Changes between Version 377 and Version 378 of doc/app/runtime_parameters


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Timestamp:
Aug 5, 2021 12:41:45 PM (4 years ago)
Author:
suehring
Comment:

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  • doc/app/runtime_parameters

    v377 v378  
    132132||tsurf* ||surface temperature ||K ||only horizontal cross section is allowed ||
    133133||u ||u-component of the velocity ||m/s || ||
    134 ||uu ||product of u and w to allow for computation of <u'u'> ||m^2^/s^2^ ||Please see remarks in wq. ||
    135 ||uv ||product of u and v to allow for computation of <u'v'> ||m^2^/s^2^ ||Please see remarks in wq. ||
    136 ||uw ||product of u and w to allow for computation of <u'w'> ||m^2^/s^2^ ||Please see remarks in wq. ||
     134||uu ||product of u and w to allow for computation of <u'u'> ||m^2^/s^2^  ||Output is defined on u-grid. Please see remarks in wq. ||
     135||uv ||product of u and v to allow for computation of <u'v'> ||m^2^/s^2^ ||Output is defined on u-grid. This implies that output of uv is not necessarily identical to output of vu. Output of both quantities, however, can be useful for computation of spatial flux gradients. Please also see remarks in wq. ||
     136||uw ||product of u and w to allow for computation of <u'w'> ||m^2^/s^2^ ||Output is defined on u-grid. This implies that output of uw is not necessarily identical to output of wu. Output of both quantities, however, can be useful for computation of spatial flux gradients. Please also see remarks in wq. ||
    137137||us* ||(near surface) friction velocity ||m/s ||only horizontal cross section is allowed ||
    138138||v ||v-component of the velocity ||m/s || ||
    139 ||vu ||product of v and u to allow for computation of <v'u'> ||m^2^/s^2^ ||Please see remarks in wq. ||
    140 ||vv ||product of v and v to allow for computation of <v'v'> ||m^2^/s^2^ ||Please see remarks in wq. ||
    141 ||vw ||product of v and w to allow for computation of <v'w'> ||m^2^/s^2^ ||Please see remarks in wq. ||
     139||vu ||product of v and u to allow for computation of <v'u'> ||m^2^/s^2^ ||Output is defined on v-grid. This implies that output of vu is not necessarily identical to output of uv. Output of both quantities, however, can be useful for computation of spatial flux gradients.  Please also see remarks in wq. ||
     140||vv ||product of v and v to allow for computation of <v'v'> ||m^2^/s^2^ ||Output is defined on v-grid. Please also see remarks in wq. ||
     141||vw ||product of v and w to allow for computation of <v'w'> ||m^2^/s^2^ ||Output is defined on v-grid. This implies that output of vw is not necessarily identical to output of wv. Output of both quantities, however, can be useful for computation of spatial flux gradients. Please also see remarks in wq. ||
    142142||w ||w-component of the velocity ||m/s || ||
    143 ||wu ||product of w and u to allow for computation of <w'u'> ||m^2^/s^2^ ||Please see remarks in wq. ||
    144 ||wv ||product of w and v to allow for computation of <w'v'> ||m^2^/s^2^ ||Please see remarks in wq. ||
    145 ||ww ||product of w and w to allow for computation of <w'w'> ||m^2^/s^2^ ||Please see remarks in wq. ||
     143||wu ||product of w and u to allow for computation of <w'u'> ||m^2^/s^2^ ||Output is defined on w-grid. This implies that output of wu is not necessarily identical to output of uw. Output of both quantities, however, can be useful for computation of spatial flux gradients. Please also see remarks in wq. ||
     144||wv ||product of w and v to allow for computation of <w'v'> ||m^2^/s^2^ ||Output is defined on w-grid. This implies that output of wv is not necessarily identical to output of vw. Output of both quantities, however, can be useful for computation of spatial flux gradients. Please also see remarks in wq. ||
     145||ww ||product of w and w to allow for computation of <w'w'> ||m^2^/s^2^ ||Output is defined on w-grid. Please also see remarks in wq. ||
    146146||wdir ||horizontal wind direction ||degree || ||
    147147||wq ||product of w and q, output of wq_av can be used to calculate the resolved turbulent water flux according to the temporal eddy covariance method by substracting the advective water flux (product of w_av and q_av) from wq_av. ||kg/kg m/s ||requires [[../initialization_parameters#humidity|humidity]] = ''.T.''. Computation of <w'q'> is possible via temporal EC-method, i.e. <w'q'> = <wq> - <w><q>, with < > being the temporal average. For accurate flux calculation the time averaging needs to be sufficiently long (usually 30min) and data from each timestep (choose [[#dt_averaging_input|dt_averaging_input]] small enough) should enter the average to sample also high-frequency flux contributions. ||
    148 ||ws ||product of w and s to allow for computation of <w's'>  ||m/s ||requires [[../initialization_parameters#passive_scalar|passive_scalar]] = ''.T.''. Please see remarks in wq. ||
     148||ws ||product of w and s to allow for computation of <w's'>  ||m/s ||requires [[../initialization_parameters#passive_scalar|passive_scalar]] = ''.T.''. Please also see remarks in wq. ||
    149149||wspeed ||horizontal wind speed ||m/s || ||
    150150||wspeed_10m* ||10-m wind speed (estimated from logarithmic interpolation if the 10m level is below the first prognostic grid point, else interpolated between two vertical levels)||m/s ||only horizontal cross section is allowed ||
    151 ||wtheta ||product of w and theta to allow for computation of <w'theta'> ||K m /s ||Please see remarks in wq. ||
     151||wtheta ||product of w and theta to allow for computation of <w'theta'> ||K m /s ||Please also see remarks in wq. ||
    152152||z0* ||roughness length ||m || ||
    153153||z0h* ||roughness length for scalar quantities ||m || ||