The lack of terahertz (THz) components and strong THz diffraction limit greatly THz wavefront-phase manipulation. This paper introduces a universal and versatile THz wavefront-phase manipulation mechanism through a double Pancharatnam-Berry (PB) phase-based dislocation scheme at near-infrared (NIR) region, avoiding the need of THz components while mitigating effectively the adverse effect of THz diffraction. The mechanism bases on an innovative NIR light-field manipulation mechanism enabling independent controls of two wavefront-phases by two-dimensional (2D) dislocations of two phase-plates with conjugated phase functions. Independence is ensured as long as the partial derivatives of the target phase pair with respect to the spatial variables are equal—a condition satisfied by numerous important phase pairs, such as logarithmic-axicon versus vortex phases (for Bessel and vortex beams) and one-dimensional (1D) versus 2D cubic phases (for 1D and 2D Airy beams). Notably, for only one target wavefront, it is applicable to any kinds of phases. To realize the NIR manipulation, a novel dislocation scheme is further designed with two PB plates as the conjugated phase-plates, which not only enables the NIR manipulation but also produces a pair of collinear pulses with conjugated modulated phases and orthogonal polarizations. By using the pulse pair as the pumps, the dislocation scheme can transfer the wavefront-phase manipulation from NIR to THz region by type-II difference frequency generation. Finally, a proof-of-principle experiment successfully presents the flexible realization of this dislocation scheme for multiple wavefront-phase manipulation at NIR and exhibits its ability to dynamically generate and control THz vortex, Bessel, and vortex-Bessel fields with adjustable topological charge and “diffraction-free” propagation distances. This work offers a flexibly way for universal and versatile manipulation, especially where direct phase manipulation is practically restricted, especially in THz region.