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We study the influence of relativity on the chaotic properties and dynamical outcomes of an unstable triple system; the Pythagorean three-body problem. To this end, we extend the brutus N-body code to include post-Newtonian pairwise terms up to 2.5 order, and the first order Taylor expansion to the Einstein-Infeld-Hoffmann equations of motion. The degree to which our system is relativistic depends on the scaling of the total mass (the unit size was 1 parsec). Using the brutus method of convergence, we test for time-reversibility in the conservative regime, and demonstrate that we are able to obtain definitive solutions to the relativistic three-body problem. It is also confirmed that the minimal required numerical accuracy for a successful time-reversibility test correlates with the amplification factor of an initial perturbation, as was found previously for the Newtonian case. When we take into account dissipative effects through gravitational wave emission, we find that the duration of the resonance, and the amount of exponential growth of small perturbations depend on the mass scaling. For a unit mass ≤ 10 M⊙, the system behavior is indistinguishable from Newton's equations of motion, and the resonance always ends in a binary and one escaping body. For a mass scaling up to 107 M⊙, relativity gradually becomes more prominent, but the majority of the systems still dissolve in a single body and an isolated binary. The first mergers start to appear for a mass of ~ 105 M⊙, and between 107 M⊙ and 109 M⊙ all systems end prematurely in a merger. These mergers are preceded by a gravitational wave driven in-spiral. For a mass scaling ≥ 109 M⊙, all systems result in a gravitational wave merger upon the first close encounter. Relativistic three-body encounters thus provide an efficient pathway for resolving the final parsec problem. The onset of mergers at the characteristic mass scale of 107 M⊙ potentially leaves an imprint in the mass function of supermassive black holes. [ABSTRACT FROM AUTHOR]