Changes between Version 205 and Version 206 of doc/tec/changelog_2018

Timestamp:

Nov 29, 2012 5:00:17 PM (12 years ago)

Author:

franke

Comment:

--

doc/tec/changelog_2018

@@ -11 +11 @@
 
 ||='''Date'''  =||='''Author'''  =||='''svn\\Revision'''  =||='''Last\\Release'''  =||='''Type''' =||='''Description''' =||
+|----------------
+{{{#!td style="vertical-align:top;width: 50px"
+29/11/12
+}}}
+{{{#!td style="vertical-align:top;width: 50px"
+TR
+}}}
+{{{#!td style="vertical-align:top;width: 75px"
+r1071
+}}}
+{{{#!td style="vertical-align:top"
+3.9
+}}}
+{{{#!td style="vertical-align:top"
+N, C, B
+}}}
+{{{#!td style="vertical-align:top"
+'''New:''' 
+Ventilation effect for evaporation of large cloud droplets included. (lpm_droplet_condensation)
+
+'''Changed:''' \\
+Removed unnecessary calculations in lpm_droplet_condensation.
+
+Calculation of droplet growth due to collisions now uses collision-coalescence formulation proposed by Wang in case of Hall and Wang kernel. (lpm_droplet_collision)
+
+'''Bugfixes:'''\\
+Collision efficiencies for Hall kernel should not be negative. (lpm_collision_kernels)
+
+Surface tension for calculation of cloud droplet condensation/evaporation using Rosenbrock method corrected. (lpm_droplet_condensation)
+
+Check for unreasonable results included in calculation of Rosenbrock method since unreasonable results may occur if external conditions significantly change. For the same reason the first internal time step in Rosenbrock method should be < 1.0E02 in case of evaporation. (lpm_droplet_condensation)
+
+Message identifiers added. (lpm_droplet_collision)
+}}}
 |----------------
 {{{#!td style="vertical-align:top;width: 50px"