source: palm/trunk/DOC/app/chapter_4.6.html @ 100

Last change on this file since 100 was 97, checked in by raasch, 17 years ago

New:
---
ocean version including prognostic equation for salinity and equation of state for seawater. Routine buoyancy can be used with both temperature and density.
+ inipar-parameters bc_sa_t, bottom_salinityflux, ocean, sa_surface, sa_vertical_gradient, sa_vertical_gradient_level, top_salinityflux

advec_s_bc, average_3d_data, boundary_conds, buoyancy, check_parameters, data_output_2d, data_output_3d, diffusion_e, flow_statistics, header, init_grid, init_3d_model, modules, netcdf, parin, production_e, prognostic_equations, read_var_list, sum_up_3d_data, swap_timelevel, time_integration, user_interface, write_var_list, write_3d_binary

New:
eqn_state_seawater, init_ocean

Changed:


inipar-parameter use_pt_reference renamed use_reference

hydro_press renamed hyp, routine calc_mean_pt_profile renamed calc_mean_profile

format adjustments for the ocean version (run_control)

advec_particles, buoyancy, calc_liquid_water_content, check_parameters, diffusion_e, diffusivities, header, init_cloud_physics, modules, production_e, prognostic_equations, run_control

Errors:


Bugfix: height above topography instead of height above level k=0 is used for calculating the mixing length (diffusion_e and diffusivities).

Bugfix: error in boundary condition for TKE removed (advec_s_bc)

advec_s_bc, diffusion_e, prognostic_equations

  • Property svn:keywords set to Id
File size: 115.8 KB
RevLine 
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[40]2<html><head>
[62]3<meta http-equiv="CONTENT-TYPE" content="text/html; charset=windows-1252"><title>PALM chapter 4.6</title> <meta name="GENERATOR" content="StarOffice 7 (Win32)"> <meta name="AUTHOR" content="Marcus Oliver Letzel"> <meta name="CREATED" content="20041103;9554421"> <meta name="CHANGED" content="20041117;12591937"> <meta name="KEYWORDS" content="parallel LES model"> <style>
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[61]7</style></head>
8<body style="direction: ltr;" lang="en-US"><h3>4.6
9Listing of the steering parameters in alphabetical order<br>
10</h3><p style="margin-bottom: 0cm;">Initialization
11parameters
[5]12(class = I),
13run parameters (R), package parameters (P) as well as user-defined
14parameters (U) are alphabetically listed in the following table. <br>
15&nbsp;
[61]16</p><p style="margin-bottom: 0cm;" align="center"><br>
17</p><table style="width: 100%;" border="1" cellpadding="2" cellspacing="4"> <col width="38*">
18<col width="12*"> <col width="18*"> <col width="42*"> <col width="146*"> <tbody>
19<tr> <td style="vertical-align: middle;" width="15%">
20<h3><b>Parameter name</b></h3> </td> <td style="vertical-align: middle;" width="5%"> <h3>Class</h3>
21</td> <td style="vertical-align: middle;" width="7%">
22<h3>Type</h3> </td> <td style="vertical-align: middle;" width="16%"> <h3>Default<br>
23value</h3> </td> <td style="vertical-align: middle;" width="57%"> <h3>Explanation</h3> </td> </tr>
24<tr> <td style="vertical-align: middle;" width="15%">
25<p><a href="chapter_4.1.html#adjust_mixing_length"><b>adjust_mixing_length</b></a></p>
26</td> <td style="vertical-align: middle;" width="5%">
27<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>L</p>
28</td> <td style="vertical-align: middle;" width="16%">
29<p><i>.F.</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Near-surface
30adjustment of the
31mixing length to the Prandtl-layer law.</p> </td> </tr>
32<tr> <td style="vertical-align: middle;" width="15%">
33<p><a href="chapter_4.1.html#alpha_surface"><b>alpha_surface</b></a></p>
34</td> <td style="vertical-align: middle;" width="5%">
35<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
36</td> <td style="vertical-align: middle;" width="16%">
37<p><i>0.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Inclination
38of the model domain
39with respect to the horizontal (in degrees).</p> </td> </tr>
40<tr> <td><a href="chapter_4.2.html#averaging_interval"><span style="font-weight: bold;">averaging_interval</span></a></td>
41<td>R</td> <td>R</td> <td><span style="font-style: italic;">0.0</span></td> <td>Averaging
42interval for all&nbsp;output of temporally averaged data (in s).</td>
43</tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#averaging_interval_pr"><b>averaging_interval_pr</b></a></p>
44</td> <td style="vertical-align: middle;" width="5%">
45<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
46</td> <td style="vertical-align: middle;" width="16%"><span style="font-style: italic;">value of <a href="chapter_4.2.html#averaging_interval">averaging_<br>
47interval</a></span></td> <td style="width: 57%; text-align: left; vertical-align: middle;">
48Averaging interval for vertical profiles&nbsp;output to local
49file <font color="#000000"><font color="#000000"><a href="chapter_3.4.html#DATA_1D_PR_NETCDF">DATA_1D_PR_NETCDF</a>
50</font></font>and/or&nbsp; <a href="chapter_3.4.html#PLOT1D_DATA">PLOT1D_DATA</a>
51(in s).&nbsp;</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#averaging_interval_sp"><b>averaging_interval_sp</b></a></p>
52</td> <td style="vertical-align: middle;" width="5%">
53<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
54</td> <td style="vertical-align: middle;" width="16%"><span style="font-style: italic;">value of <a href="chapter_4.2.html#averaging_interval">averaging_<br>
55interval</a></span></td> <td style="vertical-align: middle;" width="57%">Averaging
56interval for spectra output to local
57file <font color="#000000"><font color="#000000"><a href="chapter_3.4.html#DATA_1D_SP_NETCDF">DATA_1D_SP_NETCDF</a>
58</font></font>and/or&nbsp; <a href="chapter_3.4.html#PLOTSP_X_DATA">PLOTSP_X_DATA</a>
59/ &nbsp;&nbsp; <a href="chapter_3.4.html#PLOTSP_Y_DATA">PLOTSP_Y_DATA</a>
60(in s).&nbsp;</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#bc_e_b"><b>bc_e_b</b></a></p>
61</td> <td style="vertical-align: middle;" width="5%">
62<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
63* 20</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'neumann'</i></p>
64</td> <td style="vertical-align: middle;" width="57%">
65<p>Bottom boundary condition of the
66TKE. <br> </p> </td> </tr> <tr> <td style="vertical-align: middle;"><b><a href="chapter_4.1.html#bc_lr"><b>bc_lr</b></a></b></td>
67<td style="vertical-align: middle;">I<br> </td>
68<td style="vertical-align: middle;">C * 20<br> </td>
69<td style="vertical-align: middle;"><span style="font-style: italic;">&acute;cyclic&acute;</span><br>
70</td> <td style="vertical-align: middle;">Boundary
71condition along x (for all quantities).</td> </tr> <tr>
72<td style="vertical-align: middle;"><b><b><a href="chapter_4.1.html#bc_ns"><b>bc_ns</b></a></b></b></td>
73<td style="vertical-align: middle;">I<br> </td>
74<td style="vertical-align: middle;">C * 20</td> <td style="vertical-align: middle;"><span style="font-style: italic;">'cyclic'</span></td>
75<td style="vertical-align: middle;">Boundary
76condition along y (for all quantities).</td> </tr> <tr>
77<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#bc_p_b"><b>bc_p_b</b></a></p>
78</td> <td style="vertical-align: middle;" width="5%">
79<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
80* 20</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'neumann'</i></p>
81</td> <td style="vertical-align: middle;" width="57%">
82<p>Bottom boundary condition of the
83perturbation pressure. <br> </p> </td> </tr>
84<tr> <td style="vertical-align: middle;" width="15%">
85<p><a href="chapter_4.1.html#bc_p_t"><b>bc_p_t</b></a></p>
86</td> <td style="vertical-align: middle;" width="5%">
87<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
88* 20</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'dirichlet'</i></p>
89</td> <td style="vertical-align: middle;" width="57%">
90<p>Top boundary condition of the
91perturbation pressure. <br> </p> </td> </tr>
92<tr> <td style="vertical-align: middle;"><b><a href="chapter_4.2.html#bc_par_b"><b>bc_par_b</b></a></b></td>
93<td style="vertical-align: middle;">P<br> </td>
94<td style="vertical-align: middle;">C*15</td> <td style="vertical-align: middle;"><i>&acute;reflect&acute;</i></td>
95<td style="vertical-align: middle;"> <p>Bottom
96boundary condition for particle transport. </p> </td> </tr>
97<tr> <td style="vertical-align: middle;"><b><a href="chapter_4.2.html#bc_par_lr"><b>bc_par_lr</b></a></b></td>
98<td style="vertical-align: middle;">P<br> </td>
99<td style="vertical-align: middle;">C*15</td> <td style="vertical-align: middle;"><i>&acute;cyclic&acute;</i></td>
100<td style="vertical-align: middle;">Lateral boundary
[5]101condition
102(x-direction) for particle
[61]103transport.</td> </tr> <tr> <td style="vertical-align: middle;"><b><a href="chapter_4.2.html#bc_par_ns"><b>bc_par_ns</b></a></b></td>
104<td style="vertical-align: middle;">P<br> </td>
105<td style="vertical-align: middle;">C*15</td> <td style="vertical-align: middle;"><i>&acute;cyclic&acute;</i></td>
106<td style="vertical-align: middle;">Lateral boundary
[5]107condition
108(y-direction) for particle
[61]109transport.</td> </tr> <tr> <td style="vertical-align: middle;"><b><a href="chapter_4.2.html#bc_par_t"><b>bc_par_t</b></a></b></td>
110<td style="vertical-align: middle;">P<br> </td>
111<td style="vertical-align: middle;">C*15</td> <td style="vertical-align: middle;"><i>&acute;absorb&acute;</i></td>
112<td style="vertical-align: middle;">Top boundary
[5]113condition for
[61]114particle transport.</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#bc_pt_b"><b>bc_pt_b</b></a></p>
115</td> <td style="vertical-align: middle;" width="5%">
116<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
117* 20</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'dirichlet'</i></p>
118</td> <td style="vertical-align: middle;" width="57%">
119<p>Bottom boundary condition of the
120potential temperature. <br> </p> </td> </tr>
121<tr> <td style="vertical-align: middle;" width="15%">
122<p><a href="chapter_4.1.html#pc_pt_t"><b>bc_pt_t</b></a></p>
123</td> <td style="vertical-align: middle;" width="5%">
124<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
[97]125* 20</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'initial_gradient'</i></p>
[61]126</td> <td style="vertical-align: middle;" width="57%">
127<p>Top boundary condition of the
128potential temperature. <br> </p> </td> </tr>
129<tr> <td style="vertical-align: middle;" width="15%">
130<p><a href="chapter_4.1.html#bc_q_b"><b>bc_q_b</b></a></p>
131</td> <td style="vertical-align: middle;" width="5%">
132<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
133* 20</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'dirichlet'</i></p>
134</td> <td style="vertical-align: middle;" width="57%">
135<p>Bottom boundary condition of the
136specific humidity / total water content. <br> </p> </td>
137</tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#bc_q_t"><b>bc_q_t</b></a></p>
138</td> <td style="vertical-align: middle;" width="5%">
139<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
140* 20</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'neumann'</i></p>
141</td> <td style="vertical-align: middle;" width="57%">
142<p>Top boundary condition of the
143specific humidity / total water content. <br> </p> </td>
144</tr> <tr valign="top"> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#bc_s_b"><b>bc_s_b</b></a></p>
145</td> <td style="vertical-align: middle;" width="5%">
146<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
147* 20</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'dirichlet'</i></p>
148</td> <td style="vertical-align: middle;" width="57%">
149<p>Bottom boundary condition of the
150scalar concentration. <br> </p> </td> </tr>
151<tr valign="top"> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#bc_s_t"><b>bc_s_t</b></a></p>
152</td> <td style="vertical-align: middle;" width="5%">
153<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
154* 20</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>&acute;neumann&acute;</i></p>
155</td> <td style="vertical-align: middle;" width="57%">
156<p>Top boundary condition of the
157scalar concentration. <br> </p> </td> </tr>
[97]158<tr><td align="undefined" valign="undefined"><a href="chapter_4.1.html#bc_sa_t"><span style="font-weight: bold;">bc_sa_t</span></a></td><td align="undefined" valign="undefined">I</td><td align="undefined" valign="undefined">C * 20</td><td align="undefined" valign="undefined"><span style="font-style: italic;">'neumann'</span></td><td align="undefined" valign="undefined">Top boundary condition of the salinity.&nbsp;</td></tr><tr> <td style="vertical-align: middle;" width="15%">
[61]159<p><a href="chapter_4.1.html#bc_uv_b"><b>bc_uv_b</b></a></p>
160</td> <td style="vertical-align: middle;" width="5%">
161<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
162* 20</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'dirichlet'</i></p>
163</td> <td style="vertical-align: middle;" width="57%">
164<p>Bottom boundary condition of the horizontal wind
[5]165components u
[61]166and v.</p> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#bc_uv_t"><b>bc_uv_t</b></a></p>
167</td> <td style="vertical-align: middle;" width="5%">
168<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
169* 20</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'dirichlet'</i></p>
