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Circle through three points

The general equation of a circle through three points (a, bi), (02/ 2)/ and (03/ 3) (provided three points do not fall on a straight line) can be given as... [Pg.33]

For each porosity, there is a particular yield locus, a family of three 3deld loci is shown in Figure 12.38. Many experiments [72] have established that the envelope of the Mohr circles through the points Ei that lead to steady state flow for different porosities is, to a veiy close... [Pg.599]

The fabric design (weaving pattern, fibre density, etc.) is determinant for the POF bend. The radius of fibre curvature in the fabric is expressed by the radius of the circle that passes through three points, X, Y and Z, that are shown in Figure 8.8. [Pg.183]

From the definition of a particle used in this book, it follows that the motion of the surrounding continuous phase is inherently three-dimensional. An important class of particle flows possesses axial symmetry. For axisymmetric flows of incompressible fluids, we define a stream function, ij/, called Stokes s stream function. The value of Imj/ at any point is the volumetric flow rate of fluid crossing any continuous surface whose outer boundary is a circle centered on the axis of symmetry and passing through the point in question. Clearly ij/ = 0 on the axis of symmetry. Stream surfaces are surfaces of constant ij/ and are parallel to the velocity vector, u, at every point. The intersection of a stream surface with a plane containing the axis of symmetry may be referred to as a streamline. The velocity components, and Uq, are related to ij/ in spherical-polar coordinates by... [Pg.6]

Exercise 10.17 Suppose pr, p2 and pi are points on the unit sphere in that do not lie on one common great circle. (A great circle is the intersection of the unit sphere with a plane through the origin in ) Show that every point p on the sphere is uniquely defined by its distances from the three points pi, P2, p3. Interpret great circles in PCC ) physically i.e., give a definition in terms of experiments and probabilities. [Pg.337]

A geometric analogue of this puts the new e-vertex on the circle whose curvature is the mean of circles through left and right groups of three points. (The curvature can be defined as a vector and so this is well-defined for curves in three-dimensional space.) If four points happened to lie on a circle initially, the mean would give the same circle and so the new point would lie on it too. If all the initial points lay on the same circle, then the limit curve could never leave that circle. [Pg.162]

Figure 25 Phase diagram for the 2 4-solute-solvent system in three dimensions. The open circles are the data obtained from Monte Carlo simulations (a thin line is drawn through these points). The dashed lines are the tie-lines from the simulations. The quasi-chemical results are shown by the solid lines. (From Ref 25.)... Figure 25 Phase diagram for the 2 4-solute-solvent system in three dimensions. The open circles are the data obtained from Monte Carlo simulations (a thin line is drawn through these points). The dashed lines are the tie-lines from the simulations. The quasi-chemical results are shown by the solid lines. (From Ref 25.)...
Fig. 5.13. A two-dimensional illustration of Miller indices and Bragg planes planes are in fact lines. Larger open circles denote lattice points, smaller black dots indicate the midpoint of the a periodicity. Planes (11) (heavy dashed lines) pass through the points (a.O) and (0,b), planes (21) (continuous lines) pass through the points (a/2,0) and (0,b). The <<21 spacing is less than the 1 spacing. The (11) and (21) lines are the traces of the (110) and (210) planes in the three-dimensional equivalent. Fig. 5.13. A two-dimensional illustration of Miller indices and Bragg planes planes are in fact lines. Larger open circles denote lattice points, smaller black dots indicate the midpoint of the a periodicity. Planes (11) (heavy dashed lines) pass through the points (a.O) and (0,b), planes (21) (continuous lines) pass through the points (a/2,0) and (0,b). The <<21 spacing is less than the 1 spacing. The (11) and (21) lines are the traces of the (110) and (210) planes in the three-dimensional equivalent.
The diagram in Figure 3-2 illustrates the triangulation method, which makes it possible to later pinpoint the exact location of an object. In this accident, the victim contacted a high-voltage line with a metal tree-trimming pole. The position of the victim s head is measured from three points. Notice the small circles with horizontal lines through them. These circles indicate where photos were taken. Also, directional north is indicated and all major objects are identified. [Pg.35]

Fig. 1. Ideal surface (100) plane of alumina after Peri [25]. (A) Top layer viewed per-pendicualrly to the plane (B) section through the three top layers, (a) Fully hydrated surface, (b) dehydroxylated surface. Open circles denote oxygen, filled circles hydroxyl, small black points aluminium,... Fig. 1. Ideal surface (100) plane of alumina after Peri [25]. (A) Top layer viewed per-pendicualrly to the plane (B) section through the three top layers, (a) Fully hydrated surface, (b) dehydroxylated surface. Open circles denote oxygen, filled circles hydroxyl, small black points aluminium,...
Fig. 6.2. Comparison of measured three-body y moments with theory (heavy curve) for hydrogen and the fundamental band y 3) dots and circles from [187] the thin line is a visual average through the experimental points [295]. Fig. 6.2. Comparison of measured three-body y moments with theory (heavy curve) for hydrogen and the fundamental band y 3) dots and circles from [187] the thin line is a visual average through the experimental points [295].
Figure 20. Structure of [Cu(4,4 -bipy)X], X is Cl, Br, or I. Circles represent Cu. Each short connection shown here is provided by two p2 X bridges. Long connections are provided by bipy, some of which are present in close side-by-side pairs. The 3-connecting nodes of the (6,3) net are located at the mid-points of the Cu(X)2Cu 4-gons i.e. at the mid-points of the short connections shown here. A 6-gon of one horizontal sheet is shown here in heavy black and three independent inclined nets are seen passing through it, a central one represented by fine lines and a front and a back one by open connections. Figure 20. Structure of [Cu(4,4 -bipy)X], X is Cl, Br, or I. Circles represent Cu. Each short connection shown here is provided by two p2 X bridges. Long connections are provided by bipy, some of which are present in close side-by-side pairs. The 3-connecting nodes of the (6,3) net are located at the mid-points of the Cu(X)2Cu 4-gons i.e. at the mid-points of the short connections shown here. A 6-gon of one horizontal sheet is shown here in heavy black and three independent inclined nets are seen passing through it, a central one represented by fine lines and a front and a back one by open connections.

See other pages where Circle through three points is mentioned: [Pg.33]    [Pg.33]    [Pg.421]    [Pg.162]    [Pg.421]    [Pg.180]    [Pg.149]    [Pg.30]    [Pg.76]    [Pg.171]    [Pg.120]    [Pg.28]    [Pg.102]    [Pg.39]    [Pg.223]    [Pg.240]    [Pg.90]    [Pg.1717]    [Pg.275]    [Pg.39]    [Pg.597]    [Pg.44]    [Pg.223]    [Pg.411]    [Pg.85]    [Pg.294]    [Pg.174]    [Pg.243]    [Pg.1035]    [Pg.1093]    [Pg.1100]    [Pg.508]    [Pg.344]    [Pg.59]    [Pg.275]    [Pg.329]   
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