We investigate the magnetism of a previously unexplored distorted spin-1/2 kagome model consisting of three symmetry-inequivalent nearest-neighbor antiferromagnetic Heisenberg couplings J ⬡, J, and \[J^{\prime}\] , and uncover a rich ground state phase diagram even at the classical level. Using analytical arguments and numerical techniques we identify a collinear \[\overrightarrow{Q}=0\] magnetic phase, two unusual non-collinear coplanar \[\overrightarrow{Q}=(1/3,1/3)\] phases and a classical spin liquid phase with a degenerate manifold of non-coplanar ground states, resembling the jammed spin liquid phase found in the context of a bond-disordered kagome antiferromagnet. We further show with density functional theory calculations that the recently synthesized Y-kapellasite Y 3Cu 9(OH) 19Cl 8 is a realization of this model and predict its ground state to lie in the region of \[\overrightarrow{Q}=(1/3,1/3)\] order, which remains stable even after the inclusion of quantum fluctuation effects within variational Monte Carlo and pseudofermion functional renormalization group. The presented model opens a new direction in the study of kagome antiferromagnets.