170</td> <td style="vertical-align: middle;" width="57%">
171<p>Top boundary condition of the
172horizontal velocity components u and v.</p> </td> </tr>
[97]173<tr><td align="undefined" valign="undefined"><a href="chapter_4.1.html#bottom_salinityflux"><span style="font-weight: bold;">bottom_salinityflux</span></a></td><td align="undefined" valign="undefined">I</td><td align="undefined" valign="undefined">R</td><td align="undefined" valign="undefined"><span style="font-style: italic;">0.0</span></td><td align="undefined" valign="undefined">Kinematic salinity flux near the surface (in psu m/s).</td></tr><tr> <td style="font-weight: bold;"><a href="chapter_4.1.html#building_height">building_height</a></td>
[61]174<td>I</td> <td>R</td> <td style="font-style: italic;">50.0</td> <td>Height
175of a single building in m.</td> </tr> <tr> <td style="font-weight: bold;"><a href="chapter_4.1.html#building_length_x">building_length_x</a></td>
176<td>I</td> <td>R</td> <td style="font-style: italic;">50.0</td> <td>Width
177of a single building in m.</td> </tr> <tr> <td style="font-weight: bold;"><a href="chapter_4.1.html#building_length_y">building_length_y</a></td>
178<td>I</td> <td>R</td> <td style="font-style: italic;">50.0</td> <td>Depth
179of a single building in m.</td> </tr> <tr> <td style="font-weight: bold; vertical-align: middle;"><a href="chapter_4.1.html#building_wall_left">building_wall_left</a></td>
180<td style="vertical-align: middle;">I</td> <td style="vertical-align: middle;">R</td> <td style="font-style: italic;"><span style="font-style: italic;">building centered in x-direction</span></td>
181<td style="vertical-align: middle;">x-coordinate of the
182left building wall in m.</td> </tr> <tr> <td style="font-weight: bold; vertical-align: middle;"><a href="chapter_4.1.html#building_wall_south">building_wall_south</a></td>
183<td style="vertical-align: middle;">I</td> <td style="vertical-align: middle;">R</td> <td style="font-style: italic;"><span style="font-style: italic;">building centered in y-direction</span></td>
184<td style="vertical-align: middle;">y-coordinate of the
185South building wall&nbsp;in m.</td> </tr> <tr> <td style="vertical-align: middle;"><b><a href="chapter_4.2.html#call_psolver_at_all_substeps"><b>call_psolver_at_all_substeps</b></a></b></td>
186<td style="vertical-align: middle;">R<br> </td>
187<td style="vertical-align: middle;">L<br> </td>
188<td style="vertical-align: middle;"><span style="font-style: italic;">.T..</span><br> </td>
189<td style="vertical-align: middle;">Switch
190to steer the call of the pressure solver.</td> </tr> <tr>
191<td><b><a href="chapter_4.2.html#fcl_factor"><b>cfl_factor</b></a></b></td>
192<td>R</td> <td>R</td> <td><i>0.1,
1930.8&nbsp;or 0.9 </i>(see parameter description)</td> <td>Time
194step limiting factor.</td> </tr> <tr> <td style="vertical-align: top;"><a href="chapter_4.1.html#cloud_droplets"><span style="font-weight: bold;">cloud_droplets</span></a><br>
195</td> <td style="vertical-align: top;">I<br> </td>
196<td style="vertical-align: top;">L<br> </td> <td style="vertical-align: top;"><span style="font-style: italic;">.F.</span><br> </td>
197<td style="vertical-align: top;">Parameter to switch
198on usage of cloud droplets.</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#cloud_physics"><b>cloud_physics</b></a></p>
199</td> <td style="vertical-align: middle;" width="5%">
200<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>L</p>
201</td> <td style="vertical-align: middle;" width="16%">
202<p><i>.F.</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Parameter
203to switch on the condensation scheme. <br> </p> </td>
204</tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#comp_spectra_level"><b>comp_spectra_level</b></a></p>
205</td> <td style="vertical-align: middle;" width="5%">
206<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>I
207(10)</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>no level</i></p>
208</td> <td style="vertical-align: middle;" width="57%">
209<p>Vertical level for which horizontal spectra are to be
210calculated and output (gridpoints).</p> </td> </tr>
211<tr> <td><a href="chapter_4.1.html#conserve_volume_flow"><span style="font-weight: bold;">conserve_volume_flow</span></a></td>
212<td>I</td> <td>L</td> <td><span style="font-style: italic;">.F.</span></td> <td>Conservation
213of volume flow in x- and y-direction.</td> </tr> <tr>
214<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#create_disturbances"><b>create_disturbances</b></a></p>
215</td> <td style="vertical-align: middle;" width="5%">
216<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>L</p>
217</td> <td style="vertical-align: middle;" width="16%">
218<p><i>.T.</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Switch
219to impose random perturbations to the horizontal
220velocity field. <br> </p> </td> </tr> <tr>
221<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#cross_normalized_x"><b>cross_normalized_x</b></a></p>
222</td> <td style="vertical-align: middle;" width="5%">
223<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
224* 10 (100)</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>100
225* ' '</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Type
226of normalization applied to the x-coordinate of
[5]227vertical
228profiles to be plotted with <span style="font-weight: bold;">profil</span>.</p>
[61]229</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#cross_normalized_y"><b>cross_normalized_y</b></a></p>
230</td> <td style="vertical-align: middle;" width="5%">
231<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
232* 10&nbsp; <br>
233(100)</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>100 * ' '</i></p>
234</td> <td style="vertical-align: middle;" width="57%">
235<p>Type of normalization applied to the y-coordinate of
[5]236vertical
237profiles to be plotted with <span style="font-weight: bold;">profil</span>.
[61]238<br> </p> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#cross_profiles"><b>cross_profiles</b></a></p>
239</td> <td style="vertical-align: middle;" width="5%">
240<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
241* 100 (100)</p> </td> <td style="vertical-align: middle;" width="16%"> <p>see
242parameter description</p> </td> <td style="vertical-align: middle;" width="57%"> <p>Determines
243which vertical profiles are to be presented
[5]244in
245which coordinate system if the plot software <span style="font-weight: bold;">profil</span> is
[61]246used.&nbsp; <br> </p> </td> </tr> <tr>
247<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#cross_xtext"><b>cross_xtext</b></a></p>
248</td> <td style="vertical-align: middle;" width="5%">
249<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
250* 40&nbsp; <br>
251&nbsp;(100)</p> </td> <td style="vertical-align: middle;" width="16%"> <p>see
252parameter description</p> </td> <td style="vertical-align: middle;" width="57%"> <p>x-axis
253labels of vertical profile coordinate systems to
[5]254be
255plotted with <span style="font-weight: bold;">profil</span>.
[61]256<br> </p> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#cut_spline_overshoot"><b>cut_spline_overshoot</b></a></p>
257</td> <td style="vertical-align: middle;" width="5%">
258<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>L</p>
259</td> <td style="vertical-align: middle;" width="16%">
260<p><i>.T.</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Cut
261off of so-called overshoots, which can occur with
262the upstream-spline-scheme.</p> </td> </tr> <tr>
263<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#cycle_mg"><b>cycle_mg</b></a></p>
264</td> <td style="vertical-align: middle;" width="5%">
265<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
266* 1</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'w'</i></p> </td>
267<td style="vertical-align: middle;" width="57%">Type
[5]268of cycle to
269be used with the multi-grid
[61]270method.&nbsp;</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#damp_level_1d"><b>damp_level_1d</b></a></p>
271</td> <td style="vertical-align: middle;" width="5%">
272<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
273</td> <td style="vertical-align: middle;" width="16%">
274<p><i>zu(nz+1)</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Height
275where the damping layer begins in the 1d-model
276(in m). <br> </p> </td> </tr> <tr> <td><a href="chapter_4.2.html#data_output"><span style="font-weight: bold;">data_output</span></a></td>
277<td>R</td> <td>C * 10 (100)</td> <td><span style="font-style: italic;">100 * &acute; &acute;</span></td>
278<td>Quantities for which 2d cross section and/or 3d volume data
279are to be output.</td> </tr> <tr> <td><a href="chapter_4.2.html#data_output_format"><span style="font-weight: bold;">data_output_format</span></a></td>
280<td>R</td> <td>C * 10 (10)</td> <td><span style="font-style: italic;">'netcdf'</span></td>
281<td>Format of output data.</td> </tr> <tr> <td><a href="chapter_4.2.html#data_output_pr"><span style="font-weight: bold;">data_output_pr</span></a></td>
282<td>R</td> <td>C * 10 (100)</td> <td><span style="font-style: italic;">100 * ' '</span></td>
283<td>Quantities for which vertical profiles (horizontally
284averaged)
[89]285are to be output.</td> </tr> <tr><td><a href="chapter_4.3.html#data_output_pr_user"><span style="font-weight: bold;">data_output_pr_user</span></a></td><td>U</td><td>C * 10<br>(200)</td><td><span style="font-style: italic;">200 * ' '</span></td><td>User defined quantities for which horizontally averaged profile data is to be output.</td></tr><tr> <td><a href="chapter_4.2.html#data_output_sp"><span style="font-weight: bold;">data_output_sp</span></a></td>
[61]286<td>P</td> <td>C * 10 (10)</td> <td><span style="font-style: italic;">10 * ' '</span></td>
287<td>Quantities for which horizontal spectra are to be calculated
288and output.</td> </tr> <tr> <td><a href="chapter_4.3.html#data_output_user"><span style="font-weight: bold;">data_output_user</span></a></td>
289<td>U</td> <td>C * 10 (100)</td> <td><span style="font-style: italic;">100 * ' '</span></td>
290<td>User defined quantities for which 2d cross section and/or 3d
291volume data are to be output.</td> </tr> <tr> <td><a href="chapter_4.2.html#data_output_2d_on_each_pe"><span style="font-weight: bold;">data_output_2d_on_each_pe</span></a></td>
292<td>R</td> <td>L</td> <td><span style="font-style: italic;">.T.</span></td> <td>Output
2932d cross section data by one or
294all processors.&nbsp;</td> </tr> <tr valign="top">
295<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#density_ratio"><b>density_ratio</b></a></p>
296</td> <td style="vertical-align: middle;" width="5%">
297<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R
298(10)</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>0.0, 9</i> * <i>9999999.9</i></p>
299</td> <td style="vertical-align: middle;" width="57%">
300<p>Ratio of the density of the fluid and the density of the
301particles.</p> </td> </tr> <tr> <td><a href="chapter_4.1.html#dissipation_1d"><span style="font-weight: bold;">dissipation_1d</span></a></td>
302<td>I</td> <td>C * 20</td> <td><span style="font-style: italic;">'as_in_3d_model'</span></td>
303<td>Calculation method for the energy dissipation term in the TKE
304equation of the 1d-model.</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#disturbance_amplitude"><b>disturbance</b></a>&nbsp;&nbsp;&nbsp;
305<br> <a href="chapter_4.2.html#disturbance_amplitude">&nbsp;<b>_amplitude</b></a></p>
306</td> <td style="vertical-align: middle;" width="5%">
307<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
308</td> <td style="vertical-align: middle;" width="16%">
309<p><i>0.25</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Maximum
310perturbation amplitude of the random
[5]311perturbations
[61]312imposed to the horizontal velocity field (in m/s). <br> </p>
313</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#disturbance_energy_limit"><b>disturbance_energy</b></a>&nbsp;&nbsp;&nbsp;
314<br> <a href="chapter_4.2.html#disturbance_energy_limit">&nbsp;<b>_limit</b></a></p>
315</td> <td style="vertical-align: middle;" width="5%">
316<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
317</td> <td style="vertical-align: middle;" width="16%">
318<p><i>0.01</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p lang="en-GB">Upper limit value of the
[5]319perturbation energy of
320the velocity field used as a criterion for imposing random
321perturbations (in m<sup>2</sup>/s<sup>2</sup>).&nbsp;</p>
[61]322</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#disturbance_level_b"><b>disturbance_level_b</b></a></p>
323</td> <td style="vertical-align: middle;" width="5%">
324<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
325</td> <td style="vertical-align: middle;" width="16%">
[97]326<p><i>zu(3) or zu(nz*2/3)</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p lang="en-GB"><font face="Thorndale, serif"><font size="3">Lower
[5]327limit of the vertical range for which random perturbations are to be
328imposed on the horizontal wind field (</font></font>in <font face="Thorndale, serif"><font size="3">m).&nbsp;
[61]329</font></font> </p> <span lang="en-GB"></span></td>
330</tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#disturbance_level_t"><b>disturbance_level_t</b></a></p>
331</td> <td style="vertical-align: middle;" width="5%">
332<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
