrom eter spectral response, as

    w ell as calibration data. Finally, using

    satellite sensor data, each w ind

    m easurem ent for each altitud e layerm ust be located in an E arth reference

    fram e.

    A schem atic flow diag ram for the

    data processing, calibration andvalidation, and inform ation

    dissem ination for the space-borne

    D oppler w ind lidar is show n in Fig. 6.

    The processing of D W L data in a

    realistic atm osphere has been

    sim ulated in order to verify

    perform ance in b oth clear and cloudy

    areas. C ontrary to passive satellite

    sensors, w hich have relatively large

    footprints, an active D W L, firing m any

    shots per second , exhibits good

    potential for extracting usefulinform ation on the atm osphere in

    partly cloudy cases. This w as m ad e

    clear in the LITE back-scatter lidar

    com ponent has been translated from

    the m ission accuracy req uirem ent of

    2-3 m s-1 for each w ind com ponent

    (see Table 1). Stringent requirem ents

    on w ind accuracy and the large

    vertical dom ain (up to 20 km ) lead to

    the consideration of an instrum ent

    concep t w hich relies on m olecular

    backscatter at high altitude (w here

    background aerosols becom e rare)

    and on aerosol backscatter at low er

    altitude. Fig. 5 also show s the

    baseline m easurem ent profile.

    The d esign features of the selected

    baseline concep t are show n in [M gie

    and Readings, this issue, Fig. 4]. The

    satellite is a conventional boxstructure w ith a central cone upon

    w hich the instrum ent is m ounted via

    the three isostatic m ounts (bipods).

    Since the satellite is flow n in a daw n-

    dusk orbit, the y-side alw ays faces

    aw ay from the Sun, and the solar

    arrays can be w ing s, one forw ard and

    one aft of the bus (w ith reference to

    the flight direction), fixed in

    orientation.

    Data ProcessingThe instrum ent w ill transm it raw data

    to the ground, w hich consists of the

    accum ulated spectra from the M ie

    receiver and the flux intensities from

    the R ayleigh receiver. These data are

    nom inally provided every 3.5 km

    along-track. The instrum ent has the

    potential to provide data every 1 km

    horizontally for dedicated areas (when

    required) and for each altitude bin

    (-1 km (for calibration) to 16.5 km

    height for the M ie channel, 0.5 km to

    26.5 km for the R ayleigh channel). Thevertical resolution is configurable

    betw een 500 m and 2 km .

    Prior to integrating data over 50 km

    along-track, som e signal processing

    w ill be carried out to segregate the

    sam ples from clear air from those

    affected by cloud, to control the

    processing in case of variable

    conditions, e.g., due to cloud. A s

    such, besides w ind profiles ab ove

    clouds and optically thick cloudlayers, even full w ind profiles of useful

    quality m ay be obtained in m any

    cases of scattered cloud. G round (or

    Earth Explorer Missions 16

    Fig. 5: Baseline Aeolus-AD M m easurem ent geom etry the baseline

    m easurem ent profile depicting the m apping of atm ospheric heights to layers

    m easured by the detector. The vertical as w ell as the horizontal values can be

    program m ed, thus providing good flexibility.

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    European S pace A gency, 1999b : The

    ESA Living PlanetProg ram m e, EO Q ,

    N 63, pp 1-20

    W orld M eteorolog ical O rganisation,

    1996: G uide to M eteorolog ical

    Instrum ents and M ethods of

    O bservation, 6th edition, W M O -N o.8,

    Secretariat of the W orld

    M eteorolog ical O rganisation, G eneva,

    Sw itzerland.

    W orld M eteorolog ical O rganisation,

    1998: Prelim inary S tatem ent of

    G uidance R egarding H ow W ell

    Satellite C ap ab ilities M eet W M O U ser

    R equirem ents in Several A pplication

    A reas. W M O Satellite R ep orts SAT-21.

    W M O /TD No

    913.

    ADM17

    Fig. 6: Schem atic flow diagram for the data processing, validation and

    calibration of the inform ation from a space-borne D W L (L = processing level).

    m ission on the Space S huttle. The

    sim ulated D W L m easurem ents have

    also been assim ilated in a state-of-

    the-art atm ospheric data assim ilation

    system , in a so-called O bserving

    System Sim ulation Experim ent

    (O SSE). Im proved analyses and

    forecasts w ere dem onstrated in the

    N orthern H em isphere through the

    addition of A eolus-A D M D W L

    m easurem ents.

    Context

    The A tm ospheric D ynam ics E arth

    Exp lorer C ore M ission w ill for the first

    tim e provide direct observations, on a

    global scale, of atm ospheric w ind

    profiles in clear or partly cloudy air

    over the dep th of the atm osphere, a

    notable deficiency of currentob serving system s. These data w ill

    find w ide application in advancing the

    perform ance of num erical m odels

    used in clim ate research and w eather

    forecasting, as these are suffering

    increasingly from the lack of such

    data. R eliab le m easurem ents of the

    tropospheric, three-dim ensional, w ind

    field are of the utm ost im portance for

    N W P, seasonal-to-interannual

    forecasting and for studying

    atm osp heric dynam ics, energeticsand the w ater, chem ical and aerosol

    cycles associated w ith the state of the

    global clim ate and its future evolution.

    W ith these data it w ill also be possible

    to increase und erstanding of

    atm ospheric processes occurring in

    tropical regions to the point w here it

    w ill be possible to take proper

    account of them in clim ate m od els. A t

    present, in tropical regions little

    inform ation ab out atm ospheric

    dynam ics can be inferred from the

    existing G O S. The proposed concep t

    also m eets the req uirem ents of grow th

    potential, w hich is relevant in view of a

    future operational m ission.

    M ore detailed inform ation on the

    scientific context and the m ission

    im plem entation can b e found in

    [ESA 1999a].

    ReferencesEuropean Space A gency, 1996:

    A tm ospheric D ynam ics M ission, ESA

    SP-1196 (4).

    European Sp ace A gency, 1998: The

    Science and R esearch E lem ents of

    ESAs Living Planet Prog ram m e, ESA

    SP -1227, 105p p.

    European Space A gency, 1999a:

    A tm ospheric D ynam ics M ission,

    R eport for M ission Selection, ESASP-1233(4) also on the internet at

    < http://w w w.estec.esa.nl/m ag/doc/ad

    m .pdf>