In an accelerated system, objects attached to a rope share the same acceleration, but the tensions in the rope vary based on the mass being accelerated. The discussion highlights that without specific mass values, assuming equal masses leads to the conclusion that the tensions are not equal. Tension FT3 only needs to accelerate the third mass, while FT2 must accelerate both the second and third masses, and FT1 has to account for all attached masses. This results in different tension values throughout the system. Understanding these dynamics is crucial for solving problems related to tension in accelerated systems.