Body-Pin Rigidity

4. Vertex deletion and self-stress🔗

Section 2.2 of Zheng (2026) measures what deleting one vertex does to the self-stress space, over a coefficient field that shrinks with the graph. The measurement is the step of the induction that proves the stress–codimension inequality s + \operatorname{trdeg}_k K \le 3|V|: each step deletes a vertex v of degree at most three, and equation (2.6) below expresses the resulting change in s + \operatorname{trdeg}_k K - 3|V| through two local numbers, a kernel dimension u and a transcendence degree \delta_v, both defined in this chapter.

We follow the paper's order. An exact sequence relates the self-stress space of F to that of H = F - v; the tower formula for transcendence degree does the same for the coordinate fields; and a local classification, Lemma 2.3, shows that u + \delta_v \le 3 whenever \deg_F(v) \le 3, except in one case: a degree-three vertex whose three neighbours are collinear. The last two lemmas of the chapter show that in this exceptional case the three rigidity rows on pairs of neighbours already lie in the row space of the deleted graph; in the flags chapter the case is retained as a collinearity flag and carried through the remaining steps of the induction.

  1. 4.1. Direction rows over a coefficient field
  2. 4.2. Deleting one vertex
  3. 4.3. Certified response edges
  4. 4.4. The local classification
  5. 4.5. Descent and the three neighbour rows
  6. 4.6. Base change and field towers