Can you characterize the group of transformations of knot diagrams which preserve the knot embedding? Suppose we call a knot an equivalence class of embeddings of S1 --> R3 under ambient isotopy, a knot representative a particular such embedding, and a knot diagram the "2 1/2 dimensional" shadow of such a knot representative on S2 from a particular vantage point P, i.e. the light source for the shadow is at P, and the "2 1/2" means that the over and under information is shown.
My question involves how the set of knot diagrams of a particular fixed knot representative vary as P, the viewpoint varies.  We know about the Reidemeister rules, which generate a group of transformations of knot diagrams in a way such that the underlying knot remains invariant under changes of both ambient isotopy and projection.   Intuitively there is also a smaller group of pure "projective" transformations of knot diagrams under which any fixed knot representative remains invariant.   Assuming that, what are the relations between these two groups of transformations of knot diagrams?
 A: I remember attending a talk by Barbara Jablonska at Knots in Washington (2009) in which she studied a knot in a geometric, rigid fashion.  As the direction of projection varies over $S^2$, she obtained interesting surfaces by looking at the locus of a particular crossing (if memory serves).  Here's an abstract of the talk, but I cannot find anything published.
http://atlas-conferences.com/c/a/x/q/18.htm
A: As Daniel Moskovich points out, you don't get a different set of moves on (isotopy classes of) planar diagrams.
More specifically, given diagrams $D_1$ and $D_2$ which differ by a (any) single Reidemeister move, one can find isotopic diagrams $D'_1$ and $D'_2$ such that $D'_1$ and $D'_2$ are both projections (shadows) of the same fixed knot $K$ in $R^3$.
The only way I see to rescue your question is to not take isotopy classes of knot diagrams in $R^2$ -- just consider "moves" form one rigid diagram to another.  But this seems to be a difficult question even for diagrams without any crossings.
A: If you consider knots made of piecewise linear segments, then one can say a couple of things. First, crossings will be between various segments, and for any pair of segments, one could compute the possible projections for any given direction. This will give a quadrilateral of projection directions where the segments cross. If you're interested in generic projections, then one could compute the non-generic phenomena. A Reidemeister 3 move occurs when there's a triple of segments which project to a triple crossing. The set of lines through 3 skew segments forms part of a hyperbolic paraboloid or hyperboloid. So the Gauss image will be part of a quadratic curve in $S^2$. There are some other possible non-generic phenomena, such as the planes containing adjacent segments, or vertices and segments (the boundaries of the quadrilaterals). In any case, once you've computed these, $S^2$ gets partitioned up into regions in which a generic projection occurs, and in principle one could compute each projection for each region. In fact, this is one way to prove that the Reidemeister moves suffice for PL equivalence of knots.  
