Changes between Version 275 and Version 276 of doc/app/initialization_parameters


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Timestamp:
Apr 7, 2016 12:18:24 PM (9 years ago)
Author:
hoffmann
Comment:

--

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  • doc/app/initialization_parameters

    v275 v276  
    26842684|----------------
    26852685{{{#!td style="vertical-align:top;width: 150px"
    2686 [=#curvature_solution_effects '''curvature_solution_effects''']
     2686[=#c_sedimentation '''c_sedimentation''']
     2687}}}
     2688{{{#!td style="vertical-align:top;width: 50px"
     2689R
     2690}}}
     2691{{{#!td style="vertical-align:top;width: 75px"
     26922.0
     2693}}}
     2694{{{#!td
     2695Courant number for sedimentation process.
     2696
     2697A Courant number that is too big inhibits microphysical interactions of the sedimented quantity. There is no need to use the limiter ([#limiter_sedimentation limiter_sedimentation]) if [#c_sedimentation c_sedimentation] <= 1.0.
     2698
     2699This parameter only comes into effect if the microphysical cloud scheme according to Seifert and Beheng (2006) is used ([#cloud_scheme cloud_scheme] = 'seifert_beheng').
     2700}}}
     2701|----------------
     2702{{{#!td style="vertical-align:top;width: 150px"
     2703[=#cloud_water_sedimentation '''cloud_water_sedimentation''']
     2704}}}
     2705{{{#!td style="vertical-align:top;width: 50px"
     2706L
     2707}}}
     2708{{{#!td style="vertical-align:top;width: 75px"
     2709.T.
     2710}}}
     2711{{{#!td
     2712Parameter to consider sedimentation of cloud water according to Ackermann et al. (2009, MWR).
     2713
     2714This parameter only comes into effect if the microphysical cloud scheme according to Seifert and Beheng (2006) ([#cloud_scheme cloud_scheme] = 'seifert_beheng') or by Kessler (1969)  ([#cloud_scheme cloud_scheme] = 'kessler') is used.
     2715}}}
     2716|----------------
     2717{{{#!td style="vertical-align:top;width: 150px"
     2718[=#limiter_sedimentation '''limiter_sedimentation''']
     2719}}}
     2720{{{#!td style="vertical-align:top;width: 50px"
     2721L
     2722}}}
     2723{{{#!td style="vertical-align:top;width: 75px"
     2724.T.
     2725}}}
     2726{{{#!td
     2727Slope limiter in sedimentation process according to Stevens and Seifert (2008).
     2728
     2729This parameter only comes into effect if the microphysical cloud scheme according to Seifert and Beheng (2006) is used ([#cloud_scheme cloud_scheme] = 'seifert_beheng').
     2730
     2731If [#c_sedimentation c_sedimentation] <= 1.0 there is no need to use the limiter.
     2732}}}
     2733|----------------
     2734{{{#!td style="vertical-align:top;width: 150px"
     2735[=#nc_const '''nc_const''']
     2736}}}
     2737{{{#!td style="vertical-align:top;width: 50px"
     2738R
     2739}}}
     2740{{{#!td style="vertical-align:top;width: 75px"
     274170.0E6
     2742}}}
     2743{{{#!td
     2744Fixed cloud droplet number density (in 1/m^3^). The default value is applicable for marine conditions.
     2745
     2746This parameter only comes into effect if the microphysical cloud scheme according to Seifert and Beheng (2006) is used ([#cloud_scheme cloud_scheme] = 'seifert_beheng').
     2747}}}
     2748|----------------
     2749{{{#!td style="vertical-align:top;width: 150px"
     2750[=#collision_turbulence '''collision_turbulence''']
    26872751}}}
    26882752{{{#!td style="vertical-align:top;width: 50px"
     
