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    Zimmermann Hydrological Modeling 1

    Dr. Lothar ZimmermannBavarian Forest Institute

    Phone:

    08161-71-4914

    For questions:

    [email protected]

    Introduction Hydrological Modelling

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    Zimmermann Hydrological Modeling 2

    Lecture: Hydrological Modeling

    Short description:

    Overview in application of hydrological models in

    water ressources management in order to quantify

    effects of land use and climate change on water

    budget (ground water recharge) and flood

    generation

    Aim of the course:

    General knowledge about hydrological

    problems and their solution by models

    practical work experience with a model

    introduction towards sophisticated models

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    Zimmermann Hydrological Modeling 3

    What is Hydrological Modeling Good for?

    Climate and land use change and its

    impacts on the water budget, dischargeand water quality

    Extremes

    Flood forecast and protection

    Drought and low flows

    River management

    Ground water management

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    Zimmermann Hydrological Modeling 4

    Structure of the lecture

    1. Water budget and its components (Review)

    2. Model theory for water budget models

    3. Change of land use and effects for water and

    element budget

    4. Climate change scenarios

    5. Practical examples with BROOK90

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    Precipitation

    (rain, snow)Transpiration and

    Interception fromplants

    Evaporation from bare soil

    Overland flowTranspiration and

    Interzeption from

    plantsSoil Percolation

    Interflow

    Soil Percolation

    Capillary rise

    Groundwater flow

    Soil PercolationSoil Percolation

    River flow,

    discharge

    Water Circle Components of a Landscape

    (mod. after Bremicker 1999)

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    Water budget components in the Eastern U.S

    (Hewlett 1982)

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    Zimmermann Hydrological Modeling 8

    Precipitation: Measurement of Rainfall

    Unit: 1 l/m2*d = 1 mm/d

    German Hellmann collector 200cm

    (Maidment 1982)

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    Zimmermann Hydrological Modeling 9

    Precipitation: Correction for systematic undercatch

    Mean rain gauge deficiency for

    snowfall of US gauges in dependence on wind speed Wind shield

    3 main errors:

    Wind 10%Evaporation 2-3%

    Interception 2-3%

    (Maidment 1982) (Dyck&Peschke 1995)

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    Zimmermann Hydrological Modeling 10

    Precipitation: Measurement of snow height and

    water equivalent

    Snowpack depth

    Water equivalent:

    Depth of water produced by the melted snow

    Water equivalent=snow density [kg/m**3]*snow depth [m]

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    Zimmermann Hydrological Modeling 11

    Areal Precipitation: IDW Inverse Distance Weighting

    Catchment with precipitation gauges

    point precipitation

    Catchment with areal precipitation

    ?

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    Zimmermann Hydrological Modeling 12

    Variability of Precipitation

    Precipitation DWD-Weihenstephan year/vegetation period in comparison

    to long-term average (1951-80 resp. since 1995 : 1961-90)

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    Zimmermann Hydrological Modeling 13

    Evapotranspiration: Measurement

    Lysimeter Evaporation pan

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    Zimmermann Hydrological Modeling 14

    Evapotranspiration: Energy and Water Budget

    R G H L E.E R S PW

    Energy balance

    Water balance

    Rn: radiation balance, net radiation [W/m2]

    G: heat flow in the ground [W/m

    2

    ]H: sensible heat flux [W/m2]

    L.E: latent heat flux [W/m2]

    Energyflux densities

    Fluxes

    Energy

    flux densities

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    Zimmermann Hydrological Modeling 16

    Potential evapotranspiration

    Maximum possible evapotranspiration under given climatic conditions

    2 * If

    Short-cut grass is in the midst of a large, unbroken, similarly

    vegetated stretch of land

    Soil moisture is so plentiful that uptake by plants is not inhibited

    Advantage:Calculation by meteorological quantities(air temperature, relative humidity, net or global radiation, sunshine

    duration, windspeed)

    Definition:

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    Zimmermann Hydrological Modeling 17

    Potential evapotranspiration: Upper limit

    Rn: net radiation [W m

    -2

    ]

    L

    RnradiationnetofequivalentWater

    The water equivalent of net radiation is the upper limit for potential evapotrans-

    piration if sensible (H) and ground heat flux (G) is neglected (see energy balance).

