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Tangent vector

To specify the directions of two different vectors at nearby points it is necessary to define tangent vectors (tangent space) at these points. Important... [Pg.162]

This derivative is the unit vector tangent to the curve defined by a succession of points r at the point r, and hence it must give the direction of the vector Vp(r) at this point. Thus... [Pg.24]

Figure 1 The Gauss map g between a surface E around a point P of position vector r and the unit sphere Si. Q ow Si corresponds to P on Z. The vector tangent plane n is the same. dQ transforms dL into dS = dG dT), changing its shape and area. Figure 1 The Gauss map g between a surface E around a point P of position vector r and the unit sphere Si. Q ow Si corresponds to P on Z. The vector tangent plane n is the same. dQ transforms dL into dS = dG dT), changing its shape and area.
PFR. The reaction rate at constant density is a vector tangent to the trajectory of component concentration, because the length variation can be translated in time. [Pg.342]

Here, t is the vector tangent to the CSTR locus, as defined in Chapter 6. [Pg.222]

Rate vectors tangent to H(n, b), satisfying the condition n r(C) = 0. Points that satisfy this condition may or may not be achievable. [Pg.263]

Substituting - fii Vx, for qu where /t, is a 4D vector tangent to the surface of the 4D hypersphere at X having a modulus equal to the dipole moment fii of particle i, the dipole-dipole potential gives [20-22]... [Pg.170]

By varying e, we obtain a set of planes, each tangent to a two-dimensional sphere of one and the same radius. Therefore, the two vectors K, e, which satisfy the above equations, define uniquely a certain vector tangent to a two- dimensional sphere. This precisely proves the lemma since the bundle tangent to a sphere is defined as a four-dimensional manifold whose points are pairs of the form (e, ), where e is a point on the sphere, and ( is an arbitrary vector tangent to the sphere at the point e. [Pg.35]

Here t is any vector tangent to the interface and it follows that the potentials on either side of the interface differ by at most a constant. If no work is done in transferring charge across the interface, the constant is zero. [Pg.29]

Unit tangent vector Tangent surface vector... [Pg.1583]

For the continuous curve the angular correlation is related to the relative orientation between the unit vector tangent tt> die curve... [Pg.234]


See other pages where Tangent vector is mentioned: [Pg.98]    [Pg.37]    [Pg.171]    [Pg.206]    [Pg.59]    [Pg.149]    [Pg.75]    [Pg.69]    [Pg.1]    [Pg.255]    [Pg.564]    [Pg.186]    [Pg.416]    [Pg.2192]    [Pg.127]    [Pg.1132]    [Pg.416]    [Pg.59]    [Pg.2176]    [Pg.114]    [Pg.914]    [Pg.192]    [Pg.244]    [Pg.316]    [Pg.170]    [Pg.119]    [Pg.791]    [Pg.914]    [Pg.170]    [Pg.6027]    [Pg.9121]    [Pg.2461]    [Pg.257]    [Pg.634]    [Pg.364]    [Pg.31]    [Pg.1368]    [Pg.12]    [Pg.1416]   
See also in sourсe #XX -- [ Pg.162 ]




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Correlation function of the tangent vectors

Tangent

Tangent, unit vector

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