    26932757}}}
    26942758{{{#!td
    2695 Parameter to consider solution and curvature effects on the equilibrium vapor pressure of cloud droplets.
    2696 
    2697 This parameter only comes into effect if Lagrangian cloud droplets are used (see [#cloud_droplets cloud_droplets]) and if the droplet radius is smaller than ''1.0E-6'' m. In case of '''curvature_solution_effects''' = ''.T.'', solution and curvature effects are included in the growth equation of droplets by condensation. Since in this case the growth equation is a stiff o.d.e, it is integrated in time using the Rosenbrock method (see Numerical Recipes in FORTRAN, 2nd Edition, p.731). If the droplet radius is larger or equal ''1.0E-6'' m, solution and curvature effects are neglected and the growth is calculated by a simple analytic formula (as for '''curvature_solution_effects''' = ''.F.'').\\\\
    2698 '''Attention:''' '''curvature_solution_effects''' = ''.T.'' may significantly increase CPU time of jobs.
    2699 }}}
    2700 |----------------
    2701 {{{#!td style="vertical-align:top;width: 150px"
    2702 [=#c_sedimentation '''c_sedimentation''']
    2703 }}}
    2704 {{{#!td style="vertical-align:top;width: 50px"
    2705 R
    2706 }}}
    2707 {{{#!td style="vertical-align:top;width: 75px"
    2708 2.0
    2709 }}}
    2710 {{{#!td
    2711 Courant number for sedimentation process.
    2712 
    2713 A Courant number that is too big inhibits microphysical interactions of the sedimented quantity. There is no need to use the limiter ([#limiter_sedimentation limiter_sedimentation]) if [#c_sedimentation c_sedimentation] <= 1.0.
    2714 
    2715 This parameter only comes into effect if the microphysical cloud scheme according to Seifert and Beheng (2006) is used ([#cloud_scheme cloud_scheme] = 'seifert_beheng').
    2716 }}}
    2717 |----------------
    2718 {{{#!td style="vertical-align:top;width: 150px"
    2719 [=#drizzle '''drizzle''']
    2720 }}}
    2721 {{{#!td style="vertical-align:top;width: 50px"
    2722 L
    2723 }}}
    2724 {{{#!td style="vertical-align:top;width: 75px"
    2725 .T.
    2726 }}}
    2727 {{{#!td
    2728 Parameter to consider sedimentation of cloud water according to Ackermann et al. (2009, MWR).
    2729 
    2730 This parameter only comes into effect if the microphysical cloud scheme according to Seifert and Beheng (2006) is used ([#cloud_scheme cloud_scheme] = 'seifert_beheng').
    2731 }}}
    2732 |----------------
    2733 {{{#!td style="vertical-align:top;width: 150px"
    2734 [=#limiter_sedimentation '''limiter_sedimentation''']
    2735 }}}
    2736 {{{#!td style="vertical-align:top;width: 50px"
    2737 L
    2738 }}}
    2739 {{{#!td style="vertical-align:top;width: 75px"
    2740 .T.
    2741 }}}
    2742 {{{#!td
    2743 Slope limiter in sedimentation process according to Stevens and Seifert (2008).
    2744 
    2745 This parameter only comes into effect if the microphysical cloud scheme according to Seifert and Beheng (2006) is used ([#cloud_scheme cloud_scheme] = 'seifert_beheng').
    2746 
    2747 If [#c_sedimentation c_sedimentation] <= 1.0 there is no need to use the limiter.
    2748 }}}
    2749 |----------------
    2750 {{{#!td style="vertical-align:top;width: 150px"
    2751 [=#nc_const '''nc_const''']
    2752 }}}
    2753 {{{#!td style="vertical-align:top;width: 50px"
    2754 R
    2755 }}}
    2756 {{{#!td style="vertical-align:top;width: 75px"
    2757 70.0E6
    2758 }}}
    2759 {{{#!td
    2760 Fixed cloud droplet number density (in 1/m^3^). The default value is applicable for marine conditions.
    2761 
    2762 This parameter only comes into effect if the microphysical cloud scheme according to Seifert and Beheng (2006) is used ([#cloud_scheme cloud_scheme] = 'seifert_beheng').
    2763 }}}
    2764 |----------------
    2765 {{{#!td style="vertical-align:top;width: 150px"
    2766 [=#turbulence '''turbulence''']
    2767 }}}
    2768 {{{#!td style="vertical-align:top;width: 50px"
    2769 L
    2770 }}}
    2771 {{{#!td style="vertical-align:top;width: 75px"
    2772 .F.
    2773 }}}
    2774 {{{#!td
    2775 Turbulence effects on autoconversion and accretion according to Seifert, Nuijens and Stevens (2010).
     2759Turbulence effects on the collision process, namely the autoconversion and accretion according to Seifert, Nuijens and Stevens (2010).
    27762760
    27772761This parameter only comes into effect if the microphysical cloud scheme according to Seifert and Beheng (2006) is used ([#cloud_scheme cloud_scheme] = 'seifert_beheng').