Distinctive orderings and phase diagram structures are found, from renormalization-group theory, for odd q-state clock spin-glass models in d=3 dimensions. These models exhibit asymmetric phase diagrams, as is also the case for quantum Heisenberg spin-glass models. No finite-temperature spin-glass phase occurs. For all odd $qgeqslant 5$, algebraically ordered antiferromagnetic phases occur. One such phase is dominant and occurs for all $qgeqslant 5$. Other such phases occupy small low-temperature portions of the phase diagrams and occur for $5 leqslant q leqslant 15$. All algebraically ordered phases have the same structure, determined by an attractive finite-temperature sink fixed point where a dominant and a subdominant pair states have the only non-zero Boltzmann weights. The phase transition critical exponents quickly saturate to the high q value.