    It describes that all net incoming radiative energy is completely used for the

    evaporation of water, so it assumes that no bodies are warmed (heat flow in the

    ground G) or that air is warmed and bubbles up as eddy (sensible heat flow). Forreal calculations the terms of H and G cannot be neglected.

    From energy balance: L.ET=Rn-G-H G, H neglected

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    Zimmermann Hydrological Modeling 18

    Potential evapotranspiration: Formulae I

    Haude: [mm/d]

    e: vapour pressure at 2 pm localtime [hPa]

    es: saturation vapour pressure at 2 pm [hPa]

    f: monthly proportional factor (empirical)

    ETP f e es( )

    Vapour deficit driven by air temperature and therefore

    indirectly by radiation

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    Zimmermann Hydrological Modeling 19

    Empirical monthly factors dependent on vegetation type

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    Zimmermann Hydrological Modeling 20

    Haude: Empirical monthly factors also dependent on altitude

    Upper physical limit of ET

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    Zimmermann Hydrological Modeling 21

    Potential evapotranspiration: Formulae II

    Priestley-Taylor

    : 1.26 (arid: 1.74)

    s: slope of vapour pressure curve e(T) [hPa*K-1]

    : psychrometric constant [hPa*K-1]

    Rn: net radiation [Wm-2]

    G: ground heat flow [Wm-2]

    GRns

    s

    ETP *

    Psychrometric constant :

    = air pressure p [Pa]* specific heat of air at constant pressure [J*kg-1*K-1] / (m*L) [J*kg-1]

    m: ratio of individual gas constants for water vapor and dry air =0.622

    = 0.016286 * p/L p=1013.25 hPa, T=15.2C = 0.67hPa*K-1

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    Zimmermann Hydrological Modeling 22

    PenmanETP

    s RL

    f u e e

    s

    ns* ( ) ( )

    Potential evapotranspiration: Formulae III

    From all three formulae for potential evapotranspiration PENMAN is the most

    pyhsically based one since it considers

    radiation

    vapour deficit

    ventilation (wind)as the three meteorological driving forces of evapotranspiration.

    Wind function f(u)=0.26 (1+0,54u) [mm/hPa] u in m/s

    Slope of the saturation vapor curve s=4098T / (237.3+T) [hPa/K] T in C

    Latent heat of water L=2501-2.37T [kJ/kg]

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    Zimmermann Hydrological Modeling 24

    Evapotranspiration: Comparison of ETP

    Potential Evapotranspiration Schluchsee/Black Forest

    0

    100

    200

    300

    400

    500

    600

    700

    800

    900

    88 89 90 91 92 93 94 95 mean

    Hydrological Years

    m

    m/a Rn / L

    PenmanPriestley-Taylor

    Haude forest

    Water balance P-R

    Variability of Evapotranspiration

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    Zimmermann Hydrological Modeling 25

    Variability of Evapotranspiration

    Evapotranspiration acc. to Haude and climatic water balance DWD

    Weihenstephan 1991-2001

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    Zimmermann Hydrological Modeling 26

    Soil water

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    Zimmermann Hydrological Modeling 27

    Soil Retention: Measurement of Soil Moisture

    DataloggerSatellit

    Tensiometer,TDR-Sonde

    5

    13

    18

    9

    5cmThermofhler10cmThermofhler,TDR-Sonde20cmTensiometer,TDR-Sonde

    3m2m

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    Zimmermann Hydrological Modeling 28

    Measurement of soil water content by

    TDR (Time Domain Reflectometry)

    Quantity: volumetric water content [cm3/cm3 or volume-%)

    Principle:

