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Physical Climatology: Principles

GEOG 5211/4211 - Fall 2003

Professor Konrad Steffen
CIRES Ekeley Building, S264
Tel o: 492 4524
e-mail konrad.steffen@colorado.edu


Field Excursion: November 9 & 23, 2003

Exercises on the evaluation of energy and mass fluxes in the surface boundary layer, on instrumentation for energy flux measurements, and on climates of vegetated surfaces. 

1. Describe the instrumentation need for turbulent energy flux measurements (sensible, latent) based on the gradient method, for radiation balance, and for ground heat flux.

2. What is the Richardson Number and why do we use a stability function for the derivation of convective fluxes?

3. In the following two different sets of measurements are given.

    a)    Calculate the Richardson Number for both cases.
    b)    Plot the temperature and wind profile on semi-logarithmic paper; e.g., log(z) versus T and V.
    c)    Derive the roughness length for both data sets (use plot of log(z) versus V)
    d)    Discuss the two profiles in the context of the atmospheric stability.
    e)    Derive the radiation balance and the albedo from the two date sets.        
    f)    Calculate the sensible and latent heat flux for both data sets and use the stability function if needed. To derive the vapor pressure from the measured relative humidity use the following approximation:
                Relative Humidity = 100 (e/es)
                vapor density  r = 2.17 e / T;     e[Pa], T[K]
                e = vapor pressure
                es = saturation vapor pressure
                P = pressure

Table for saturation vapor pressure:  sat_vapor_table.pdf

    QH=[-Cak2(du * dT)/(ln(z2/z1))2] X
    Ca : heat capacity of the air = 0.0012 106 J m-3 K-1
    QE=[-Lvk2(du *dr)/(ln(z2/z1))
2] X
    Lv : latent heat of vaporization = 2.52 106 J kg-1
    X: factor stable condition = (1-5 Ri)
2          
                X: factor unstable condition = (1-16 Ri)3/4               
    g)    Derive the ground heat flux as residual of the above calculated energy balance.
    h)    Calculate the Bowen ratio for both case studies.

Instruments heights: Level 1= 0.2 m; level 2 = 0.6 m; level 3 = 1.3 m

JD_time      Net R.    S(refl)    S(in)          V1    V2       V3       T1     T2     T3        H1     H2       H3    P
                   W/m
2     W/m2    W/m2        ms-1   ms-1     ms-1       C      C        C       %       %          %       mb
303.5521    36.35    199.08   273.81    .97    1.43     1.65     -7.7    -8.0    -8.3    76.0    82.6    87.7    835.66  
306.8542    -58.67     .00       .00          .88    1.11     1.35   -13.0  -12.2  -11.7    68.9    67.5    65.7    836.26      

V: wind speed    H: relative humidity    P: pressure   
Net R.: net radiation    S(refl).: short-wave reflected radiation    S(in): short-wave incoming radiation


The relative calibration data from the field class can be downloaded : ftp://seaice.colorado.edu/pub/class