333</td> <td style="vertical-align: middle;" width="16%">
[97]334<p><i>zu(nz/3) or zu(nzt-3)</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p lang="en-GB"><font face="Thorndale, serif"><font size="3">Upper
[5]335limit of the vertical range for which random perturbations are to be
336imposed on the horizontal wind field (</font></font>in <font face="Thorndale, serif"><font size="3">m). <br>
[61]337</font></font></p> </td> </tr> <tr>
338<td><a href="chapter_4.2.html#do2d_at_begin"><span style="font-weight: bold;">do2d_at_begin</span></a></td>
339<td>R</td> <td>L</td> <td><span style="font-style: italic;">.F.</span></td> <td>Output
3402d cross section data by one or
341all processors.&nbsp;</td> </tr> <tr> <td><a href="chapter_4.2.html#do3d_at_begin"><span style="font-weight: bold;">do3d_at_begin</span></a></td>
342<td>R</td> <td>L</td> <td><span style="font-style: italic;">.F.</span></td> <td>Output
343of 3d volume data at the beginning
344of a run.</td> </tr> <tr> <td><a href="chapter_4.2.html#do3d_compress"><span style="font-weight: bold;">do3d_compress</span></a></td>
345<td>R</td> <td>L</td> <td><span style="font-style: italic;">.F.</span></td> <td>Output
346of data for 3d plots in compressed form.&nbsp;</td> </tr>
347<tr> <td><a href="chapter_4.2.html#do3d_precision"><span style="font-weight: bold;">do3d_precision</span></a></td>
348<td>R</td> <td>C * 7 (100)</td> <td>see
349parameter description</td> <td>Significant digits in case
350of compressed data output.&nbsp;</td> </tr> <tr>
351<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#dt"><b>dt</b></a></p>
352</td> <td style="vertical-align: middle;" width="5%">
353<p>I/R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
354</td> <td style="vertical-align: middle;" width="16%">
355<p><i>variable</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p><font face="Thorndale, serif"><font size="3">Time
[5]356step for the 3d-model (</font></font>in <font face="Thorndale, serif"><font size="3">s). <br>
[61]357</font></font></p> </td> </tr> <tr>
358<td><a href="chapter_4.2.html#dt_averaging_input"><span style="font-weight: bold;">dt_averaging_input</span></a></td>
359<td>R</td> <td>R</td> <td><span style="font-style: italic;">0.0</span></td> <td>Temporal
360interval of&nbsp;data which are subject to temporal averaging (in
361s).</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#dt_averaging_input_pr"><b>dt_averaging_input_pr</b></a></p>
362</td> <td style="vertical-align: middle;" width="5%">
363<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
364</td> <td style="vertical-align: middle;" width="16%"><span style="font-style: italic;">value of <a href="chapter_4.2.html#dt_averaging_input">dt_<br>
[5]365averaging_<br>
[61]366input</a></span></td> <td style="vertical-align: middle;" width="57%">Temporal
367interval of&nbsp;data which are subject to temporal averaging of <font face="Thorndale, serif"><font size="3">vertical
368profiles and/or spectra&nbsp;(</font></font>in <font face="Thorndale, serif"><font size="3">s).&nbsp;</font></font></td>
369</tr> <tr> <td><a href="chapter_4.2.html#dt_data_output"><span style="font-weight: bold;">dt_data_output</span></a></td>
370<td>R</td> <td>R</td> <td><span style="font-style: italic;">9999999.9</span></td>
371<td> <p lang="en-GB"><font face="Thorndale"><font face="Thorndale, serif">Temporal interval</font>
372at which&nbsp;data (3d volume data (instantaneous or time
373averaged),
[5]374cross sections (instantaneous or time averaged), vertical profiles,
375spectra) shall be output (</font>in <font face="Thorndale">s).&nbsp;</font></p>
[61]376</td> </tr> <tr> <td><a href="chapter_4.2.html#dt_data_output_av"><span style="font-weight: bold;">dt_data_output_av</span></a></td>
377<td>R</td> <td>R</td> <td><i>value
378of &nbsp;<a href="chapter_4.2.html#dt_data_output">dt_data_<br>
379output</a></i></td> <td> <p lang="en-GB"><font face="Thorndale"><font face="Thorndale, serif">Temporal
380interval</font>
[5]381at which time averaged 3d volume data and/or 2d cross section data
382shall be output (</font>in <font face="Thorndale">s).&nbsp;</font></p>
[61]383</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#dt_disturb"><b>dt_disturb</b></a></p>
384</td> <td style="vertical-align: middle;" width="5%">
385<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
386</td> <td style="vertical-align: middle;" width="16%">
387<p><i>9999999.9</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p lang="en-GB"><font face="Thorndale"><font face="Thorndale, serif">Temporal interval</font> at
[5]388which random
389perturbations are to be imposed on the horizontal velocity field
[61]390(</font>in <font face="Thorndale">s). <br> </font></p>
391</td> </tr> <tr> <td><a href="chapter_4.2.html#dt_dopr"><span style="font-weight: bold;">dt_dopr</span></a></td>
392<td>R</td> <td>R</td> <td><i>value
393of &nbsp;<a href="chapter_4.2.html#dt_data_output">dt_data_<br>
394output</a></i></td> <td><span lang="en-GB"><font face="Thorndale">Temporal interval at
[5]395which data&nbsp;of vertical profiles shall be output (to local
[61]396file <a href="chapter_3.4.html#DATA_1D_PR_NETCDF">DATA_1D_PR_NETCDF</a>
397or/and </font></span><a href="chapter_3.4.html#PLOT1D_DATA"><span lang="en-GB"><font face="Thorndale">PLOT1D_DATA</font></span></a><span lang="en-GB"><font face="Thorndale">) (</font></span>in
398<span lang="en-GB"><font face="Thorndale">s).&nbsp;</font></span></td>
399</tr> <tr> <td><a href="chapter_4.2.html#dt_dopr_listing"><span style="font-weight: bold;">dt_dopr_listing</span></a></td>
400<td>R</td> <td>R</td> <td><span style="font-style: italic;">9999999.9</span></td>
401<td> <p><span lang="en-GB"><font face="Thorndale, serif">Temporal
402interval</font> at which data <font face="Thorndale">of
403vertical
404profiles shall be output (output for printouts, local file </font></span><a href="chapter_3.4.html#LIST_PROFIL"><span lang="en-GB"><font face="Thorndale">LIST_PROFIL</font></span></a><span lang="en-GB"><font face="Thorndale">) (</font></span>in
405<span lang="en-GB"><font face="Thorndale">s).&nbsp;</font></span>
406</p> </td> </tr> <tr> <td align="undefined" valign="undefined"><a href="chapter_4.2.html#dt_dopts"><span style="font-weight: bold;">dt_dopts</span></a></td>
407<td align="undefined" valign="undefined">P</td>
408<td align="undefined" valign="undefined">R</td>
409<td align="undefined" valign="undefined"><i>value
410of &nbsp;<a href="chapter_4.2.html#dt_data_output">dt_data_<br>
411output</a></i></td> <td align="undefined" valign="undefined"> <p lang="en-GB"><font face="Thorndale"><font face="Thorndale, serif">Temporal
412interval</font> at which time series data of particle quantities
413shall be output (</font>in <font face="Thorndale">s).&nbsp;</font></p>
414</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#dt_dosp"><b>dt_dosp</b></a></p>
415</td> <td style="vertical-align: middle;" width="5%">
416<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
417</td> <td style="vertical-align: middle;" width="16%"><i>value
418of &nbsp;<a href="chapter_4.2.html#dt_data_output">dt_data_<br>
419output</a></i></td> <td style="vertical-align: middle;" width="57%">Temporal
420interval at which&nbsp;spectra data shall be output
421(in s).&nbsp;</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#dt_dots"><b>dt_dots</b></a></p>
422</td> <td style="vertical-align: middle;" width="5%">
423<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
424</td> <td style="vertical-align: middle;" width="16%">
425<p>see parameter description</p> </td> <td style="vertical-align: middle;" width="57%"> <p lang="en-GB"><font face="Thorndale"><font face="Thorndale, serif">Temporal interval</font> at
426which&nbsp;time series data shall be output (</font>in <font face="Thorndale">s). <br> </font></p> </td>
427</tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#dt_do2d_xy"><b>dt_do2d_xy</b></a></p>
428</td> <td style="vertical-align: middle;" width="5%">
429<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
430</td> <td style="vertical-align: middle;" width="16%"><i>value
431of &nbsp;<a href="chapter_4.2.html#dt_data_output">dt_data_<br>
432output</a></i></td> <td style="vertical-align: middle;" width="57%"> <p lang="en-GB"><font face="Thorndale"><font face="Thorndale, serif">Temporal interval</font> at
433which horizontal cross section data shall be output (</font>in <font face="Thorndale">s). <br> </font></p> </td>
434</tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#dt_do2d_xz"><b>dt_do2d_xz</b></a></p>
435</td> <td style="vertical-align: middle;" width="5%">
436<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
437</td> <td style="vertical-align: middle;" width="16%"><i>value
438of &nbsp;<a href="chapter_4.2.html#dt_data_output">dt_data_<br>
439output</a></i></td> <td style="vertical-align: middle;" width="57%"> <p lang="en-GB"><font face="Thorndale"><font face="Thorndale, serif">Temporal interval</font> at
440which vertical cross section data (xz) shall be output&nbsp;(</font>in
441<font face="Thorndale">s). <br> </font></p>
442</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#dt_do2d_yz"><b>dt_do2d_yz</b></a></p>
443</td> <td style="vertical-align: middle;" width="5%">
444<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
445</td> <td style="vertical-align: middle;" width="16%"><i>value
446of &nbsp;<a href="chapter_4.2.html#dt_data_output">dt_data_<br>
447output</a></i></td> <td style="vertical-align: middle;" width="57%"> <p lang="en-GB"><font face="Thorndale"><font face="Thorndale, serif">Temporal interval</font> at
448which vertical cross section data (yz)&nbsp;shall be
449output&nbsp;(</font>in s<font face="Thorndale">).</font></p>
450</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#dt_do3d"><b>dt_do3d</b></a></p>
451</td> <td style="vertical-align: middle;" width="5%">
452<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
453</td> <td style="vertical-align: middle;" width="16%"><i>value
454of &nbsp;<a href="chapter_4.2.html#dt_data_output">dt_data_<br>
455output</a></i></td> <td style="vertical-align: middle;" width="57%"> <p lang="en-GB"><font face="Thorndale"><font face="Thorndale, serif">Temporal interval</font> at
456which 3d volume data shall be output (</font>in <font face="Thorndale">s). <br> </font></p> </td>
457</tr> <tr> <td><b><a href="chapter_4.2.html#dt_dvrp"><b>dt_dvrp</b></a></b></td>
458<td>P</td> <td>R</td> <td><span style="font-style: italic;">9999999.9</span></td>
459<td>Temporal interval of scenes to be displayed with the <span style="font-weight: bold;">dvrp</span> software (in
460s). </td> </tr> <tr><td><a style="font-weight: bold;" href="chapter_4.2.html#dt_max">dt_max</a></td><td>R</td><td>R</td><td><span style="font-style: italic;">20.0</span></td><td>Maximum
461allowed value of the timestep (in s).</td></tr><tr> <td align="undefined" valign="undefined"><a href="chapter_4.2.html#dt_min_part"><span style="font-weight: bold;">dt_min_part</span></a></td>
462<td align="undefined" valign="undefined">P</td>
463<td align="undefined" valign="undefined">R</td>
464<td align="undefined" valign="undefined"><span style="font-style: italic;">0.0002</span></td> <td align="undefined" valign="undefined">Minimum value
465for the particle timestep when SGS velocities are used (in s).</td>
466</tr> <tr valign="top"> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#dt_prel"><b>dt_prel</b></a></p>
467</td> <td style="vertical-align: middle;" width="5%">
468<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
469</td> <td style="vertical-align: middle;" width="16%">
470<p><i>9999999.9</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p><font face="Thorndale, serif"><span lang="en-GB">Temporal
[5]471interval at
472which particles are to be released <span lang="en-GB">from
473a particle
474source </span>(</span></font>in <font face="Thorndale, serif"><span lang="en-GB">s).</span>&nbsp;</font></p>
[61]475</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#dt_pr_1d"><b>dt_pr_1d</b></a></p>
476</td> <td style="vertical-align: middle;" width="5%">
477<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
478</td> <td style="vertical-align: middle;" width="16%">
479<p><i>9999999.9</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Temporal
480interval of vertical profile output of the
[5]4811D-model
[61]482(in s).&nbsp;</p> </td> </tr> <tr> <td style="vertical-align: middle;"><b><a href="chapter_4.2.html#dt_restart"><b>dt_restart</b></a></b></td>
483<td style="vertical-align: middle;">R<br> </td>
484<td style="vertical-align: middle;">R<br> </td>
485<td style="vertical-align: middle;">9999999.9<br> </td>
486<td style="vertical-align: middle;"><font face="Thorndale"><font face="Thorndale, serif">Temporal
[5]487interval</font> at which a new
[61]488restart run is to be carried out (</font>in <font face="Thorndale">s).</font></td> </tr> <tr>
489<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#dt_run_control"><b>dt_run_control</b></a></p>
490</td> <td style="vertical-align: middle;" width="5%">
491<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
492</td> <td style="vertical-align: middle;" width="16%">
493<p><i>60.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p lang="en-GB"><font face="Thorndale"><font face="Thorndale, serif">Temporal interval</font> at
[5]494which run control
495output is to be made (</font>in <font face="Thorndale">s).
