Using the Modern-Era Retrospective Analysis for Research and Applications (MERRA) reanalysis winds, temperatures, and anvil cloud ice, we use our domain-filling, forward trajectory model combined with a new cloud module to show that convective transport of saturated air and ice to altitudes below the tropopause has a significant impact on stratospheric water vapor and upper tropospheric clouds. We find that including cloud microphysical processes (rather than assuming that parcel water vapor never exceeds saturation) increases the lower stratospheric average H 2 O by 10-20%. Our model-computed cloud fraction shows reasonably good agreement with tropical upper troposphere (TUT) cloud frequency observed by the Cloud-Aerosol Lidar with Orthogonal Polarization (CALIOP) instrument in boreal winter with poorer agreement in summer. Our results suggest that over 40% of TUT cirrus is due to convection, and it is the saturated air from convection rather than injected cloud ice that primarily contributes to this increase. Convection can add up to 13% more water to the stratosphere. With just convective hydration (convection adds vapor up to saturation), the global lower stratospheric modeled water vapor is close to Microwave Limb Sounder observations. Adding convectively injected ice increases the modeled water vapor to~8% over observations. Improving the representation of MERRA tropopause temperatures fields reduces stratospheric water vapor by~4%. Trajectory models have demonstrated success at simulating many aspects of stratospheric H 2 O [e.g., Fueglistaler et al., 2005; Schoeberl and Dessler, 2011, hereafter SD11; Schoeberl et al., 2012, hereafter S12; Schoeberl et al., 2013, hereafter S13;Ueyama et al., 2014]. In the SD11 forward domain-filling trajectory model, winds determine the parcel motion and temperature determines the H 2 O content through instant adjustment of the parcel water vapor to not exceed predefined saturation limit. The assumption in this formulation is that any ice that forms quickly falls to lower atmospheric layers. We refer to this adjustment as instantaneous dehydration (ID).Air parcels moving slowly upward across the tropopause will have their water vapor concentration fixed as they pass through the cold point. However, convective systems can bypass the cold point and deposit ice directly into the lower stratosphere. Hydration through convection was parameterized in SD11 through a system described by Dessler et al. [2007]. In that system, parcels coincident with convection were set to the local saturation mixing ratio. Methane oxidation can also add water to the air parcel, but this process is unimportant in the lower tropical stratosphere where methane oxidation rates are slow (SD11).In SD11 and S12, we compared the modeled stratospheric water vapor to Microwave Limb Sounder (MLS) observations. These papers identified a number of processes that controlled stratospheric water vapor. These processes include the following: (1) the level of supersaturation permitted before ID, (2) the level of c...