    Retardation of propagation velocity of

    electromagnetic waves in wet soil

    High dielectric constant of water ( =82) compared todry soil ( < 5) and air ( = 1)

    Strong correlation between dielectric constant in thesoil and volumetric water content

    Annual variation of soil water content

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    Zimmermann Hydrological Modeling 29

    Annual variation of soil water content

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    Zimmermann Hydrological Modeling 30

    Matric potential

    The matric potential describes

    with how much energy, as a result

    of the soils capillary and

    adhesive forces, water is hold by

    the soil

    [hPa, cm WC]

    (Hewlett 1982)

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    A18

    180 185 190 195 200 205 210

    Rasterpunkte

    2

    4

    6

    8

    10

    1214

    16

    18

    Woche

    -800

    -700

    -600

    -500

    -400

    -300

    -200

    -100

    0

    Erosionspillway

    Gleyic

    featuresm.

    NN 465

    460

    455

    Surface Morphology

    and stratigraphy

    influence soil moisture

    and runoff generation

    Change of Matric Potentials within a Field

    Transect of tensiometers in 90 cm depth: change of matric potentials in dependent on

    site and slope position

    Annual variation of

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    Zimmermann Hydrological Modeling 32

    Annual variation of

    Open-field precipitation

    Potential evapotranspiration

    Matric potential (soil moisture)

    Snow cover

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    Zimmermann Hydrological Modeling 34

    Runoff: Measurement of Flow Velocity I

    R Runoff, discharge = flow velocity * river profile area A

    (width*water depth)

    R = v * A

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    Zimmermann Hydrological Modeling 35

    Runoff: Measurement of Flow Velocity II

    (Hewlett 1982)

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    Zimmermann Hydrological Modeling 36

    Runoff: Stage-Discharge Curve I

    Discharge [m3/s] = f (Water level (Stage))

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    Zimmermann Hydrological Modeling 37

    Runoff: Stage-Discharge Curve II

    (Hewlett 1982)

    E l f it i t d l t fl

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    Here, discharge and element concentration are

    continuously monitored and stored in a data

    logger.

    automaticsampler

    Datalogger

    60V-weir

    Laptop

    pressuregauge

    WieseBrache

    Acker 19

    Acker 20

    Fichtenwald

    BW4

    A1A2A3

    A4

    A5A6

    A7BN

    BE6

    BW1Waldrand

    Lage der Wehre und Drnagen

    100 m100 m

    Example for monitoring water and element fluxes

    Position of weirs and drains

    V-notch sharp crested weir

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    Zimmermann Hydrological Modeling 39

    V-notch, sharp crested weir

    Q=1.34*h2.48

    Defined relation

    between h and Q

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    Zimmermann Hydrological Modeling 40

    Catchment area

    (Hewlett 1982)

    C t h t I

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    Zimmermann Hydrological Modeling 41

    Catchment I

    Surface catchment

    Underground catchment

    permeable

    impermeable

    Ground water

    Water divide

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    Zimmermann Hydrological Modeling 42

    Catchment II

    Definition:

    A catchment is the area in horizontal projection in km, limited

    by water divides through which at a certain point of the river all

    discharge originates

    The water divide can be constructed in a topographical map

    including isohypses. It starts from a point at the river (river

    profile) by cutting the isohypses vertically.

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    Zimmermann Hydrological Modeling 43

    Surface and Subsurface Catchment

    G d t D fi iti I

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    Zimmermann Hydrological Modeling 44

    Groundwater Definitions I

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    Fl i i d d l

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    Zimmermann Hydrological Modeling 46

    Flow regime in dependence on geology

    Salt river:impermeable, shallow soils

    (clayey glacial till)

    Manistee River:

    deep, permeabale soils

    Structure of the lecture

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    Zimmermann Hydrological Modeling 47

    Structure of the lecture

    1. Water budget and its components (Review)

    2. Model theory for water budget models

    3. Change of land use and effects for water and

    element budget

    4. Climate change scenarios

    5. Practical examples with BROOK90

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    Natural Land use change

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    Zimmermann Hydrological Modeling 49

    Bavarian Forest

    National Park

    No counter-

    measures against

    bark beetles

    Water Budget Model as Scenario Tool

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    Zimmermann Hydrological Modeling 50

    g

    State of the System

    Hydrometeorology River bed parameter Basin characterisitics

    Discharge

    Input for Water quality and ground water models

    Change in the state of the system (scenario) controllable

    Operational forecast

    What is a system a process a model?

