$Ae^{-B(\mathrm{tau}-C)^2}$ $\begin{cases}\mathrm{time\_} & \text{if $\mathrm{time\_}\le \mathrm{period}$}\\ \mathrm{time\_}-\mathrm{period} & \text{if $\mathrm{time\_}\le \mathrm{period}\times 2$}\\ \mathrm{time\_}-\mathrm{period}\times 2 & \text{if $\mathrm{time\_}\le \mathrm{period}\times 3$}\\ \mathrm{time\_}-\mathrm{period}\times 3 & \text{if $\mathrm{time\_}\le \mathrm{period}\times 4$}\\ \mathrm{time\_}-\mathrm{period}\times 4 & \text{if $\mathrm{time\_}\le \mathrm{period}\times 5$}\\ \mathrm{time\_}-\mathrm{period}\times 5 & \text{if $\mathrm{time\_}\le \mathrm{period}\times 6$}\\ \mathrm{time\_}-\mathrm{period}\times 6 & \text{if $\mathrm{time\_}\le \mathrm{period}\times 7$}\\ \mathrm{time\_}-\mathrm{period}\times 7 & \text{if $\mathrm{time\_}\le \mathrm{period}\times 8$}\\ \mathrm{time\_}-\mathrm{period}\times 8 & \text{if $\mathrm{time\_}\le \mathrm{period}\times 9$}\\ \mathrm{time\_}-\mathrm{period}\times 9 & \text{if $\mathrm{time\_}\le \mathrm{period}\times 10$}\\ \mathrm{time\_}-\mathrm{period}\times 10 & \text{if $\mathrm{time\_}\le \mathrm{period}\times 11$}\\ \mathrm{time\_}-\mathrm{period}\times 11 & \text{if $\mathrm{time\_}\le \mathrm{period}\times 12$}\\ \mathrm{time\_}-\mathrm{period}\times 12 & \text{if $\mathrm{time\_}\le \mathrm{period}\times 13$}\end{cases}$ $\mathrm{V\_lv}+\mathrm{V\_rv}$ $\mathrm{P\_0\_pcd}(e^{\mathrm{lambda\_pcd}(\mathrm{V\_pcd}-\mathrm{V\_0\_pcd})}-1)$ $\mathrm{P\_pcd}+\mathrm{P\_th}$ $\mathrm{E\_es\_lvf}(\mathrm{V\_lvf}-\mathrm{V\_d\_lvf})$ $\mathrm{P\_0\_lvf}(e^{\mathrm{lambda\_lvf}(\mathrm{V\_lvf}-\mathrm{V\_0\_lvf})}-1)$ $\mathrm{V\_lv}-\mathrm{V\_spt}$ $\mathrm{e\_t}\mathrm{P\_es\_lvf}-1\mathrm{P\_ed\_lvf}$ $\mathrm{P\_lvf}+\mathrm{P\_peri}$ $\begin{cases}0 & \text{if $(\mathrm{Q\_mt}< 0)\land (\mathrm{Q\_av}< 0)$}\\ -\mathrm{Q\_av} & \text{if $\mathrm{Q\_mt}< 0$}\\ \mathrm{Q\_mt} & \text{if $\mathrm{Q\_av}< 0$}\\ \mathrm{Q\_mt}-\mathrm{Q\_av} & \text{otherwise}\end{cases}$ $\mathrm{E\_es\_rvf}(\mathrm{V\_rvf}-\mathrm{V\_d\_rvf})$ $\mathrm{P\_0\_rvf}(e^{\mathrm{lambda\_rvf}(\mathrm{V\_rvf}-\mathrm{V\_0\_rvf})}-1)$ $\mathrm{V\_rv}+\mathrm{V\_spt}$ $\mathrm{e\_t}\mathrm{P\_es\_rvf}-1\mathrm{P\_ed\_rvf}$ $\mathrm{P\_rvf}+\mathrm{P\_peri}$ $\begin{cases}0 & \text{if $(\mathrm{Q\_tc}< 0)\land (\mathrm{Q\_pv}< 0)$}\\ -\mathrm{Q\_pv} & \text{if $\mathrm{Q\_tc}< 0$}\\ \mathrm{Q\_tc} & \text{if $\mathrm{Q\_pv}< 0$}\\ \mathrm{Q\_tc}-\mathrm{Q\_pv} & \text{otherwise}\end{cases}$ $\mathrm{E\_es\_pa}(\mathrm{V\_pa}-\mathrm{V\_d\_pa})+\mathrm{P\_th}$ $\begin{cases}-\mathrm{Q\_pul} & \text{if $\mathrm{Q\_pv}< 0$}\\ \mathrm{Q\_pv}-\mathrm{Q\_pul} & \text{otherwise}\end{cases}$ $\mathrm{E\_es\_pu}(\mathrm{V\_pu}-\mathrm{V\_d\_pu})+\mathrm{P\_th}$ $\begin{cases}\mathrm{Q\_pul} & \text{if $\mathrm{Q\_mt}< 0$}\\ \mathrm{Q\_pul}-\mathrm{Q\_mt} & \text{otherwise}\end{cases}$ $\mathrm{E\_es\_ao}(\mathrm{V\_ao}-\mathrm{V\_d\_ao})$ $\begin{cases}-\mathrm{Q\_sys} & \text{if $\mathrm{Q\_av}< 0$}\\ \mathrm{Q\_av}-\mathrm{Q\_sys} & \text{otherwise}\end{cases}$ $\mathrm{E\_es\_vc}(\mathrm{V\_vc}-\mathrm{V\_d\_vc})$ $\begin{cases}\mathrm{Q\_sys} & \text{if $\mathrm{Q\_tc}< 0$}\\ \mathrm{Q\_sys}-\mathrm{Q\_tc} & \text{otherwise}\end{cases}$ $\frac{\mathrm{P\_ao}-\mathrm{P\_vc}}{\mathrm{R\_sys}}$ $\frac{\mathrm{P\_pa}-\mathrm{P\_pu}}{\mathrm{R\_pul}}$ $\begin{cases}0 & \text{if $(\mathrm{P\_pu}-\mathrm{P\_lv}< 0)\land (\mathrm{Q\_mt}< 0)$}\\ \frac{\mathrm{P\_pu}-\mathrm{P\_lv}-\mathrm{Q\_mt}\mathrm{R\_mt}}{\mathrm{L\_mt}} & \text{otherwise}\end{cases}$ $\begin{cases}0 & \text{if $(\mathrm{P\_lv}-\mathrm{P\_ao}< 0)\land (\mathrm{Q\_av}< 0)$}\\ \frac{\mathrm{P\_lv}-\mathrm{P\_ao}-\mathrm{Q\_av}\mathrm{R\_av}}{\mathrm{L\_av}} & \text{otherwise}\end{cases}$ $\begin{cases}0 & \text{if $(\mathrm{P\_vc}-\mathrm{P\_rv}< 0)\land (\mathrm{Q\_tc}< 0)$}\\ \frac{\mathrm{P\_vc}-\mathrm{P\_rv}-\mathrm{Q\_tc}\mathrm{R\_tc}}{\mathrm{L\_tc}} & \text{otherwise}\end{cases}$ $\begin{cases}0 & \text{if $(\mathrm{P\_rv}-\mathrm{P\_pa}< 0)\land (\mathrm{Q\_pv}< 0)$}\\ \frac{\mathrm{P\_rv}-\mathrm{P\_pa}-\mathrm{Q\_pv}\mathrm{R\_pv}}{\mathrm{L\_pv}} & \text{otherwise}\end{cases}$