The role of interchange reconnection as a drive mechanism for the solar wind
is explored by solving the global magnetic-field-aligned equations describing
wind acceleration. Boundary conditions in the low corona, including a
reconnection-driven Alfv\'enic outflow and associated heating differ from
previous models. Additional heating of the corona associated with Alfv\'en
waves or other MHD turbulence, which has been the foundation of many earlier
models, is neglected. For this simplified model a sufficient condition for
interchange reconnection to overcome gravity to drive the wind is derived. The
combination of Alfv\'enic ejection and reconnection-driven heating yields a
minimum value of the Alfv\'en speed of the order of 350-400km/s that is
required to drive the wind. Recent evidence based on Parker Solar Probe (PSP)
observations suggests that this threshold is typically exceeded in the coronal
holes that are the source regions of the fast wind. On the other hand, since
reconnection in the coronal environment is predicted to have a bursty
character, the magnitude of reconnection outflows can be highly variable. The
consequence is a highly non-uniform wind in which in some regions the velocity
increases sharply to super-Alfv\'enic values while in adjacent regions the
formation of an asymptotic wind fails. A simple model is constructed to
describe the turbulent mixing of these highly-sheared super-Alfv\'enic flows
that suggests these flows are the free-energy source of the Alfv\'enic
turbulence and associated switchbacks that have been documented in the PSP data
in the near coronal environment. The global wind profiles are presented and
benchmarked with Parker Solar Probe (PSP) observations at 12 solar radii