Strong dipole−dipole interactions in mesogenfree aliphatic comblike polymers can induce unique liquid crystalline (LC) self-assembly. By comparing atactic and isotactic poly(oxypropylene)s with n-alkylsulfonyl side groups (aPOP-SO 2 C n and iPOP-SO 2 C n ), the effect of main-chain tacticity on the ordered phase behavior was studied in this work. For aPOP-SO 2 C n , LC self-assemblies were observed when n is ≥3. Two types of LC phases were formed depending on the side chain length n: (i) a three-dimensional (3D) high-order LC structure (possibly crystal B or E) for n = 3−5 and (ii) a smectic A (SmA) structure for n = 6−12. For iPOP-SO 2 C n , crystallization was favored as a result of regular mainchain configuration. Only when n ≥ 10, the isotactic comblike polymers exhibited a monotropic phase behavior with the SmA phase appearing during cooling from the isotropic melt. Regardless of atactic or isotactic main chains, these ordered LC and crystalline phases featured a double-layer structure, which was dictated by the optimal dipole−dipole interaction distance (i.e., 0.40−0.44 nm) between sulfonyl groups in the neighboring side chains. This study showed that the chiral centers incorporated in the backbone could not induce chiral smectic self-assembly for the isotactic polymers. As such, we are currently implementing chiral centers in the side chains for the formation of ferroelectric structures for these mesogen-free aliphatic LC polymers.