[61]496<br> </font></p> </td> </tr> <tr>
497<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#dt_run_control_1d"><b>dt_run_control_1d</b></a></p>
498</td> <td style="vertical-align: middle;" width="5%">
499<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
500</td> <td style="vertical-align: middle;" width="16%">
501<p><i>60.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Temporal
502interval of runtime control output of the
[5]5031d-model
[61]504(in s).</p> </td> </tr> <tr> <td style="vertical-align: middle;"><b><a href="chapter_4.2.html#dt_write_particle_data"><b>dt_write_particle_data</b></a></b></td>
505<td style="vertical-align: middle;">P<br> </td>
506<td style="vertical-align: middle;">R<br> </td>
507<td style="vertical-align: middle;"><i>9999999.9</i></td>
508<td style="vertical-align: middle;">Temporal
[5]509interval for output
[61]510of particle data (in s).</td> </tr> <tr valign="top">
511<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#dvrp_directory"><b>dvrp_directory</b></a></p>
512</td> <td style="vertical-align: middle;" width="5%">
513<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
514* 80</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'default'</i></p>
515</td> <td style="vertical-align: middle;" width="57%">
516<p>Name of the directory into which data created by the <span style="font-weight: bold;">dvrp</span>
517software shall be saved. <br> </p> </td> </tr>
518<tr valign="top"> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#dvrp_file"><b>dvrp_file</b></a></p>
519</td> <td style="vertical-align: middle;" width="5%">
520<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
521* 80</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'default'</i></p>
522</td> <td style="vertical-align: middle;" width="57%">
523<p>Name of the file into which data created by the <span style="font-weight: bold;">dvrp</span> software shall
524be output.</p> </td> </tr> <tr valign="top">
525<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#dvrp_host"><b>dvrp_host</b></a></p>
526</td> <td style="vertical-align: middle;" width="5%">
527<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
528* 80</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'origin.rvs. <br>
529uni- hanover.de'</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Name
530of the computer to which data created by the <span style="font-weight: bold;">dvrp</span> software shall
[5]531be
[61]532transferred. <br> </p> </td> </tr> <tr valign="top"> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#dvrp_output"><b>dvrp_output</b></a></p>
533</td> <td style="vertical-align: middle;" width="5%">
534<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
535* 10</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'rtsp'</i></p> </td>
536<td style="vertical-align: middle;" width="57%"> <p>Output
537mode for the <span style="font-weight: bold;">dvrp</span>
538software. </p> </td> </tr> <tr valign="top">
539<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#dvrp_password"><b>dvrp_password</b></a></p>
540</td> <td style="vertical-align: middle;" width="5%">
541<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
542* 80</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'********'</i></p>
543</td> <td style="vertical-align: middle;" width="57%">Password
[5]544for the
545computer to which data created
546by the <span style="font-weight: bold;">dvrp</span>
547software is to be
[61]548transferred.</td> </tr> <tr valign="top"> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#dvrp_psize"><b>dvrp_psize</b></a></p>
549</td> <td style="vertical-align: middle;" width="5%">
550<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
551</td> <td style="vertical-align: middle;" width="16%">
552<p><i>0.2</i> * <i>dx</i></p> </td>
553<td style="vertical-align: middle;" width="57%"> <p>Diameter
554that the particles is given in visualizations
[5]555with
556the <span style="font-weight: bold;">dvrp</span>
557software (in
[61]558m). <br> </p> </td> </tr> <tr valign="top"> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#dvrp_username"><b>dvrp_username</b></a></p>
559</td> <td style="vertical-align: middle;" width="5%">
560<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
561* 80</p> </td> <td style="vertical-align: middle;" width="16%"> <p>no default value </p> </td>
562<td style="vertical-align: middle;" width="57%"> <p>User
563name of a valid account on the computer to which
[5]564data
565created by the <span style="font-weight: bold;">dvrp</span>
566software
567is to be
[61]568transferred. <br> </p> </td> </tr> <tr>
569<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#dx"><b>dx</b></a></p>
570</td> <td style="vertical-align: middle;" width="5%">
571<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
572</td> <td style="vertical-align: middle;" width="16%">
573<p><i>1.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Horizontal
574grid spacing along the x-direction (in m). <br> </p> </td>
575</tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#dy"><b>dy</b></a></p>
576</td> <td style="vertical-align: middle;" width="5%">
577<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
578</td> <td style="vertical-align: middle;" width="16%">
579<p><i>1.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Horizontal
[83]580grid spacing along the y-direction (in m). <br> </p> </td>
[61]581</tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#dz"><b>dz</b></a></p>
582</td> <td style="vertical-align: middle;" width="5%">
583<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
584</td> <td style="vertical-align: middle;" width="16%">
585<p>no default, see parameter description </p> </td>
586<td style="vertical-align: middle;" width="57%"> <p>Vertical
587grid spacing (in m).</p> </td> </tr> <tr> <td align="undefined" valign="undefined"><a style="font-weight: bold;" href="chapter_4.1.html#dz_max">dz_max</a></td>
588<td align="undefined" valign="undefined">I</td>
589<td align="undefined" valign="undefined">R</td>
590<td align="undefined" valign="undefined"><span style="font-style: italic;">9999999.9</span></td>
591<td align="undefined" valign="undefined">Allowed
592maximum vertical grid spacing (in m).<br> </td> </tr>
593<tr> <td style="vertical-align: middle;" width="15%">
594<p><a href="chapter_4.1.html#dz_stretch_factor"><b>dz_stretch_factor</b></a></p>
595</td> <td style="vertical-align: middle;" width="5%">
596<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
597</td> <td style="vertical-align: middle;" width="16%">
598<p><i>1.08</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Stretch
599factor for a vertically stretched grid (see <a href="chapter_4.1.html#dz_stretch_level">dz_stretch_level</a>).</p>
600</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#dz_stretch_level"><b>dz_stretch_level</b></a></p>
601</td> <td style="vertical-align: middle;" width="5%">
602<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
603</td> <td style="vertical-align: middle;" width="16%">
604<p><i>100000.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Height
605level above which the grid is to be stretched
606vertically (in m). <br> </p> </td> </tr> <tr>
607<td><a href="chapter_4.1.html#e_min"><b>e_min</b></a></td>
608<td>I</td> <td>R</td> <td>0.0</td>
609<td>Minimum TKE in m<sup>2</sup>s<sup>-2</sup>.</td>
610</tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#end_time"><b>end_time</b></a></p>
611</td> <td style="vertical-align: middle;" width="5%">
612<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
613</td> <td style="vertical-align: middle;" width="16%">
614<p><i>0.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p lang="en-GB"><font face="Thorndale">Simulation
[5]615time of the 3D
[61]616model (</font>in <font face="Thorndale">s)</font><font face="Thorndale">.</font></p> </td> </tr>
617<tr> <td align="undefined" valign="undefined"><a href="chapter_4.2.html#end_time_prel"><span style="font-weight: bold;">end_time_prel</span></a></td>
618<td align="undefined" valign="undefined">P</td>
619<td align="undefined" valign="undefined">R</td>
620<td align="undefined" valign="undefined"><span style="font-style: italic;">9999999.9</span></td>
621<td align="undefined" valign="undefined">Time of
622the last release of particles (in s).</td> </tr> <tr>
623<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#end_time_1d"><b>end_time_1d</b></a></p>
624</td> <td style="vertical-align: middle;" width="5%">
625<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
626</td> <td style="vertical-align: middle;" width="16%">
627<p><i>864000.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Time
628to be simulated for the 1D-model (in s).&nbsp;</p> </td>
629</tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#fft_method"><b>fft_method</b></a></p>
630</td> <td style="vertical-align: middle;" width="5%">
631<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
632* 20</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'system specific'</i></p>
633</td> <td style="vertical-align: middle;" width="57%">
634<p>FFT-method to be used.</p> </td> </tr> <tr>
635<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#force_print_header"><b>force_print_header</b></a></p>
636</td> <td style="vertical-align: middle;" width="5%">
637<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>L</p>
638</td> <td style="vertical-align: middle;" width="16%">
639<p><i>.F.</i></p> </td> <td style="width: 57%; vertical-align: middle;"> <p>Steering
640of header output to the local file <a href="chapter_3.4.html#RUN_CONTROL">RUN_CONTROL</a>. </p>
641</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#galilei_transformation"><b>galilei_transformation</b></a></p>
642</td> <td style="vertical-align: middle;" width="5%">
643<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>L</p>
644</td> <td style="vertical-align: middle;" width="16%">
645<p><i>.F.</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Application
646of a Galilei-transformation to the
[5]647coordinate
[61]648system of the model.</p> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#grid_matching"><b>grid_matching</b></a></p>
649</td> <td style="vertical-align: middle;" width="5%">
650<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
651* 6</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'match'</i></p> </td>
652<td style="vertical-align: middle;" width="57%"> <p>Variable
653to adjust the subdomain sizes in parallel runs.</p> </td> </tr>
[75]654<tr><td><b><a href="chapter_4.1.html#humidity"><b>humidity</b></a></b></td><td>I</td><td>L</td><td><span style="font-style: italic;">.F.</span></td><td>Parameter
655to switch on the prognostic equation for
656specific
657humidity q.</td></tr><tr> <td style="vertical-align: middle;"><b><a href="chapter_4.1.html#inflow_disturbance_begin"><b>inflow_disturbance_begin</b></a></b></td>
[61]658<td style="vertical-align: middle;">I<br> </td>
659<td style="vertical-align: middle;">I<br> </td>
660<td style="vertical-align: middle;"><span style="font-style: italic;">MIN(10,</span><br style="font-style: italic;"> <span style="font-style: italic;">nx/2 or ny/2)</span></td>
661<td style="vertical-align: middle;">Lower
[5]662limit of the horizontal range for which random perturbations are to be
[61]663imposed on the horizontal velocity field (gridpoints).</td> </tr>
664<tr> <td style="vertical-align: middle;"><b><b><a href="chapter_4.1.html#inflow_disturbance_end"><b>inflow_disturbance_end</b></a></b></b></td>
665<td style="vertical-align: middle;">I<br> </td>
666<td style="vertical-align: middle;">I<br> </td>
667<td style="vertical-align: middle;"><span style="font-style: italic;">MIN(100,</span><br style="font-style: italic;"> <span style="font-style: italic;">3/4*nx or</span><br style="font-style: italic;"> <span style="font-style: italic;">3/4*ny)</span></td> <td style="vertical-align: middle;">Upper
[5]668limit of the horizontal range for which random perturbations are
669to be imposed on the horizontal velocity field (gridpoints).</td>
[61]670</tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#initializing_actions"><b>initializing_actions</b></a></p>
671</td> <td style="vertical-align: middle;" width="5%">
672<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
673* 100</p> </td> <td style="vertical-align: middle;" width="16%"> <p>no default, see parameter description</p>
674</td> <td style="vertical-align: middle;" width="57%">
675<p style="font-style: normal;">Initialization
[5]676actions
[61]677to be carried out. <br> </p> </td> </tr> <tr>
678<td style="vertical-align: top;"><a href="chapter_4.2.html#initial_weighting_factor"><span style="font-weight: bold;">initial_weighting_factor</span></a><br>
679</td> <td style="vertical-align: top;">P<br> </td>
680<td style="vertical-align: top;">R<br> </td> <td style="vertical-align: top;"><span style="font-style: italic;">1.0</span><br> </td>
681<td style="vertical-align: top;">Factor to define
682the real number of initial droplets in a grid cell.</td> </tr>
683<tr> <td style="vertical-align: middle;" width="15%">
684<p><a href="chapter_4.1.html#km_constant"><b>km_constant</b></a></p>
685</td> <td style="vertical-align: middle;" width="5%">
686<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
687</td> <td style="vertical-align: middle;" width="16%">
688<p><i>variable (computed from TKE)</i></p> </td>
689<td style="vertical-align: middle;" width="57%"> <p>Constant
690eddy diffusivities are used (laminar
691simulations).&nbsp;</p> </td> </tr> <tr>
692<td style="vertical-align: middle;"><b><a href="chapter_4.1.html#km_damp_max"><b>km_damp_max</b></a></b></td>
693<td style="vertical-align: middle;">I<br> </td>
694<td style="vertical-align: middle;">R<br> </td>
695<td style="vertical-align: middle;"><span style="font-style: italic;">0.5*(dx
696or dy)</span></td> <td style="vertical-align: middle;">Maximum
[5]697diffusivity used for filtering the velocity field in the vicinity of
[61]698the outflow (in m<sup>2</sup>/s).</td> </tr> <tr>
699<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#long_filter_factor"><b>long_filter_factor</b></a></p>
700</td> <td style="vertical-align: middle;" width="5%">
701<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
702</td> <td style="vertical-align: middle;" width="16%">
703<p><i>0.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Filter
704factor for the so-called Long-filter.</p> </td> </tr>
[62]705<tr><td><a style="font-weight: bold;" href="chapter_4.1.html#loop_optimization">loop_optimization</a></td><td>I</td><td>C * 16</td><td>see parameter description</td><td>Method used to optimize loops for solving the prognostic equations .</td></tr><tr> <td style="vertical-align: middle;" width="15%">
[61]706<p><a href="chapter_4.2.html#maximum_number_of_particles"><b>maximum_number_</b></a>
707<br> <a href="chapter_4.2.html#maximum_number_of_particles"><b>of_particles</b></a></p>
708</td> <td style="vertical-align: middle;" width="5%">
709<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>I</p>
710</td> <td style="vertical-align: middle;" width="16%">
711<p><i>1000</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Maximum
712number of particles (on a PE). <br> </p> </td> </tr>
713<tr> <td style="vertical-align: middle;" width="15%">
714<p><a href="chapter_4.2.html#maximum_number_of_tailpoints"><b>maximum_number_</b></a>
715<br> <a href="chapter_4.2.html#maximum_number_of_tailpoints"><b>of_tailpoints</b></a></p>
716</td> <td style="vertical-align: middle;" width="5%">
717<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>I</p>
718</td> <td style="vertical-align: middle;" width="16%">
719<p><i>100</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Maximum
720number of tailpoints that a particle tail can
721have. <br> </p> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#maximum_tailpoint_age"><b>maximum_tailpoint_</b></a>
722<br> <a href="chapter_4.2.html#maximum_tailpoint_age"><b>age</b></a></p>
723</td> <td style="vertical-align: middle;" width="5%">
724<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
725</td> <td style="vertical-align: middle;" width="16%">
726<p><i>100000.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Maximum
727age that the end point of a particle tail is allowed to have (in s). <br>
728</p> </td> </tr> <tr> <td><b><a href="chapter_4.2.html#mg_cycles"><b>mg_cycles</b></a></b></td>
729<td>R</td> <td>I</td> <td><i>- 1</i></td>
730<td>Number of cycles to be used with the multi-grid scheme.</td>
731</tr> <tr> <td><b><b><a href="chapter_4.2.html#mg_switch_to_pe0_level"><b>mg_switch_to_pe0_level</b></a></b></b></td>
732<td>R</td> <td>I</td> <td>see parameter
733description</td> <td>Grid