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    Zimmermann Hydrological Modeling 51

    What is a system, a process, a model?

    Input p Output qSystem

    P-q=dS/dt

    A model describes a system and its processes.

    A system is an unit of elements which is separated from its environment and

    relates an input of element, energy or information to an output of element, energy

    or information in its time pattern to each other.

    A process is defined as quantitative or qualitative change with time. For

    hydrological processes, in most cases, the coordinates of a water body or

    particle are changed, together with a change in temperature, pressure or other

    properties of water. They are often non-linear.

    The operation of the system is modelled.

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    Zimmermann Hydrological Modeling 52

    Model requirements

    A model should include:

    basic laws (cont inui ty , geometry, boundary co ndi t ions)

    st ructure of the sy stem

    parameters of the system

    A model is an idealized abstraction of reality. Models should berepresetative of real systems.

    Hydrological System

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    Zimmermann Hydrological Modeling 53

    Hydrological System

    A catchment (watershed) or a defined section between two

    gauges at a river or a lake is a system.

    It consists out of subsystems like land surface (plant canopy),soil, groundwater, river bed, epi- and hypolimnion etc.

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    Zimmermann Hydrological Modeling 54

    Classification of hydrological models

    Aim of the model application?

    real-time forecasting, scenarios, planning

    Which type of system is modelled?

    aquifers, catchment, river section

    Which hydrological process or variable?

    infiltration, ET, ground water recharge

    Which degree of deterministic behaviour (cause-effect

    relationships)?

    Overview of hydrological models

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    Zimmermann Hydrological Modeling 55

    Deterministic Models

    (Cause-Effect-Relations

    Stochastic Models

    (Statistical relations)

    Fundamental

    Laws (Hydrodynam.)

    Conceptual

    Models

    Black Box

    Models

    Distributed Models

    (areal-detailed information)

    Lumped Models

    (no/coarse spatial partitioning)

    Elementary

    Unit Areas

    Larger

    Subareas

    Statistical

    distribution

    No

    DistributionRaster

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    Description of process in dependence on spatial

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    Zimmermann Hydrological Modeling 57

    process resolution (acc.to Becker 1995)

    Conceptual models>1000 km2>30 kmmacro

    Physically based

    conceptual models0,01-1000 km20,1 30 kmmeso

    Basic

    physical laws< 0,01 km2< 100 mmicro

    Process

    description

    AreaLengthScale

    Discretization in space and time

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    Zimmermann Hydrological Modeling 58

    Discretization in space and time

    Discretization in time

    According to the aim of the modeling different time steps have to be

    used (e.g. floods, urban drainage down to minutes, water budget

    daily to monthly)

    Discretization in space

    Input data, parameters which describe the basin (topography, land

    use, soils)and resulting fluxes of energy and mass are spatially

    heterogeneous

    Raster, homogeneous areas, largersubareas or statistical distribution

    Example spatial discretization

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    Zimmermann Hydrological Modeling 59

    Subcatchments as block

    models

    Zones or hydrotopes,

    for element transport furtherseparated into segments or

    cascades

    Regular raster

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    Complex hydrological factors: hydrotopes

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    Zimmermann Hydrological Modeling 61

    Errors in hydrological models

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    Zimmermann Hydrological Modeling 62

    Error of model:

    Decreases with increasing model complexity

    Error of measurement (input data)

    Increases with increasing model complexity since datademand increase

    Total errorerror

    Model complexity

    Input error

    model error

    Lumped Water Budget Model

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    Zimmermann Hydrological Modeling 63

    Deterministic Models

    (Cause-Effect-Relations

    Stochastic Models

    (Statistical relations)

    Fundamental

    Laws (Hydrodynam.)

