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CURVE BOUNDED SURFACE

Barrett [50] has interestingly reviewed and compared the properties of the Abelian and non-Abelian Stokes theorems, a review and comparison that makes it clear that the Abelian and non-Abelian Stokes theorems must not be confused [83,95]. The Abelian, or original, Stokes theorem states that if A(x) is a vector field, S is an open, orientable surface, C is the closed curve bounding S, dl is a line element of C, n is the normal to S, and C is traversed in a right-handed (positive direction) relative to n, then the line integral of A is equal to the surface integral over 5 of V x A-n ... [Pg.97]

Fig. 10. Sensitivity evaluation of SPFS on planar surfaces. (1), (2), (3) are fluorescence kinetic curves of the binding of L2F5 to surfaces of different biotin densities of % — 0.0004, 0.0001, 0, respectively. (4), (5), (6) are fluorescence kinetic curves of the binding of AF-RaM to 2F5 (mouse IgG) bound surfaces of different X = 0.0004, 0.0001, 0, respectively. Fig. 10. Sensitivity evaluation of SPFS on planar surfaces. (1), (2), (3) are fluorescence kinetic curves of the binding of L2F5 to surfaces of different biotin densities of % — 0.0004, 0.0001, 0, respectively. (4), (5), (6) are fluorescence kinetic curves of the binding of AF-RaM to 2F5 (mouse IgG) bound surfaces of different X = 0.0004, 0.0001, 0, respectively.
Let AB (Fig. 100) be any curve whose equation is known. It q B is required to find the area of the portion bounded by the curve the two coordinates PM, QN and that portion of the a>axis, MN, included between the ordinates at the extremities of that portion of the curve under investigation. The area can be approximately determined by supposing PQMN to be cut up into small strips—called surface elements— perpendicular to the ic-axis finding the area of each separate strip on the assumption that the curve bounding one end of the strip is a straight Univ Calif - Digitized by Microsoft ... [Pg.230]

The principle of the pump-probe observation scheme is plotted in Fig. 1. The clusters are excited from a low vibrational level of the electronic ground state to an excited state. Due to the spectral width of the employed fs-pump pulse, a coherent superposition of several vibrational states is created, which leads to the formation of an evolving wave packet. If a bound electronic state is excited [Fig. 1(a)], this wave packet will oscillate between the inner and outer turning point of the potential energy curve or surface, reflecting the vibrational motion of the excited molecule. The temporal evolution of this... [Pg.159]

Engineers modify free form curves and surfaces interactively. Connector constraints join curves into more complex curves. Modification of a curve or a connecting point causes modification of all attached curves to save the connector constraints. This action also modifies the surfaces bounded by the modified curves. [Pg.110]

A simple closed curve T in space, with a projection on the z = 0 plane that forms a simple closed curve, has surfaces bounded by F that can be written in the form... [Pg.200]

The most interesting behavior, however, is observed when the parameters are located between the solid and dashed curves. Here, the behavior of the sample significantly depends on whether it is confined the sample oscillates when it is free and remains in the stationary state when it is attached to the bounding surfaces. [Pg.71]

The optional curves on-Surfaces correspond to the bounding parameter values. They are the best available approximations. The receiving system will have to check whether they can be used immediately or whether they have to be enhanced. [Pg.90]

The interior of the bounded surface is defined to be n t from any point on the boundary, where n is the surface normal and t the boundary curve tangent vector at this point. The region so defined must be simply connected. [Pg.92]

Let S be an open, two-sided surface bounded by a curve C, then the line integral of vector A (ciiiwe C is traversed in the positive direction) is expressed as... [Pg.257]

Let the mid-surface of the Kirchhoff-Love plate occupy a domain flc = fl Tc, where C is a bounded domain with the smooth boundary T, and Tc is the smooth curve without self-intersections recumbent in fl (see Fig.3.4). The mid-surface of the plate is in the plane z = 0. Coordinate system (xi,X2,z) is assumed to be Descartes and orthogonal, x = xi,X2)-... [Pg.219]

Let C be a bounded domain with the smooth boundary L, which has an inside smooth curve Lc without self-intersections. We denote flc = fl Tc. Let n = (ni,ri2) be a unit normal vector at L, and n = ( 1,1 2) be a unit normal vector at Lc, which defines a positive and a negative surface of the crack. We assume that there exists a closed continuation S of Lc dividing fl into two domains the domain fl with the outside normal n at S, and the domain 12+ with the outside normal —n at S (see Section 1.4). By doing so, for a smooth function w in flc, we define the traces of w at boundaries 912+ and, in particular, the traces w+ and the jump [w] = w+ — w at Lc. Let us consider the bilinear form... [Pg.234]

The rotor of the vane pump is mounted off centre in a cylindrical casing (Figure 8.9). It carries rectangular vanes in a series of slots arranged at intervals round the curved surface of the rotor. The vanes are thrown outwards by centrifugal action and the fluid is carried in the spaces bounded by adjacent vanes, the rotor, and the casing. Most of the wear is on the vanes and these can readily be replaced. [Pg.324]

Fig. 10. Concentration curves fitted by exponential regression for the reaction of l,2,4,5r tetrabromobenzene (A) with surface bound chloride, a consecutive four-stage reaction with three intermediates (B,C,D) and the product E. Fig. 10. Concentration curves fitted by exponential regression for the reaction of l,2,4,5r tetrabromobenzene (A) with surface bound chloride, a consecutive four-stage reaction with three intermediates (B,C,D) and the product E.
Stuart and Hlady [37] found that unintentional lateral forces influenced their measurements of adhesion between surface-bound protein molecules and colloid probe-bound ligands. They noted a greatly exaggerated separation distance and a stick-shp behavior in their adhesion curves, which they attribute to roUiug and buckling of the cantilever under the influence of lateral forces as the sample was retracted with the probe stuck to it. [Pg.31]

Temperature programmed reaction spectra depicting the reaction of H2O and OH groups with oxygen on Pd(lOO) are shown in fig. 3. Curve (a) was obtained for H2O adsorption on the clean surface and contains two peaks, the state at 167 K of multilayer H2O, and the <>2 state at 182 K due to H2O bound directly to the surface /7/. An additional state at 255 K, labelled y, is observed following coadsorption of 1 0 and 0 (fig. 3b). This state represents the reaction of OH groups III... [Pg.170]


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See also in sourсe #XX -- [ Pg.2 , Pg.9 , Pg.91 ]




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Curved surface

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