734level at which data shall be gathered on PE0.</td> </tr> <tr>
735<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#minimum_tailpoint_distance"><b>minimum_tailpoint_</b></a>
736<br> <a href="chapter_4.2.html#minimum_tailpoint_distance"><b>distance</b></a></p>
737</td> <td style="vertical-align: middle;" width="5%">
738<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
739</td> <td style="vertical-align: middle;" width="16%">
740<p><i>0.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Minimum
741distance allowed between two adjacent points of
[5]742a
[61]743particle tail (in m). <br> </p> </td> </tr>
744<tr> <td><a href="chapter_4.1.html#mixing_length_1d"><span style="font-weight: bold;">mixing_length_1d</span></a></td>
745<td>I</td> <td>C * 20</td> <td><span style="font-style: italic;">'as_in_3d_model'</span></td>
746<td>Mixing length used in the 1d-model.</td> </tr> <tr valign="top"> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#mode_dvrp"><b>mode_dvrp</b></a></p>
747</td> <td style="vertical-align: middle;" width="5%">
748<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
749* 20 (10)</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>10 * ' '</i></p>
750</td> <td style="vertical-align: middle;" width="57%">
751<p>Graphical objects (isosurfaces, slicers, particles)
[5]752which are
753to be created by the <span style="font-weight: bold;">dvrp</span>
[75]754software. <br> </p> </td> </tr>  <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#momentum_advec"><b>momentum_advec</b></a></p>
[61]755</td> <td style="vertical-align: middle;" width="5%">
756<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
757* 10</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'pw-scheme</i>'</p>
758</td> <td style="vertical-align: middle;" width="57%">
759<p>Advection scheme to be used for the momentum equations.</p>
760</td> </tr> <tr> <td><a href="chapter_4.1.html#netcdf_precision"><span style="font-weight: bold;">netcdf_precision</span></a></td>
761<td>I</td> <td>C * 20 (10)</td> <td><span style="font-style: italic;">single preci</span><span style="font-style: italic;">sion for all</span><br style="font-style: italic;"> <span style="font-style: italic;">output quan</span><span style="font-style: italic;">tities</span></td> <td>Defines
762the accuracy of the NetCDF output.<br> </td> </tr> <tr>
763<td><a href="chapter_4.2.html#netcdf_64bit"><span style="font-weight: bold;">netcdf_64bit</span></a></td>
764<td>R</td> <td>L</td> <td><span style="font-style: italic;">.F.</span></td> <td>NetCDF
765files will have 64 bit offset format.</td> </tr> <tr><td><a style="font-weight: bold;" href="chapter_4.2.html#netcdf_64bit_3d">netcdf_64bit_3d</a></td><td>R</td><td>L</td><td><span style="font-style: italic;">.T.</span></td><td>NetCDF
766files containing 3d volume data will have 64 bit offset format.</td></tr><tr valign="top"> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#ngsrb"><b>ngsrb</b></a></p>
767</td> <td style="vertical-align: middle;" width="5%">
768<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>I</p>
769</td> <td style="vertical-align: middle;" width="16%">
770<p><i>2</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Grid
771level at which data shall be gathered on PE0.</p> </td> </tr>
772<tr> <td style="vertical-align: middle;" width="15%">
773<p><a href="chapter_4.2.html#normalizing_region"><b>normalizing_region</b></a></p>
774</td> <td style="vertical-align: middle;" width="5%">
775<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>I</p>
776</td> <td style="vertical-align: middle;" width="16%">
777<p><i>0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Determines
778the subdomain from which the normalization
779quantities are calculated. <br> </p> </td> </tr>
780<tr> <td style="vertical-align: middle;" width="15%">
781<p><a href="chapter_4.1.html#npex"><b>npex</b></a></p>
782</td> <td style="vertical-align: middle;" width="5%">
783<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>I</p>
784</td> <td style="vertical-align: middle;" width="16%">
785<p>no default, see parameter description</p> </td> <td style="vertical-align: middle;" width="57%"> <p>Number
786of processors along x-direction of the virtual
[5]787processor
[61]788net. <br> </p> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#npey"><b>npey</b></a></p>
789</td> <td style="vertical-align: middle;" width="5%">
790<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>I</p>
791</td> <td style="vertical-align: middle;" width="16%">
792<p>no default, see parameter description</p> </td> <td style="vertical-align: middle;" width="57%"> <p>Number
793of processors along y-direction of the virtual
[5]794processor
[61]795net. <br> </p> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#nsor"><b>nsor</b></a></p>
796</td> <td style="vertical-align: middle;" width="5%">
797<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>I</p>
798</td> <td style="vertical-align: middle;" width="16%">
799<p><i>20</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Number
800of iterations to be used with the SOR-scheme. <br> </p> </td>
801</tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#nsor_ini"><b>nsor_ini</b></a></p>
802</td> <td style="vertical-align: middle;" width="5%">
803<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>I</p>
804</td> <td style="vertical-align: middle;" width="16%">
805<p><i>100</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Initial
806number of iterations with the SOR algorithm</p> </td> </tr>
807<tr> <td><a href="chapter_4.2.html#number_of_particle_groups"><span style="font-weight: bold;">number_of_particle_groups</span></a></td>
808<td>P</td> <td>I</td> <td><span style="font-style: italic;">1</span></td> <td>Number
809of particle groups to be used.</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#nx"><b>nx</b></a></p>
810</td> <td style="vertical-align: middle;" width="5%">
811<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>I</p>
812</td> <td style="vertical-align: middle;" width="16%">
813<p>no default, see parameter description</p> </td> <td style="vertical-align: middle;" width="57%"> <p>Number
814of grid points in x-direction. <br> </p> </td> </tr>
815<tr> <td style="vertical-align: middle;" width="15%">
816<p><a href="chapter_4.1.html#ny"><b>ny</b></a></p>
817</td> <td style="vertical-align: middle;" width="5%">
818<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>I</p>
819</td> <td style="vertical-align: middle;" width="16%">
820<p>no default, see parameter description</p> </td> <td style="vertical-align: middle;" width="57%"> <p>Number
821of grid points in y-direction.</p> </td> </tr> <tr>
822<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#nz"><b>nz</b></a></p>
823</td> <td style="vertical-align: middle;" width="5%">
824<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>I</p>
825</td> <td style="vertical-align: middle;" width="16%">
826<p>no default, see parameter description</p> </td> <td style="vertical-align: middle;" width="57%"> <p>Number
827of grid points in z-direction.</p> </td> </tr> <tr>
828<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#nz_do3d"><b>nz_do3d</b></a></p>
829</td> <td style="vertical-align: middle;" width="5%">
830<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>I</p>
831</td> <td style="vertical-align: middle;" width="16%">
832<p><i>nz+1</i></p> </td> <td style="vertical-align: middle;" width="57%"> Limits
833the output of 3d volume data along the vertical direction (grid point
[97]834index k).</td> </tr> <tr><td align="undefined" valign="undefined"><a href="chapter_4.1.html#ocean"><span style="font-weight: bold;">ocean</span></a></td><td align="undefined" valign="undefined">I</td><td align="undefined" valign="undefined">L</td><td align="undefined" valign="undefined"><span style="font-style: italic;">.F.</span></td><td align="undefined" valign="undefined">Parameter to switch on&nbsp;ocean runs.</td></tr><tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#omega"><b>omega</b></a></p>
[61]835</td> <td style="vertical-align: middle;" width="5%">
836<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
837</td> <td style="vertical-align: middle;" width="16%">
838<p><i>7.29212E-5</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Angular
839velocity of the rotating system (in rad s<sup>-1</sup>).&nbsp;</p>
840</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#omega_sor"><b>omega_sor</b></a></p>
841</td> <td style="vertical-align: middle;" width="5%">
842<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
843</td> <td style="vertical-align: middle;" width="16%">
844<p><i>1.8</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Convergence
845factor to be used with the the SOR-scheme. <br> </p> </td>
846</tr> <tr> <td style="vertical-align: middle;"><b><a href="chapter_4.2.html#outflow_damping_width"><b>outflow_damping_width</b></a></b></td>
847<td style="vertical-align: middle;">I<br> </td>
848<td style="vertical-align: middle;">I<br> </td>
849<td style="vertical-align: middle;"><span style="font-style: italic;">MIN(20,
[5]850nx/2</span> or <span style="font-style: italic;">ny/2)</span></td>
[61]851<td style="vertical-align: middle;">Width of
[5]852the damping range in the vicinity of the outflow (gridpoints).</td>
[61]853</tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#overshoot_limit_e"><b>overshoot_limit_e</b></a></p>
854</td> <td style="vertical-align: middle;" width="5%">
855<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
856</td> <td style="vertical-align: middle;" width="16%">
857<p><i>0.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Allowed
858limit for the overshooting of subgrid-scale TKE
[5]859in
860case that the upstream-spline scheme is switched on (in m<sup>2</sup>/s<sup>2</sup>).</p>
[61]861</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#overshoot_limit_pt"><b>overshoot_limit_pt</b></a></p>
862</td> <td style="vertical-align: middle;" width="5%">
863<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
864</td> <td style="vertical-align: middle;" width="16%">
865<p><i>0.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Allowed
866limit for the overshooting of potential
[5]867temperature in
868case that the upstream-spline scheme is switched on (in K). <br>
[61]869</p> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#overshoot_limit_u"><b>overshoot_limit_u</b></a></p>
870</td> <td style="vertical-align: middle;" width="5%">
871<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
872</td> <td style="vertical-align: middle;" width="16%">
873<p><i>0.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Allowed
874limit for the
[5]875overshooting of
876the u-component of velocity in case that the upstream-spline scheme is
[61]877switched on (in m/s).</p> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#overshoot_limit_v"><b>overshoot_limit_v</b></a></p>
878</td> <td style="vertical-align: middle;" width="5%">
879<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
880</td> <td style="vertical-align: middle;" width="16%">
881<p><i>0.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Allowed
882limit for the overshooting of the v-component of
[5]883velocity in case that the upstream-spline scheme is switched on
[61]884(in m/s). <br> </p> </td> </tr> <tr>
885<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#overshoot_limit_w"><b>overshoot_limit_w</b></a></p>
886</td> <td style="vertical-align: middle;" width="5%">
887<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
888</td> <td style="vertical-align: middle;" width="16%">
889<p><i>0.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Allowed
890limit for the overshooting of the w-component of
[5]891velocity in case that the upstream-spline scheme is switched on
[61]892(in m/s). <br> </p> </td> </tr> <tr>
893<td align="undefined" valign="undefined"><a href="chapter_4.2.html#particles_per_point"><span style="font-weight: bold;">particles_per_point</span></a></td>
894<td align="undefined" valign="undefined">P</td>
895<td align="undefined" valign="undefined">I</td>
896<td align="undefined" valign="undefined"><span style="font-style: italic;">1</span></td> <td align="undefined" valign="undefined">Number of
897particles to be started per point.</td> </tr> <tr> <td style="vertical-align: top;"><b><a href="chapter_4.2.html#particle_advection_start"><b>particle_advection_start</b></a></b></td>
898<td style="vertical-align: top;">P<br> </td> <td style="vertical-align: top;">R<br> </td> <td style="vertical-align: top;"><span style="font-style: italic;">0.0</span><br> </td>
899<td style="vertical-align: top;">Time of the first
[5]900release of
[61]901particles (in s).</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#particle_maximum_age"><b>particle_maximum_age</b></a></p>
902</td> <td style="vertical-align: middle;" width="5%">
903<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
904</td> <td style="vertical-align: middle;" width="16%">
905<p><i>9999999.9</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Maximum
906allowed age of particles (in s). <br> </p> </td> </tr>
907<tr> <td style="vertical-align: middle;" width="15%">
908<p><a href="chapter_4.1.html#passive_scalar"><b>passive_scalar</b></a></p>
909</td> <td style="vertical-align: middle;" width="5%">
910<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>L</p>
911</td> <td style="vertical-align: middle;" width="16%">
912<p><i>.F.</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Parameter
913to switch on the prognostic equation for a
[5]914passive
[61]915scalar. </p> </td> </tr> <tr valign="top">
916<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#pdx"><b>pdx</b></a></p>
917</td> <td style="vertical-align: middle;" width="5%">
918<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R
919(10)</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>10 * dx</i></p> </td>
920<td style="vertical-align: middle;" width="57%"> <p>Distance
921along x between particles within a particle
[5]922source
[61]923(in m). <br> </p> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#pdy"><b>pdy</b></a></p>
924</td> <td style="vertical-align: middle;" width="5%">
925<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R
926(10)</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>10 * dy</i></p> </td>
927<td style="vertical-align: middle;" width="57%"> <p>Distance
928along y between
[5]929particles within a
[61]930particle source (in m). <br> </p> </td> </tr>
931<tr> <td style="vertical-align: middle;" width="15%">
932<p><a href="chapter_4.2.html#pdz"><b>pdz</b></a></p>
933</td> <td style="vertical-align: middle;" width="5%">
934<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R
935(10)</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>10 * ( zu(2) - zu(1) )</i></p>
936</td> <td style="vertical-align: middle;" width="57%">
937<p>Distance along z between
[5]938particles within a particle source
[61]939(in m).</p> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#phi"><b>phi</b></a></p>
940</td> <td style="vertical-align: middle;" width="5%">
941<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
942</td> <td style="vertical-align: middle;" width="16%">
943<p><i>55.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Geographical
944latitude (in degrees). <br> </p> </td> </tr>
945<tr> <td style="vertical-align: middle;" width="15%">
946<p><a href="chapter_4.2.html#plot_spectra_level"><b>plot_spectra_level</b></a></p>
947</td> <td style="vertical-align: middle;" width="5%">
948<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>I
949(10)</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>No level</i></p>
950</td> <td style="vertical-align: middle;" width="57%">
951<p>Vertical level(s) for which horizontal spectra are to be
952plotted (in gridpoints). <br> </p> </td> </tr>
953<tr> <td style="vertical-align: middle;" width="15%">
954<p><a href="chapter_4.1.html#prandtl_layer"><b>prandtl_layer</b></a></p>
955</td> <td style="vertical-align: middle;" width="5%">
956<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>L</p>
957</td> <td style="vertical-align: middle;" width="16%">
958<p><i>.T.</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Parameter
959to switch on a Prandtl layer. <br> </p> </td> </tr>
960<tr> <td style="vertical-align: middle;" width="15%">
961<p><a href="chapter_4.2.html#prandtl_number"><b>prandtl_number</b></a></p>
962</td> <td style="vertical-align: middle;" width="5%">
963<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
964</td> <td style="vertical-align: middle;" width="16%">
965<p><i>1.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Ratio
966of the eddy diffusivities for momentum and heat (K<sub>m</sub>/K<sub>h</sub>).