    Conceptual

    Models

    Black Box

    Models

    Distributed Models

    (areal-detailed information)

    Lumped Models

    (no/coarse spatial partitioning)

    Elementary

    Unit Areas

    Larger

    Subareas

    Statistical

    distribution

    No

    Distribution

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    Input data- in general

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    Zimmermann Hydrological Modeling 65

    Process variablesPrecipitation, global radiation or sunshine duration, relative humidity, air

    temperature, wind

    Physical plot or basin characteristicsCatchment area, latitude, slope, exposition, mean elevation height, land use,

    porosity of the soil, field capacity, permanent wilting point, root depth, land use,

    LAI etc.

    Model parameterprecipitation correction, interception and land surface storage capacity, storage

    constants, percentage of overland flow, temperature limit for snow/rain, snow

    melt temperature, day degree factor for snow melt, retention factor for snow

    cover, starting values for the storages

    Test and control dataDischarge, percentage of ground water flow, soil moisture and

    evapotranspiration measurements at certain points

    Lumped Water Budget Model BROOK90

    Short description

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    Zimmermann Hydrological Modeling 66

    p

    Modeling of subsystem:Precipitation

    Precipitation PREC has to be

    corrected for systematic

    undercatch outside the model

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    Zimmermann Hydrological Modeling 67

    while pre-processing the

    meteorological input data, then

    division into snowfall fraction(SFAL) and rainfall (RFAL),

    these are further divided into

    the fractions which are

    intercepted (SINT, RINT) and

    which fall through the canopy

    (RTHR, RTHR). Throughfall isfurther reduced by the amount

    of rain which is stored within

    the snow cover(SNOW). The

    snow cover is reduced by

    evaporation (SNVP) and

    snow melt (SMLT) while thelast is added with the remaining

    throughfall to the net rainfall

    (RNET).

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    Modeling of subsystem:Runoff formation

    Net rainfall RNET is dividedinto surface runoff (SRFL) and

    into infiltration into the soil

    (SLFL). The soil water

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    Zimmermann Hydrological Modeling 69

    ( )

    storage (SWATI (1->n))

    consists of several layers. The

    infiltration SLFL which can beregarded as fast deep

    infiltration by macropores is

    divided into two components

    within the soil: first infiltration

    by macropores in each layer

    (INFL(1->n)) of the soil matrix,second a fast downslope

    bypass flow through pipes

    (BYFL(1->n)) which does not

    enter the soil matrix. Within the

    soil we have a vertical matrix

    flow (VRFL(I)), when layersare saturated another

    downslope, slow flow (DSFL)

    is generated.

    Lumped Water Budget Model BROOK90Flow components

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    Zimmermann Hydrological Modeling 70

    SRFL:

    Overland flow

    BYFL:Bypass flow

    SLFL:

    surface infiltration

    INFL:

    macropore infiltrationVRFL:

    vertical matric flow

    DSFL:

    slope parallel interflow

    GWFL:ground water flow

    FLOW=SRFL+BYFL+DSFL+GWFL

    Modeling of subsystem:Evapotranspiration

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    Zimmermann Hydrological Modeling 71

    From each soil layer according

    to root density water is

    withdrawn throughtranspiration (TRAN(I->n)),

    from the first soil layer in

    addition also soil evaporation

    (SLVP) takes place, if snow

    cover is present snow

    evaporation (SNVP) as well,the interception storages

    (INTR, INTS) are emptied as

    well by interception

    evaporation (IRVP, ISVP)

    Input data- Brook90

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    Zimmermann Hydrological Modeling 72

    Process variables [unit] in dfile.dat

    global radiation [MJ cm-2d-1]maximum and minimum of air temperature [C]

    vapour pressure [kPa]

    wind speed [m/s]

    precipitation [mm/d]

    Discharge [mm/d]

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