Changes between Version 28 and Version 29 of doc/tec/lsm


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Timestamp:
Apr 15, 2016 1:56:12 PM (9 years ago)
Author:
maronga
Comment:

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  • doc/tec/lsm

    v28 v29  
    294294
    295295For more details, see also [#viterbo Viterbo et al. (1995)] and [#balsamo Balsamo et al. (2009)].
     296
     297== Exception: water surfaces ==
     298When prescribing grid points with water surface (i.e. {{{veg_class = 14,15}}}), the energy balance is solved as for land surface without evaporation from vegetation canopy and bare soil. Moreover, the water temperature is constant and time and is derived from the value of {{{pt_surface}}} at model start. In order to obtain realistic results, it is required to set a zero heat capacity for the ocean skin layer (e.g. {{{c_surface = 0.0}}}).
     299
     300A special feature of the treatment of water surfaces is the treatment of surface roughness chances due to water waves. The roughness lengths for momentum, heat, and moisture (''z'',,0,,, ''z'',,0,h,,, and ''z'',,0,q, respectively) are hence calculated after [#beljaars Beljaars (1994)] at each grid point as:
     301{{{
     302#!Latex
     303\begin{align*}
     304z_0 &= \dfrac{0.11 \nu}{u_\ast} + \alpha_\mathrm{Ch} \dfrac{u_\ast^2}{g}
     305z_\mathrm{0,h} &= \dfrac{0.4 \mu}{u_\ast}
     306z_\mathrm{0,h} &= \dfrac{0.62 \mu}{u_\ast}
     307\end{align*}
     308}}}
     309Here, ''ν'' is the molecular viscosity, and ''α'',,Ch,, = 0.018 is the Charnock constant taken from the ECMWF-IFS model.
     310
     311Please note that this parameterization was developed for large-scale models where waves are a pure subgrid-scale phenomenon. When using large-eddy simulations, however, this might no longer be the case. It has not been studies whether this parameterization is appropriate in such cases and should only be used with caution.
     312
     313== Exception: pavement ==
     314
     315
     316
    296317
    297318== Technical details ==
     
    345366}}}
    346367
    347 === Exception: water surfaces ===
    348 When prescribing grid points with water surface (i.e. {{{veg_class = 14,15}}}), the energy balance is solved as for land surface without evaporation from vegetation canopy and bare soil. Moreover, the water temperature is constant and time and is derived from the value of {{{pt_surface}}} at model start. In order to obtain realistic results, it is required to set a zero heat capacity for the ocean skin layer (e.g. {{{c_surface = 0.0}}}).
    349 
    350 A special feature of the treatment of water surfaces is the treatment of surface roughness chances due to water waves. The roughness lengths for momentum, heat, and moisture (''z'',,0,,, ''z'',,0,h,,, and ''z'',,0,q, respectively) are hence calculated after [#beljaars Beljaars (1994)] at each grid point as:
    351 {{{
    352 #!Latex
    353 \begin{align*}
    354 z_0 &= \dfrac{0.11 \nu}{u_\ast} + \alpha_\mathrm{Ch} \dfrac{u_\ast^2}{g}
    355 z_\mathrm{0,h} &= \dfrac{0.4 \mu}{u_\ast}
    356 z_\mathrm{0,h} &= \dfrac{0.62 \mu}{u_\ast}
    357 \end{align*}
    358 }}}
    359 Here, ''ν'' is the molecular viscosity, and ''α'',,Ch,, = 0.018 is the Charnock constant taken from the ECMWF-IFS model.
    360 
    361 Please note that this parameterization was developed for large-scale models where waves are a pure subgrid-scale phenomenon. When using large-eddy simulations, however, this might no longer be the case. It has not been studies whether this parameterization is appropriate in such cases and should only be used with caution.
    362 
    363 === Exception: pavement ===
    364 
    365 
    366368
    367369== Job preparation ==