967<br> </p> </td> </tr> <tr> <td style="vertical-align: middle;"><b><a href="chapter_4.1.html#precipitation"><b>precipitation</b></a></b></td>
968<td style="vertical-align: middle;">I<br> </td>
969<td style="vertical-align: middle;">L<br> </td>
970<td style="vertical-align: middle;"><span style="font-style: italic;">.F.</span></td> <td style="vertical-align: middle;">Parameter to
[5]971switch on the
[72]972precipitation scheme.</td> </tr> <tr><td><a style="font-weight: bold;" href="chapter_4.2.html#precipitation_amount_interval">precipitation_amount_<br>interval</a></td><td>R</td><td>R</td><td><i>value
973of &nbsp;<a href="chapter_4.2.html#dt_do2d_xy">dt_do2d_<br>
974xy</a></i></td><td><font face="Thorndale"><font face="Thorndale, serif">Temporal
975interval</font> for which the precipitation amount (in mm) shall be calculated and output (</font>in <font face="Thorndale">s).&nbsp;</font></td></tr><tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#profile_columns"><b>profile_columns</b></a></p>
[61]976</td> <td style="vertical-align: middle;" width="5%">
977<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>I</p>
978</td> <td style="vertical-align: middle;" width="16%">
979<p><i>3</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Number
980of coordinate systems to be plotted<span style="font-weight: bold;"></span>
981in one row by <span style="font-weight: bold;">profil</span>.
982<br> </p> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#profile_rows"><b>profile_rows</b></a></p>
983</td> <td style="vertical-align: middle;" width="5%">
984<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>I</p>
985</td> <td style="vertical-align: middle;" width="16%">
986<p><i>2</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Number
987of rows of coordinate systems to be plotted on
[5]988one page
989by <span style="font-weight: bold;">profil</span>. <br>
[61]990</p> </td> </tr> <tr valign="top"> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#psb"><b>psb</b></a></p>
991</td> <td style="vertical-align: middle;" width="5%">
992<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R
993(10)</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>10 * zu(nz/2)</i></p>
994</td> <td style="vertical-align: middle;" width="57%">
995<p>Bottom edge of a particle
996source (in m).</p> </td> </tr> <tr valign="top">
997<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#psl"><b>psl</b></a></p>
998</td> <td style="vertical-align: middle;" width="5%">
999<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R
1000(10)</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>10 * 0.0</i></p>
1001</td> <td style="vertical-align: middle;" width="57%">
1002<p>Left edge of a particle source
1003(in m). </p> </td> </tr> <tr valign="top">
1004<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#psn"><b>psn</b></a></p>
1005</td> <td style="vertical-align: middle;" width="5%">
1006<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R
1007(10)</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>10 * ( ny * dy )</i></p>
1008</td> <td style="vertical-align: middle;" width="57%">
1009<p>Rear (&ldquo;north&rdquo;) edge of a particle
1010source (in m).</p> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#psolver"><b>psolver</b></a></p>
1011</td> <td style="vertical-align: middle;" width="5%">
1012<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
1013* 10</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'poisfft'</i></p>
1014</td> <td style="vertical-align: middle;" width="57%">
1015<p>Scheme to be used to solve the Poisson equation for the
1016perturbation pressure. <br> </p> </td> </tr>
1017<tr valign="top"> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#psr"><b>psr</b></a></p>
1018</td> <td style="vertical-align: middle;" width="5%">
1019<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R
1020(10)</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>10 * ( nx * dx )</i></p>
1021</td> <td style="vertical-align: middle;" width="57%">
1022<p>Right edge of a particle source (in m).</p> </td>
1023</tr> <tr valign="top"> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#pss"><b>pss</b></a></p>
1024</td> <td style="vertical-align: middle;" width="5%">
1025<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R
1026(10)</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>10 * 0.0</i></p>
1027</td> <td style="vertical-align: middle;" width="57%">
1028<p>Front (&ldquo;south&rdquo;) edge of a particle
1029source (in m).</p> </td> </tr> <tr valign="top">
1030<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#pst"><b>pst</b></a></p>
1031</td> <td style="vertical-align: middle;" width="5%">
1032<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R
1033(10)</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>10 * zu(nz/2)</i></p>
1034</td> <td style="vertical-align: middle;" width="57%">
1035<p>Top edge of a particle source (in m).</p> </td> </tr>
1036<tr><td><a style="font-weight: bold;" href="chapter_4.1.html#pt_reference">pt_reference</a></td><td>I</td><td>R</td><td><span style="font-style: italic;">use horizontal average as
1037reference</span></td><td>Reference temperature to be
1038used in all buoyancy terms (in K).</td></tr><tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#pt_surface"><b>pt_surface</b></a></p>
1039</td> <td style="vertical-align: middle;" width="5%">
1040<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1041</td> <td style="vertical-align: middle;" width="16%">
1042<p><i>300.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Surface
1043potential temperature (in K). <br> </p> </td> </tr>
1044<tr> <td style="vertical-align: middle;" width="15%">
1045<p><a href="chapter_4.1.html#pt_surface_initial_change"><b>pt_surface_initial</b></a>&nbsp;&nbsp;&nbsp;
1046<br> <a href="chapter_4.1.html#pt_surface_initial_change">&nbsp;<b>_change</b></a></p>
1047</td> <td style="vertical-align: middle;" width="5%">
1048<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1049</td> <td style="vertical-align: middle;" width="16%">
1050<p><i>0.0</i></p> </td> <td style="vertical-align: middle;" width="57%">Change
[5]1051in surface
1052temperature to be made at the
1053beginning of
1054the 3d run
[61]1055(in K).&nbsp;</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#pt_vertical_gradient"><b>pt_vertical_gradient</b></a></p>
1056</td> <td style="vertical-align: middle;" width="5%">
1057<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R
1058(10)</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>10 * 0.0</i></p>
1059</td> <td style="vertical-align: middle;" width="57%">
1060<p>Temperature gradient(s) of the initial temperature
[5]1061profile (in
1062K
[61]1063/ 100 m). <br> </p> </td> </tr> <tr>
1064<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#pt_vertical_gradient_level"><b>pt_vertical_gradient</b></a>&nbsp;&nbsp;&nbsp;
1065<br> <a href="chapter_4.1.html#pt_vertical_gradient_level">&nbsp;<b>_level</b></a></p>
1066</td> <td style="vertical-align: middle;" width="5%">
1067<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R
1068(10)</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>10 *</i>&nbsp; <i>0.0</i></p>
1069</td> <td style="vertical-align: middle;" width="57%">
1070<p>Height level from which on the temperature gradient
[5]1071defined by <a href="chapter_4.1.html#pt_vertical_gradient">pt_vertical_gradient</a>
[61]1072is effective (in m).&nbsp;</p> </td> </tr> <tr>
1073<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#q_surface"><b>q_surface</b></a></p>
1074</td> <td style="vertical-align: middle;" width="5%">
1075<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1076</td> <td style="vertical-align: middle;" width="16%">
1077<p><i>0.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Surface
1078specific humidity / total water content (kg/kg). <br> </p>
1079</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#q_surface_initial_change"><b>q_surface_initial</b></a>
1080<br> <a href="chapter_4.1.html#q_surface_initial_change">&nbsp;<b>_change</b></a></p>
1081</td> <td style="vertical-align: middle;" width="5%">
1082<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1083</td> <td style="vertical-align: middle;" width="16%">
1084<p><i>0.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Change
1085in surface specific humidity / total water
[5]1086content to
1087be made at the beginning
[61]1088of the 3d run (kg/kg). <br> </p> </td> </tr>
1089<tr> <td style="vertical-align: middle;" width="15%">
1090<p><a href="chapter_4.1.html#q_vertical_gradient"><b>q_vertical_gradient</b></a></p>
1091</td> <td style="vertical-align: middle;" width="5%">
1092<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R
1093(10)</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>10 * 0.0</i></p>
1094</td> <td style="width: 57%; vertical-align: middle;">
1095<p>Humidity gradient(s) of the initial humidity profile
1096(in 1/100 m). </p> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#q_vertical_gradient_level"><b>q_vertical_gradient</b></a>
1097<br> <a href="chapter_4.1.html#q_vertical_gradient_level">&nbsp;<b>_level</b></a></p>
1098</td> <td style="vertical-align: middle;" width="5%">
1099<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R
1100(10)</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>10 *</i>&nbsp; <i>0.0</i></p>
1101</td> <td style="vertical-align: middle;" width="57%">
[75]1102<p>Height level from which on the humidity gradient defined
[5]1103by <a href="chapter_4.1.html#q_vertical_gradient">q_vertical_gradient</a>
[61]1104is effective (in m).&nbsp;</p> </td> </tr> <tr>
1105<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#radiation"><b>radiation</b></a></p>
1106</td> <td style="vertical-align: middle;" width="5%">
1107<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>L</p>
1108</td> <td style="vertical-align: middle;" width="16%">
1109<p><i>.F.</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Parameter
1110to switch on longwave radiation cooling at
1111cloud-tops. <br> </p> </td> </tr> <tr>
1112<td><a href="chapter_4.2.html#radius"><span style="font-weight: bold;">radius</span></a></td>
1113<td>P</td> <td>R (10)</td> <td><i>0.0,
11149</i>*<br> <i>9999999.9</i></td> <td>Particle
1115radius (in m).</td> </tr> <tr valign="top"> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#random_generator"><b>random_generator</b></a></p>
1116</td> <td style="vertical-align: middle;" width="5%">
1117<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
1118* 20</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'numerical recipes'</i></p>
1119</td> <td style="vertical-align: middle;" width="57%">
1120<p>Random number generator to be used for creating
[5]1121uniformly
[61]1122distributed random numbers. </p> </td> </tr> <tr>
1123<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#random_heatflux"><b>random_heatflux</b></a></p>
1124</td> <td style="vertical-align: middle;" width="5%">
1125<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>L</p>
1126</td> <td style="vertical-align: middle;" width="16%">
1127<p><i>.F.</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Parameter
1128to impose random perturbations on the internal two-dimensional near
1129surface heat flux field <span style="font-style: italic;">shf</span>.
1130</p> </td> </tr> <tr valign="top"> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#random_start_position"><b>random_start_position</b></a></p>
1131</td> <td style="vertical-align: middle;" width="5%">
1132<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>L</p>
1133</td> <td style="vertical-align: middle;" width="16%">
1134<p><i>.F.</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p><span style="background: transparent none repeat scroll 0% 50%; -moz-background-clip: initial; -moz-background-origin: initial; -moz-background-inline-policy: initial;"><span style="background: transparent none repeat scroll 0% 50%; -moz-background-clip: initial; -moz-background-origin: initial; -moz-background-inline-policy: initial;"><font color="#000000">Initial position of the</font></span>
[5]1135particles is
1136varied randomly within certain limits.&nbsp;</span></p>
[61]1137</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#rayleigh_damping_factor"><b>rayleigh_damping</b></a>&nbsp;&nbsp;
1138<br> <a href="chapter_4.2.html#rayleigh_damping_factor">&nbsp;<b>_factor</b></a></p>
1139</td> <td style="vertical-align: middle;" width="5%">
1140<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1141</td> <td style="vertical-align: middle;" width="16%">
1142<p><span style="font-style: italic;">0.0</span>
1143and/or <span style="font-style: italic;">0.01</span>
1144(see parameter description)</p> </td> <td style="vertical-align: middle;" width="57%"> <p>Factor
1145for Rayleigh damping.&nbsp;</p> </td> </tr> <tr>
1146<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#rayleigh_damping_height"><b>rayleigh_damping</b></a>&nbsp;&nbsp;
1147<br> <a href="chapter_4.2.html#rayleigh_damping_height">&nbsp;<b>_height</b></a></p>
1148</td> <td style="vertical-align: middle;" width="5%">
1149<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1150</td> <td style="vertical-align: middle; font-style: italic;" width="16%"> <p>2/3 * zu(nz)</p> </td> <td style="width: 57%; text-align: left; vertical-align: middle;">
1151<p>Height where the Rayleigh damping starts (in
1152m).&nbsp; </p> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#read_particles_from_restartfile"><b>read_particles_from_</b></a>
1153<br> <a href="chapter_4.2.html#read_particles_from_restartfile"><b>restartfile</b></a></p>
1154</td> <td style="vertical-align: middle;" width="5%">
1155<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>L</p>
1156</td> <td style="vertical-align: middle;" width="16%">
1157<p><i>.T.</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Read
1158particle data from the previous run. <br> </p> </td>
1159</tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.3.html#region"><b>region</b></a></p>
1160</td> <td style="vertical-align: middle;" width="5%">
1161<p>U</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
1162* 40 (0:9)</p> </td> <td style="vertical-align: middle;" width="16%"> <p>&nbsp;</p>
1163</td> <td style="vertical-align: middle;" width="57%">
1164<p>Name(s) of the subdomain(s) defined by the user.</p> </td>
1165</tr> <tr valign="top"> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#residual_limit"><b>residual_limit</b></a></p>
1166</td> <td style="vertical-align: middle;" width="5%">
1167<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1168</td> <td style="vertical-align: middle;" width="16%">
1169<p><i>1.0E-6</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Largest
1170residual permitted for the multi-grid scheme (in
1171s<sup>-2</sup>m<sup>-3</sup>). <br> </p>
1172</td> </tr> <tr> <td style="vertical-align: middle;"><b><a href="chapter_4.2.html#restart_time"><b>restart_time</b></a></b></td>
1173<td style="vertical-align: middle;">R<br> </td>
1174<td style="vertical-align: middle;">R<br> </td>
1175<td style="vertical-align: middle;">9999999.9<br> </td>
1176<td style="vertical-align: middle;">Simulated time
[5]1177after which a
1178restart run is to be carried out
[61]1179(in s).</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#rif_max"><b>rif_max</b></a></p>
1180</td> <td style="vertical-align: middle;" width="5%">
1181<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1182</td> <td style="vertical-align: middle;" width="16%">
1183<p><i>1.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Upper
1184limit of the flux-Richardson number. <br> </p> </td>
1185</tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#rif_min"><b>rif_min</b></a></p>
1186</td> <td style="vertical-align: middle;" width="5%">
1187<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1188</td> <td style="vertical-align: middle;" width="16%">
1189<p><i>- 5.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Lower
1190limit of the flux-Richardson number. <br> </p> </td>
1191</tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#roughness_length"><b>roughness_length</b></a></p>
1192</td> <td style="vertical-align: middle;" width="5%">
1193<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1194</td> <td style="vertical-align: middle;" width="16%">
1195<p><i>0.1</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Roughness
