| 78 | | The [#morrison2007 Morrison et al. (2007)] microphysics scheme can be understood as an extension of the scheme of [#seifert2001 Seifert and Beheng (2001],[#seifert2006 2006)], where ''N'',,c,, and ''q'',,c,, are prognostic quantities as well. Moreover, using the [#morrison2007 Morrison et al. (2007)] scheme includes an explicit calculation of diffusional growth and an activation parameterization. |
| | 78 | The [#morrison2007 Morrison et al. (2007)] microphysics scheme can be understood as an extension of the scheme of [#seifert2001 Seifert and Beheng (2001],[#seifert2006 2006)], where ''N'',,c,, and ''q'',,c,, are prognostic quantities as well. |
| | 79 | {{{ |
| | 80 | #!Latex |
| | 81 | \begin{align*} |
| | 82 | \frac{\partial N_\mathrm{c}}{\partial t} = - u_j \frac{\partial N_\mathrm{c}}{\partial x_j} - \frac{\partial}{\partial x_j}\left(\overline{u_j^{\prime\prime}N_\mathrm{c}^{\prime\prime}}\right) + \Psi_{N_\mathrm{c}},\\ |
| | 83 | \frac{\partial q_\mathrm{c}}{\partial t} = - u_j |
| | 84 | \frac{\partial q_\mathrm{c}}{\partial x_j} - \frac{\partial}{\partial |
| | 85 | x_j}\left(\overline{u_j^{\prime\prime}q_\mathrm{c}^{\prime\prime}}\right) |
| | 86 | + \Psi_{q_\mathrm{c}}, |
| | 87 | \end{align*} |
| | 88 | }}} |
| | 89 | |
| | 90 | Moreover, using the [#morrison2007 Morrison et al. (2007)] scheme includes an explicit calculation of diffusional growth and an activation parameterization. |
