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Euler formula for

Every connected component Cj is incident to two faces Fi and jFJ+i (mod 0 along cycles of length k and which are the numbers of (5,3)-polycycles Fi in those cycles. The Euler formula for the plane graph C,- reads ... [Pg.215]

Recall first the Euler formula for the p-vector of a 3-valent plane graph (see Theorem 1.2.3) ... [Pg.288]

A contour plot is shown in Fig. 7.8. Note that this function is cylindrically-symmetrical about the z-axis with a node in the x, y-plane. The eigenfunctions 21 1 are complex and not as easy to represent graphically. Their angular dependence is that of the spherical harmonics 7i i, shown in Fig. 6.4. As deduced in Section 4.2, any linear combination of degenerate eigenfunctions is an equally-valid alternative eigenfunction. Making use of the Euler formulas for sine and cosine,... [Pg.58]

Almost any divalent polyhedron, spherical, toroidal, or of higher genus, is at least conceivably a candidate for an sp carbon framework if reasonable bond lengths and angles can be achieved, and so there has naturally been some discussion in the literature of extended definitions of fullerenes (e.g.. Refs. 8-17). Exotic topologies are dealt with elsewhere in the present volume in the chapters by Kirby and Klein, but even within the class of pseudospherical polyhedra other face sizes are possible. The Euler formula for an n-vertex divalent spherical polyhedron is... [Pg.238]

In Table I we list a few examples of the geometrical correspondence which prevails between closo boron hydrides and the carbon fiillerenes [3]. The geometrical structure of Buckminsterflillerene maps into that of the 32-vertex closo boron hydride, B32H32. Both molecules of symmetry Ih display correspondence of the geometrical centers of the 32 carbon (polygon) faces to the 32 boron vertices, the 60 boron faces to the 60 carbon vertices, and the 90 carbon contacts to the 90 boron contacts. In accordance with the Descartes-Euler formula, for both molecules the sum of the vertices and faces exceeds by 2 the number of contacts. A cursory review of Table I indicates that similar correspondences prevail for all the examples listed. Clearly the list of examples may be readily extended. [Pg.86]

The combination of Eqs. (5.57) and (5.59) gives the explicit Euler formula for integrating differential equations... [Pg.284]

The Euler characteristic for a surface built of polygons is much more conveniently calculated according to the Euler formula [33]... [Pg.701]

Combining this with Euler s theorem we obtain 3N—S 6, or S = 3N—6, our formula for determinate structures in 3-dimensions. [Pg.53]

This relation can be easily verified by employing the Euler formula c = cos 6 i sin 0 for the pure imaginary part of the exponential function and by observing the definite integrals ... [Pg.109]

Let G be a finite group acting on a compact differentiable manifold X. Then there exists the well known formula for the Euler number of the quotient... [Pg.54]

A k-valent sphere, whose faces have gonality a orb, is called a ( a, b), k)-sphere (see Chapter 2). We call the parameters ( a, b), k) elliptic, parabolic, hyperbolic, according to the sign cfa(2, b, k). This sign has a consequence for the finiteness and growth of the number of graphs in the class of ( a, b], k)-spheres. Here, the link is provided by the Euler formula (1.1). [Pg.17]

We can interpret the quantity 2k — b(k — 2) as the curvature of the faces of gonality b Euler formula is the condition that the total curvature is a constant, equal to 4k, for fc-valent plane graphs. This curvature has an interpretation and applications in Computational Group Theory, see [Par06] and [LySc77, Chapter 9]. [Pg.24]

This formula is called Gauss-Bonnet formula (see [Ale50]). Expressed differently, Euler formula v — e + / = 2 is for plane graphs with no boundaries, but it can be extended to plane graphs with boundaries. [Pg.118]

We classify only the strictly face-regular spheres and strictly face-regular normal balanced planes. The plane case contains the toms case as a subcase. For the plane, the Euler formula does not hold, but the condition of normality, discussed thereafter,... [Pg.125]

Assume b < 11. Given a ( 5, b], 3)-plane, the gonality of a face in the major skeleton is equal to the number of (5,3)-polycycles E and C3 to which it is incident. Clearly, there are at most five such incidences for each face. Since the major skeleton is 3-valent, we reach a contradiction by Euler formula (1.1) and (i) holds. [Pg.220]

EulerS modified Arrhenius s formula for a mixture, tj A B C. . ., assuming incomplete ionisation, and represented the viscosity of a salt solution by ... [Pg.122]

From these the nodal properties of the transition densities may be derived. They are shown in Figure 2.12c for all four states considered. Use was made of the fact that and 4> j are degenerate, so the real linear combinations (4 i-2 + I -i-.-2yV2 and - 4>, j)/(iV5) can be employed instead. The transition densities between the ground state 4>v and these excited states are then obtained by means of the Euler formulae cos z = (e + e )/2 and sin z = (e - e" )/(2i) as... [Pg.81]


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See also in sourсe #XX -- [ Pg.10 , Pg.46 ]




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