In this work, we reported a ubiquitous presence of topological Floquet time crystal (TFTC) in one-dimensional periodically-driven systems. The rigidity and realization of spontaneous discrete time-translation symmetry (DTS) breaking in our TFTC model require necessarily coexistence of anomalous topological invariants, instead of the presence of disorders or manybody localization. We found that in a particular frequency range of the underlying drive, the anomalous Floquet phase coexistence between topological 0 and π modes can produce the period-doubling (2T, two cycles of the drive) that breaks the DTS spontaneously, leading to the subharmonic response (ω/2, half the drive frequency). The rigid period-2T oscillation is topologically-protected against perturbations due to both non-trivially opening of 0-and πgaps in the quasienergy spectrum, thus, as a result, can be viewed as a specific "Rabi oscillation" between two Floquet eigenstates with certain quasienergy splitting π/T . Our modeling of the time-crystalline 'ground state' can be easily realized in experimental platforms such as topological photonics and ultracold fields. Also, our work can bring significant interests to explore topological phase transition in Floquet systems and to bridge a profound connection between Floquet topological insulators and photonics and period-doubled time crystals.