[97]1196length (in m). <br> </p> </td> </tr> <tr><td align="undefined" valign="undefined"><a href="chapter_4.1.html#sa_surface"><span style="font-weight: bold;">sa_surface</span></a></td><td align="undefined" valign="undefined">I</td><td align="undefined" valign="undefined">R</td><td align="undefined" valign="undefined"><span style="font-style: italic;">35.0</span></td><td align="undefined" valign="undefined">Surface salinity (in psu).</td></tr><tr><td align="undefined" valign="undefined"><a href="chapter_4.1.html#sa_vertical_gradient"><span style="font-weight: bold;">sa_vertical_gradient</span></a></td><td align="undefined" valign="undefined">I</td><td align="undefined" valign="undefined">R(10)</td><td align="undefined" valign="undefined"><span style="font-style: italic;">10 * 0.0</span></td><td align="undefined" valign="undefined">Salinity gradient(s) of the initial salinity profile (in psu
1197/ 100 m).</td></tr><tr><td align="undefined" valign="undefined"><a href="chapter_4.1.html#sa_vertical_gradient_level"><span style="font-weight: bold;">sa_vertical_gradient_level</span></a></td><td align="undefined" valign="undefined">I</td><td align="undefined" valign="undefined">R(10)</td><td align="undefined" valign="undefined"><span style="font-style: italic;">10 * 0.0</span></td><td align="undefined" valign="undefined">Height level from which on the salinity gradient defined by <a href="chapter_4.1.html#sa_vertical_gradient">sa_vertical_gradient</a>
1198is effective (in m).</td></tr><tr>
[61]1199<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#scalar_advec"><b>scalar_advec</b></a></p>
1200</td> <td style="vertical-align: middle;" width="5%">
1201<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
1202* 10</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'pw-scheme'</i></p>
1203</td> <td style="vertical-align: middle;" width="57%">
1204<p>Advection scheme to be used for the scalar quantities. <br>
1205</p> </td> </tr> <tr> <td><a href="chapter_4.2.html#section_xy"><span style="font-weight: bold;">section_xy</span></a></td>
1206<td>R</td> <td>I (100)</td> <td><span style="font-style: italic;">no section</span></td>
1207<td><font face="Thorndale">Position
1208of&nbsp;cross section(s) for&nbsp;output of 2d horizontal cross
1209sections (grid point index k).&nbsp;</font></td> </tr>
1210<tr> <td><a href="chapter_4.2.html#section_xz"><span style="font-weight: bold;">section_xz</span></a></td>
1211<td>R</td> <td>I (100)</td> <td><span style="font-style: italic;">no section</span></td>
1212<td><font face="Thorndale">Position
1213of&nbsp;cross section(s) for&nbsp;output of 2d (xz) vertical
1214cross sections (grid point index j).&nbsp;</font></td> </tr>
1215<tr> <td><a href="chapter_4.2.html#section_yz"><span style="font-weight: bold;">section_yz</span></a></td>
1216<td>R</td> <td>I (100)</td> <td><span style="font-style: italic;">no section</span></td>
1217<td><font face="Thorndale">Position
1218of&nbsp;cross section(s) for&nbsp;output of 2d (yz) vertical
1219cross sections (grid point index i).&nbsp;</font></td> </tr>
1220<tr> <td><a href="chapter_4.2.html#skip_particles_for_tail"><span style="font-weight: bold;">skip_particles_for_tail</span></a></td>
1221<td>P</td> <td>I</td> <td><span style="font-style: italic;">1</span></td> <td>Limit
1222the number of particle tails.</td> </tr> <tr> <td><a href="chapter_4.2.html#skip_time_data_output"><span style="font-weight: bold;">skip_time_data_output</span></a></td>
1223<td>R</td> <td>R</td> <td><span style="font-style: italic;">0.0</span></td> <td>No
1224data output before this interval has passed (in s).</td> </tr>
1225<tr> <td><a href="chapter_4.2.html#skip_time_data_output_av"><span style="font-weight: bold;">skip_time_data_output_av</span></a></td>
1226<td>R</td> <td>R</td> <td><span style="font-style: italic;">value of <a href="chapter_4.2.html#skip_time_data_output">skip_time_<br>
1227data_output</a></span></td> <td>No output of
1228temporally averaged 2d/3d data before this interval has passed (in s).</td>
1229</tr> <tr> <td><a href="chapter_4.2.html#skip_time_dopr"><span style="font-weight: bold;">skip_time_dopr</span></a></td>
1230<td>R</td> <td>R</td> <td><span style="font-style: italic;">value of <a href="chapter_4.2.html#skip_time_data_output">skip_time_<br>
1231data_output</a></span></td> <td>No output of
1232vertical profile data before this interval has passed (in s).</td>
1233</tr> <tr> <td><a href="chapter_4.2.html#skip_time_dosp"><span style="font-weight: bold;">skip_time_dosp</span></a></td>
1234<td>P</td> <td>R</td> <td><span style="font-style: italic;">value of <a href="chapter_4.2.html#skip_time_data_output">skip_time_<br>
1235data_output</a></span></td> <td>No output of
1236spectra data before this interval has passed (in s).</td> </tr>
1237<tr> <td><a href="chapter_4.2.html#skip_time_do2d_xy"><span style="font-weight: bold;">skip_time_do2d_xy</span></a></td>
1238<td>R</td> <td>R</td> <td><span style="font-style: italic;">value of <a href="chapter_4.2.html#skip_time_data_output">skip_time_<br>
1239data_output</a></span></td> <td>No output of
1240instantaneous horizontal cross section data before this interval has
1241passed (in s).</td> </tr> <tr> <td><a href="chapter_4.2.html#skip_time_do2d_xz"><span style="font-weight: bold;">skip_time_do2d_xz</span></a></td>
1242<td>R</td> <td>R</td> <td><span style="font-style: italic;">value of <a href="chapter_4.2.html#skip_time_data_output">skip_time_<br>
1243data_output</a></span></td> <td>No output of
1244instantaneous vertical (xz) cross section data before this interval has
1245passed (in s).</td> </tr> <tr> <td><a href="chapter_4.2.html#skip_time_do2d_yz"><span style="font-weight: bold;">skip_time_do2d_yz</span></a></td>
1246<td>R</td> <td>R</td> <td><span style="font-style: italic;">value of <a href="chapter_4.2.html#skip_time_data_output">skip_time_<br>
1247data_output</a></span></td> <td>No output of
1248instantaneous vertical (yz) cross section data before this interval has
1249passed (in s).<br> </td> </tr> <tr> <td><a href="chapter_4.2.html#skip_time_do3d"><span style="font-weight: bold;">skip_time_do3d</span></a></td>
1250<td>R</td> <td>R</td> <td><span style="font-style: italic;">value of <a href="chapter_4.2.html#skip_time_data_output">skip_time_<br>
1251data_output</a></span></td> <td>No output of
1252instantaneous 3d volume data before this interval has passed (in s).</td>
1253</tr> <tr> <td style="vertical-align: middle;"><b><a href="file:///home/raasch/public_html/PALM_group/doc/app/chapter_4.2.html#spectra_direction"><b>slicer_range_limits_dvrp</b></a></b></td>
1254<td style="vertical-align: middle;">P<br> </td>
1255<td style="vertical-align: middle;">R(2,10)<br> </td>
1256<td style="vertical-align: middle;"><span style="font-style: italic;">10
1257* (-1,1)</span></td> <td style="vertical-align: middle;">Ranges
[5]1258of values to which a color table has to be mapped (units of the
[61]1259respective quantity).</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#spectra_direction"><b>spectra_direction</b></a></p>
1260</td> <td style="vertical-align: middle;" width="5%">
1261<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
1262* 2 (10)</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>10 * ' '</i></p>
1263</td> <td style="vertical-align: middle;" width="57%">
1264<p>Direction(s) along which spectra are to be calculated. <br>
1265</p> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#statistic_regions"><b>statistic_regions</b></a></p>
1266</td> <td style="vertical-align: middle;" width="5%">
1267<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>I</p>
1268</td> <td style="vertical-align: middle;" width="16%">
1269<p><i>0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Number
1270of additional user-defined subdomains for which
[5]1271statistical analysis
1272and corresponding output (profiles, time series) shall be made.</p>
[61]1273</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#superelevation"><b>superelevation</b></a></p>
1274</td> <td style="vertical-align: middle;" width="5%">
1275<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1276</td> <td style="vertical-align: middle;" width="16%">
1277<p><i>1.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Superelevation
1278factor for the vertical coordinate. <br> </p> </td>
1279</tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#superelevation_x"><b>superelevation_x</b></a></p>
1280</td> <td style="vertical-align: middle;" width="5%">
1281<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1282</td> <td style="vertical-align: middle;" width="16%">
1283<p><i>1.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Superelevation
1284factor for the horizontal (x) coordinate. <br> </p> </td>
1285</tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#superelevation_y"><b>superelevation_y</b></a></p>
1286</td> <td style="vertical-align: middle;" width="5%">
1287<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1288</td> <td style="vertical-align: middle;" width="16%">
1289<p><i>1.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Superelevation
1290factor for the
1291horizontal (y) coordinate. <br> </p> </td> </tr>
1292<tr> <td style="vertical-align: middle;" width="15%">
1293<p><a href="chapter_4.1.html#surface_heatflux"><b>surface_heatflux</b></a></p>
1294</td> <td style="vertical-align: middle;" width="5%">
1295<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1296</td> <td style="vertical-align: middle;" width="16%">
1297<p><span style="font-style: italic;">no prescribed
1298heatflux</span></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Kinematic
1299sensible heat flux at the bottom surface (in K m/s).</p> </td>
1300</tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#surface_pressure"><b>surface_pressure</b></a></p>
1301</td> <td style="vertical-align: middle;" width="5%">
1302<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1303</td> <td style="vertical-align: middle;" width="16%">
1304<p><i>1013.25</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Atmospheric
1305pressure at the surface (in hPa)</p> </td> </tr> <tr>
1306<td style="vertical-align: middle;"><b><a href="chapter_4.1.html#surface_scalarflux"><b>surface_scalarflux</b></a></b></td>
1307<td style="vertical-align: middle;">I<br> </td>
1308<td style="vertical-align: middle;">R<br> </td>
1309<td style="vertical-align: middle;"><i>0.0</i></td>
1310<td style="vertical-align: middle;">Scalar flux at
[5]1311the surface
[61]1312(in kg/(m<sup>2</sup> s)). <br> </td> </tr>
1313<tr> <td style="vertical-align: middle;" width="15%">
1314<p><a href="chapter_4.1.html#surface_waterflux"><b>surface_waterflux</b></a></p>
1315</td> <td style="vertical-align: middle;" width="5%">
1316<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1317</td> <td style="vertical-align: middle;" width="16%">
1318<p><i>0.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Kinematic
1319water flux near the surface (in m/s). <br> </p> </td>
1320</tr> <tr> <td style="vertical-align: middle;"><b><a href="chapter_4.1.html#s_surface"><b>s_surface</b></a></b></td>
1321<td style="vertical-align: middle;">I<br> </td>
1322<td style="vertical-align: middle;">R<br> </td>
1323<td style="vertical-align: middle;"><i>0.0</i></td>
1324<td style="vertical-align: middle;">Surface value of
[5]1325the passive
[61]1326scalar (in kg/m<sup>3</sup>). <br> </td> </tr>
1327<tr> <td style="vertical-align: middle;"><b><b><a href="chapter_4.1.html#s_surface_initial_change"><b>s_surface_initial_change</b></a></b></b></td>
1328<td style="vertical-align: middle;">I<br> </td>
1329<td style="vertical-align: middle;">R<br> </td>
1330<td style="vertical-align: middle;"><i>0.0</i></td>
1331<td style="vertical-align: middle;">Change in
[5]1332surface scalar
1333concentration to be made at the
[61]1334beginning of the 3d run (in kg/m<sup>3</sup>). <br> </td>
1335</tr> <tr> <td style="vertical-align: middle;"><b><b><a href="chapter_4.1.html#s_vertical_gradient"><b>s_vertical_gradient</b></a></b></b></td>
1336<td style="vertical-align: middle;">I<br> </td>
1337<td style="vertical-align: middle;">R(10)<br> </td>
1338<td style="vertical-align: middle;"><i>10 * 0</i><i>.0</i></td>
1339<td style="vertical-align: middle;">Scalar
[5]1340concentration
1341gradient(s) of the initial scalar
1342concentration profile (in kg/m<sup>3 </sup>/
[61]1343100 m). <br> </td> </tr> <tr> <td><a href="chapter_4.1.html#s_vertical_gradient_level"><span style="font-weight: bold;">s_vertical_gradient_level</span></a></td>
1344<td>I</td> <td>R(10)</td> <td><span style="font-style: italic;">10 * 0.0</span></td>
1345<td>Height level from which on the scalar gradient defined by <a href="chapter_4.1.html#s_vertical_gradient">s_vertical_gradient</a>
1346is effective (in m).</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#termination_time_needed"><b>termination_time</b></a>&nbsp;&nbsp;
1347<br> <a href="chapter_4.2.html#termination_time_needed">&nbsp;<b>_needed</b></a></p>
1348</td> <td style="vertical-align: middle;" width="5%">
1349<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1350</td> <td style="vertical-align: middle;" width="16%">
1351<p><i>35.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>CPU
1352time needed for terminal actions at the end of a run
[5]1353in
[61]1354batch mode (in s).</p> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#threshold"><b>threshold</b></a></p>
1355</td> <td style="vertical-align: middle;" width="5%">
1356<p>P</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R
1357(10)</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>0.0</i></p> </td>
1358<td style="vertical-align: middle;" width="57%"> <p>Threshold
1359value for which an isosurface is to be created
[5]1360by
1361the <span style="font-weight: bold;">dvrp</span>
[61]1362software. <br> </p> </td> </tr> <tr>
1363<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#timestep_scheme"><b>timestep_scheme</b></a></p>
1364</td> <td style="vertical-align: middle;" width="5%">
1365<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>C
1366* 20</p> </td> <td style="vertical-align: middle;" width="16%"> <p><i>'runge-kutta-3'</i></p>
1367</td> <td style="vertical-align: middle;" width="57%">
1368<p>Time step scheme to be used for integration of the prognostic
1369variables. <br> </p> </td> </tr> <tr>
1370<td><a href="chapter_4.1.html#topography"><span style="font-weight: bold;">topography</span></a></td>
1371<td>I</td> <td>C * 40</td> <td><span style="font-style: italic;">'flat'</span></td> <td>Topography
1372mode.</td> </tr> <tr><td><a style="font-weight: bold;" href="chapter_4.1.html#top_heatflux">top_heatflux</a></td><td>I</td><td>R</td><td><span style="font-style: italic;">no prescribed heatflux</span></td><td>Kinematic
[97]1373sensible heat flux at the top surface (in K m/s).</td></tr><tr><td align="undefined" valign="undefined"><a href="chapter_4.1.html#top_salinityflux"><span style="font-weight: bold;">top_salinityflux</span></a></td><td align="undefined" valign="undefined">I</td><td align="undefined" valign="undefined">R</td><td align="undefined" valign="undefined"><span style="font-style: italic;">no prescribed</span><br style="font-style: italic;"><span style="font-style: italic;">salinityflux</span></td><td align="undefined" valign="undefined">Kinematic
1374salinity flux at the top boundary, i.e. the sea surface (in psu m/s).</td></tr><tr>
[61]1375<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#ug_surface"><b>ug_surface</b></a></p>
1376</td> <td style="vertical-align: middle;" width="5%">
1377<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1378</td> <td style="vertical-align: middle;" width="16%">
1379<p><i>0.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>u-component
1380of the geostrophic wind at the surface (in m/s). <br> </p>
1381</td> </tr> <tr> <td><a href="chapter_4.1.html#ug_vertical_gradient"><span style="font-weight: bold;">ug_vertical_gradient</span></a></td>
1382<td>I</td> <td>R(10)</td> <td><span style="font-style: italic;">10 * 0.0</span></td>
1383<td>Gradient(s) of the initial
1384profile of the&nbsp; u-component of the geostrophic wind (in
13851/100s).</td> </tr> <tr> <td><a href="chapter_4.1.html#ug_vertical_gradient_level"><span style="font-weight: bold;">ug_vertical_gradient_level</span></a></td>
1386<td>I</td> <td>R(10)</td> <td><span style="font-style: italic;">10 * 0.0</span></td>
1387<td>Height level from which on the
[5]1388gradient defined by <a href="chapter_4.1.html#ug_vertical_gradient">ug_vertical_gradient</a>
[61]1389is effective (in m).<br> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#ups_limit_e"><b>ups_limit_e</b></a></p>
1390</td> <td style="vertical-align: middle;" width="5%">
1391<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1392</td> <td style="vertical-align: middle;" width="16%">
1393<p><i>0.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Subgrid-scale
1394turbulent kinetic energy difference used
[5]1395as
1396criterion for applying the upstream scheme when upstream-spline
1397advection is switched on (in m<sup>2</sup>/s<sup>2</sup>).
