By G. Albrecht (auth.), Prof. Dr. Gerald Farin, Dr. Hanspeter Bieri, Dr. Guido Brunnett, Dr. Tony De Rose (eds.)
19 papers provided through overseas specialists supply a state of the art survey of the appropriate difficulties and matters in modeling, CAD/CAM, medical visualization, and computational geometry. the subsequent themes are taken care of: • floor layout and fairing • subdivision schemes • variational layout • NURBS • opposite engineering • physically-based modelling • scientific imaging
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Additional resources for Geometric Modelling: Dagstuhl 1996
E. in! P (open halfspace), bnd P (hyperplane), and ext P (open halfspace) . • For any other Nef polyhedron P, the sets px can be determined uniquely by applying (repeatedly, in general) the following rules: (clos Pf := clos PX, (PI Il P2f := Pill Pl , and analogously for the other Boolean set operations. e. a (Nef) pyramid. px is called the pyramid locally adjoined to P in x, or just locally adjoined pyramid. Let A £; lRd have the property that px = pY for all x, YEA. In this case, we sometimes denote the locally adjoined pyramid common to all points in A by pA.
Bloor and M. 1. Wilson Figure 3. Aircraft wing, X W (u w , vw ) Figure 4. Engine nacelle, XN(un , Vn) a boundary-representation of a valid solid object. To remove the redundant sections one must effectively reparametrise the wing and nacelle surfaces in the regions around the contours. In the case of the wing, this reparametrisation is carried out as described below; the reparametrisation of the nacelle surface is carried out in an exactly anala- The Shape Parametrisation of an Aircraft Engine Nacelle and Pylon 47 gous manner.
1) which satisfies these boundary conditions, and which represents the the wing, is given by XW (u ... , vw ). The nacelle is generated by solving Eq. (rln) sin(f3) + (rni) sin(Vn) cos(f3) ) ync + (rni) cos(Vn ) -! (rln) sin(f3) + (rne) sin( Vn ) cos(f3) ) znc XN (1,V n ) = ( 43 (7) n) ync+ (rne)cos(v n ) znc +! (rln) cos(f3) - (rne) sin(vn ) sin(f3) (8) (sni) sin(f3) - (slni) (sni) sin(vn ) COS(f3)) X~ (0, Vn ) = ( -(slni)(sni) COS(Vn ) (9) (sni) cos(f3) + (slni)(sni) sin( vn ) sin(f3) N Xu (sne) sin(f3) ) 0 ( (1, Vn) = (10) (sne) cos(f3) We will assume that the solution to Eq.