𝔖 Bobbio Scriptorium
✦   LIBER   ✦

A note on “Rigid body motion from depth and optical flows”

✍ Scribed by Robert M. Haralick; Xinhua Zhuang


Publisher
Elsevier Science
Year
1986
Weight
81 KB
Volume
34
Category
Article
ISSN
0734-189X

No coin nor oath required. For personal study only.

✦ Synopsis


This paper investigates the basic properties of the class of neighborhood-uniform node label controlled (NUNLC) graph grammars. The class of NUNLC grammars is distinguished by requiring a very natural restriction on the connection relations of NLC grammars. The restriction implies the "Church-Rosser property" of derivations in an NUNLC grammar, which makes the class of NUNLC grammars " technically easier" to investigate. A number of combinatorial properties of the languages generated by the class of NUNLC grammars are proved. Also, it is demonstrated that a number of basic properties are decidable for the class of NUNLC grammar-many of them are undecidable in the whole class of NLC grammars.


📜 SIMILAR VOLUMES


Sources and observers in motion, II: Aco
✍ S.E. Wright; D.J. Lee 📂 Article 📅 1986 🏛 Elsevier Science 🌐 English ⚖ 388 KB

The theory in reference [1], for a source in rectilinear motion, using time variant analysis and an invariant surface flux source description, is extended here to include arbitrary source motion. The special case of a small rigid object is considered, with motion in a circle used as a simple example

On the existence of steady flows of a Na
✍ Ana Leonor Silvestre 📂 Article 📅 2004 🏛 John Wiley and Sons 🌐 English ⚖ 124 KB

## Abstract We prove the existence of a strong solution to the three‐dimensional steady Navier–Stokes equations in the exterior of an obstacle undergoing a rigid motion. Unlike the classical exterior problem for the Navier–Stokes equations, that only takes into account the translational motion of t

A comparison between a collocation and w
✍ G. D'Avino; M. A. Hulsen 📂 Article 📅 2009 🏛 John Wiley and Sons 🌐 English ⚖ 880 KB

## Abstract In this work, we implemented and compared two different methods to impose the rigid‐body motion constraint on a solid particle moving inside a fluid. We consider a fictitious domain method to easily manage the particle motion. As the solid as well as the fluid inertia are neglected, the