| 13 | |---------------- |
| 14 | {{{#!td style="vertical-align:top;width: 50px" |
| 15 | 22/02/12 |
| 16 | }}} |
| 17 | {{{#!td style="vertical-align:top;width: 50px" |
| 18 | SR |
| 19 | }}} |
| 20 | {{{#!td style="vertical-align:top;width: 75px" |
| 21 | r831 |
| 22 | }}} |
| 23 | {{{#!td style="vertical-align:top" |
| 24 | 3.8 |
| 25 | }}} |
| 26 | {{{#!td style="vertical-align:top" |
| 27 | N |
| 28 | }}} |
| 29 | {{{#!td style="vertical-align:top" |
| 30 | The growth equation for water droplets due to condensation now considers the dependency of water thermal conductivity from temperature (from Rogers and Yau, Table 7.1), as well as the dependency of water vapor diffusivity from temperature and pressure (after Hall und Pruppacher, 1976). This may effect condensation/evaporation considerably. (advec_particles) |
| 31 | }}} |