Finite Order Invariants of Legendrian, Transverse, and Framed Knots in Contact 3-manifolds (http://xxx.lanl.gov/abs/math.SG/9907118) Author: Vladimir Tchernov July 20, 1999, updated Aug 9, 1999. Comments: 34 pages, 8 figures. Subj-class: Symplectic Geometry; Geometric Topology MSC-class: 53C15, 57M99 (Primary), 53C42 (Secondary) Recently D. Fuchs and S. Tabachnikov proved that the quotients of the groups of $C$-valued order $\leq n$ invariants by the groups of order $\leq (n-1)$ invariants of Legendrian, of transverse, and of framed knots in the standard contact $ R^3$ are canonically isomorphic. An analogous result was obtained by J. W. Hill in the case of Legendrian and of framed knots in the spherical cotangent bundle of $ R^2$ (with the standard contact structure). The proofs of these facts were based on the fact of the existence of the universal Vassiliev invariant of framed knots in these spaces. We show that for a big class of contact manifolds the groups of order leq n$ $\invariants (with values in an arbitrary Abelian group) of Legendrian, of transverse and of framed knots are canonically isomorphic. On the other hand for an arbitrary cooriented contact structure on $S^1\times S^2$ with the nonzero Euler class of the contact bundle we construct examples of Legendrian homotopic Legendrian knots $K_1$ and $K_2$ such that they realize isotopic framed knots but can be distinguished by finite order invariants of Legendrian knots in $S^1\times S^2$. We construct similar examples for a big class of contact manifolds $M$ such that $M$ is a total space of a locally trivial $S^1$-fibration over a nonorientable surface. We show that in some of these examples the complements of $K_1$ and of $K_2$ are overtwisted. Update (Aug 9, 1999): We added many new examples of Legendrian homotopic Legendrian knots that realize isotopic framed knots but are distinguishable by finite order invariants of Legendrian knots. In some of these examples the complements of both Legendrian knots are overtwisted. We also extended Theorem 3.0.6 to the case of $S^1$-fibrations over nonorientable surfaces and corrected typos.