[61]1398&nbsp;</p> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#ups_limit_pt"><b>ups_limit_pt</b></a></p>
1399</td> <td style="vertical-align: middle;" width="5%">
1400<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1401</td> <td style="vertical-align: middle;" width="16%">
1402<p><i>0.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Temperature
1403difference used as criterion for
[5]1404applying&nbsp;
1405the upstream scheme when upstream-spline advection&nbsp; is
1406switched on
[61]1407(in K). <br> </p> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#ups_limit_u"><b>ups_limit_u</b></a></p>
1408</td> <td style="vertical-align: middle;" width="5%">
1409<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1410</td> <td style="vertical-align: middle;" width="16%">
1411<p><i>0.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Velocity
1412difference (u-component) used as criterion for
[5]1413applying the upstream scheme
[61]1414when upstream-spline advection is switched on (in m/s). <br> </p>
1415</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#ups_limit_v"><b>ups_limit_v</b></a></p>
1416</td> <td style="vertical-align: middle;" width="5%">
1417<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1418</td> <td style="vertical-align: middle;" width="16%">
1419<p><i>0.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Velocity
1420difference (v-component) used as criterion for
[5]1421applying the upstream scheme
[61]1422when upstream-spline advection is switched on (in m/s). <br> </p>
1423</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#ups_limit_w"><b>ups_limit_w</b></a></p>
1424</td> <td style="vertical-align: middle;" width="5%">
1425<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1426</td> <td style="vertical-align: middle;" width="16%">
1427<p><i>0.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Velocity
1428difference (w-component) used as criterion for
[5]1429applying the upstream scheme
[61]1430when upstream-spline advection is switched on (in m/s). <br> </p>
1431</td> </tr> <tr> <td><a href="chapter_4.2.html#use_particle_tails"><span style="font-weight: bold;">use_particle_tails</span></a></td>
1432<td>P</td> <td>L</td> <td>.F.</td>
1433<td>Give particles a tail.</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#use_prior_plot1d_parameters"><b>use_prior_plot1d</b></a>&nbsp;&nbsp;
1434<br> <a href="chapter_4.2.html#use_prior_plot1d_parameters">&nbsp;<b>_parameters</b></a></p>
1435</td> <td style="vertical-align: middle;" width="5%">
1436<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>L</p>
1437</td> <td style="vertical-align: middle;" width="16%">
1438<p><i>.F.</i></p> </td> <td style="width: 57%; text-align: left; vertical-align: middle;">
1439<p>Additional plot of vertical profile data with <span style="font-weight: bold;">profil</span> from
[5]1440preceding runs of the
[61]1441job chain.&nbsp; </p> </td> </tr> <tr> <td align="undefined" valign="undefined"><a href="chapter_4.2.html#use_sgs_for_particles"><span style="font-weight: bold;">use_sgs_for_particles</span></a></td>
1442<td align="undefined" valign="undefined">P</td>
1443<td align="undefined" valign="undefined">L</td>
1444<td align="undefined" valign="undefined"><span style="font-style: italic;">.F.</span></td> <td align="undefined" valign="undefined">Use
1445subgrid-scale velocities for particle advection.</td> </tr>
1446<tr> <td style="vertical-align: middle;" width="15%">
1447<p><a href="chapter_4.1.html#use_surface_fluxes"><b>use_surface_fluxes</b></a></p>
1448</td> <td style="vertical-align: middle;" width="5%">
1449<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>L</p>
1450</td> <td style="vertical-align: middle;" width="16%">
1451<p><i>.F.</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Parameter
1452to steer the treatment of the subgrid-scale
[5]1453vertical
[61]1454fluxes within the diffusion terms at k=1 (bottom boundary).</p> </td>
1455</tr> <tr><td><a style="font-weight: bold;" href="chapter_4.1.html#use_top_fluxes">use_top_fluxes</a></td><td>I</td><td>L</td><td><span style="font-style: italic;">.F.</span></td><td>Parameter
1456to steer the treatment of the subgrid-scale
[40]1457vertical
[61]1458fluxes within the diffusion terms at k=nz (top boundary).</td></tr><tr valign="top"> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#use_ug_for_galilei_tr"><b>use_ug_for_galilei_tr</b></a></p>
1459</td> <td style="vertical-align: middle;" width="5%">
1460<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>L</p>
1461</td> <td style="vertical-align: middle;" width="16%">
1462<p><i>.T.</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Switch
1463to determine the translation velocity in case
[5]1464that a
[61]1465Galilean transformation is used.</p> </td> </tr> <tr>
1466<td align="undefined" valign="undefined"><a href="chapter_4.1.html#use_upstream_for_tke"><span style="font-weight: bold;">use_upstream_for_tke</span></a></td>
1467<td align="undefined" valign="undefined">I</td>
1468<td align="undefined" valign="undefined">L</td>
1469<td align="undefined" valign="undefined"><span style="font-style: italic;">.F.</span></td> <td align="undefined" valign="undefined">Parameter to
1470choose the advection/timestep scheme to be used for the subgrid-scale
1471TKE.</td> </tr> <tr> <td style="vertical-align: middle;"> <p><a href="chapter_4.2.html#vertical_particle_advection"><b>vertical_particle_advection</b></a><br>
1472</p> </td> <td style="vertical-align: middle;">P<br>
1473</td> <td style="vertical-align: middle;">L<br>
1474</td> <td style="vertical-align: middle;"><i>.T.</i></td>
1475<td style="vertical-align: middle;">Switch on/off
[5]1476vertical
[61]1477particle transport.</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#vg_surface"><b>vg_surface</b></a></p>
1478</td> <td style="vertical-align: middle;" width="5%">
1479<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1480</td> <td style="vertical-align: middle;" width="16%">
1481<p><i>0.0</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>v-component
1482of the geostrophic wind at the surface (in m/s).</p> </td>
1483</tr> <tr> <td><a href="chapter_4.1.html#vg_vertical_gradient"><span style="font-weight: bold;">vg_vertical_gradient</span></a></td>
1484<td>I</td> <td>R(10)</td> <td><span style="font-style: italic;">10 * 0.0</span></td>
1485<td>Gradient(s) of the initial
1486profile of the&nbsp; v-component of the geostrophic wind (in
14871/100s).</td> </tr> <tr> <td><a href="chapter_4.1.html#vg_vertical_gradient_level"><span style="font-weight: bold;">vg_vertical_gradient_level</span></a></td>
1488<td>I</td> <td>R(10)</td> <td><span style="font-style: italic;">10 * 0.0</span></td>
1489<td>Height level from which on the
[5]1490gradient defined by <a href="chapter_4.1.html#vg_vertical_gradient">vg_vertical_gradient</a>
[61]1491is effective (in m).</td> </tr> <tr valign="top">
1492<td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.1.html#wall_adjustment"><b>wall_adjustment</b></a></p>
1493</td> <td style="vertical-align: middle;" width="5%">
1494<p>I</p> </td> <td style="vertical-align: middle;" width="7%"> <p>L</p>
1495</td> <td style="vertical-align: middle;" width="16%">
1496<p><i>.T.</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Parameter
1497to restrict the mixing length in the vicinity
[5]1498of the
1499bottom
[61]1500boundary.</p> </td> </tr> <tr> <td><a href="chapter_4.1.html#wall_heatflux"><span style="font-weight: bold;">wall_heatflux</span></a></td>
1501<td>I</td> <td>R(5)</td> <td><span style="font-style: italic;">5 * 0.0</span></td> <td>Prescribed
1502kinematic sensible heat flux in W m<sup>-2</sup>&nbsp;at
1503the five topography faces.</td> </tr> <tr> <td style="vertical-align: middle;"> <p><a href="chapter_4.2.html#write_particle_statistics"><b>write_particle_</b></a>
1504<br> <a href="chapter_4.2.html#write_particle_statistics"><b>statistics</b></a>
1505</p> </td> <td style="vertical-align: middle;">P<br>
1506</td> <td style="vertical-align: middle;">L<br>
1507</td> <td style="vertical-align: middle;"><i>.F.</i></td>
1508<td style="vertical-align: middle;">Switch on/off
[5]1509output of
[61]1510particle informations.</td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#z_max_do1d"><b>z_max_do1d</b></a></p>
1511</td> <td style="vertical-align: middle;" width="5%">
1512<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1513</td> <td style="vertical-align: middle;" width="16%"><i>zu(nzt+1)
1514(model top)</i></td> <td style="vertical-align: middle;" width="57%"> <p>Height level up to which horizontally
1515averaged profiles
[5]1516are to
1517be
1518plotted with <span style="font-weight: bold;">profil</span>
1519(in
[61]1520m). <br> </p> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#z_max_do1d_normalized"><b>z_max_do1d</b></a>&nbsp;&nbsp;
1521<br> <a href="chapter_4.2.html#z_max_do1d_normalized">&nbsp;<b>_normalized</b></a></p>
1522</td> <td style="vertical-align: middle;" width="5%">
1523<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1524</td> <td style="vertical-align: middle;" width="16%">
1525<p><i>determined by plot <br>
1526data</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Normalized
1527height level up to which horizontally
[5]1528averaged
1529profiles are to be plotted with <span style="font-weight: bold;">profil</span>.
[61]1530<br> </p> </td> </tr> <tr> <td style="vertical-align: middle;" width="15%"> <p><a href="chapter_4.2.html#z_max_do2d"><b>z_max_do2d</b></a></p>
1531</td> <td style="vertical-align: middle;" width="5%">
1532<p>R</p> </td> <td style="vertical-align: middle;" width="7%"> <p>R</p>
1533</td> <td style="vertical-align: middle;" width="16%">
1534<p><i>zu(nz)</i></p> </td> <td style="vertical-align: middle;" width="57%"> <p>Height
1535level up to which 2d cross sections are to be
[5]1536plotted
1537with <span style="font-weight: bold;">iso2d</span>
[61]1538(in m). <br> </p> </td> </tr> </tbody>
1539</table><hr>
1540<p><br><font color="#000080"><a href="chapter_4.5.6.html"><font color="#000080"><img src="left.gif" name="Grafik1" align="bottom" border="2" height="32" width="32"></font></a><a href="index.html"><font color="#000080"><img src="up.gif" name="Grafik2" align="bottom" border="2" height="32" width="32"></font></a><a href="chapter_5.0.html"><font color="#000080"><img src="right.gif" name="Grafik3" align="bottom" border="2" height="32" width="32"></font></a></font></p>
1541<p>&nbsp;<i>Last change:&nbsp;&nbsp;</i>
1542$Id: chapter_4.6.html 97 2007-06-21 08:23:15Z raasch $ </p>
1543<p><br><br>
1544<br></p>
[40]1545</body></html>
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