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Reference triangle

The trigonometric functions of angles are the ratios between the various sides of the reference triangles shown in Fig. 3-39 for the various quadrants. Clearly r = /x + y > 0. The fundamental functions (see Figs. 3-40, 3-41, 3-42) are... [Pg.438]

By the same procedure barycentric coordinates can be set up in the plane of a reference triangle Ai A2A3. If p -bp +P 0 masses p, p, p at the three vertices determine a point P (the centroid) with coordinates (P,P,P). [Pg.59]

Figure 11. Local density pt) (with rt = 1.78 Figure 11. Local density pt) (with rt = 1.78 <tlj) vs. bulk density for the SCF shown in Fig. 1 (triangles) with bulk density for reference (dashes). Computed vibrational relaxation rates for a diatomic solute in this same SCF (circles) with no-local-density-enhancement rates for reference (triangles), see text. Reprinted with permission from Ref. [12]. Copyright 1999 American Institute of Physics.
The ADT matrix for the lowest two electronic states of H3 has recently been obtained [55]. These states display a conical intersection at equilateral triangle geometi ies, but the GP effect can be easily built into the treatment of the reactive scattering equations. Since, for two electronic states, there is only one nonzero first-derivative coupling vector, w5 2 (Rl), we will refer to it in the rest of this... [Pg.197]

The dotted line in Fig. 11,17, 2 refers to the modification of the apparatus for use in fractional distillation under reduced pressure a Perkin triangle or equivalent receiver device ( vacuum distilling adapter ) is generally employed for collection of the various fractions. [Pg.98]

With reference to Fig. 18-81 (both graphs), EF represents the locus of overflow compositions for the case in which the overflow stream contains no inert sohds. E F represents the overflow streams containing some inert sohds, either by entrainment or by partial solubihty in the overflow solution. Lines GF, GL, and GM represent the loci of underflow compositions for the three different conditions indicated on the diagram. In Fig. 18-81 7, the constant underflow line GM is par-aUel to EF, the hypotenuse of the triangle, whereas GF passes through... [Pg.1676]

Figure 2. Total energies of ordered (LIq structure, squares), random (circles) and segregated (triangles) fee RhsoPdso alloys as a function of the number of neighboring shells included in the local interaction zone. Values obtained by the LSGF-CPA method are shown by filled symbols and full lines. The energies obtained by the reference calculations are shown by a dashed line (LMTO, ordered sample), a dotted line (LMTO-CPA, random sample), and a dot-dashed line (interface Green s function technique, segregated sample). Figure 2. Total energies of ordered (LIq structure, squares), random (circles) and segregated (triangles) fee RhsoPdso alloys as a function of the number of neighboring shells included in the local interaction zone. Values obtained by the LSGF-CPA method are shown by filled symbols and full lines. The energies obtained by the reference calculations are shown by a dashed line (LMTO, ordered sample), a dotted line (LMTO-CPA, random sample), and a dot-dashed line (interface Green s function technique, segregated sample).
Figures 54.6 and 54.7 illustrate the concept of rise and run. If one assumes that line O-A in Figure 54.6 represents a true, or target, shaft centerline, then side a of the triangle represents the amount of offset present in the actual shaft, which is referred to as the rise. Figures 54.6 and 54.7 illustrate the concept of rise and run. If one assumes that line O-A in Figure 54.6 represents a true, or target, shaft centerline, then side a of the triangle represents the amount of offset present in the actual shaft, which is referred to as the rise.
Fig. 1.21. Ratio of free-path distribution Xp to the scaled zero-density free-path distribution plotted as a function of reduced free-path length r/X for two-dimensional (a) and three-dimensional (b) liquids. Circles, inverted triangles and upright triangles refer to reduced volumes V/V0 of 1.6, 2, and 3, respectively (V0 is the volume of the system at close packing) [74]. Fig. 1.21. Ratio of free-path distribution Xp to the scaled zero-density free-path distribution plotted as a function of reduced free-path length r/X for two-dimensional (a) and three-dimensional (b) liquids. Circles, inverted triangles and upright triangles refer to reduced volumes V/V0 of 1.6, 2, and 3, respectively (V0 is the volume of the system at close packing) [74].
Johnstone (2000) emphasises the importance of beginning with the macro and symbolic levels (Fig. 8.3) because both comers of the triangle are vistrahsable and can be made concrete with models (p. 12). The strb-micro level, by far the most difficult (Nelson, 2002), is described by the atomic theory of matter, in terms of particles such as electrorrs, atoms and molecules. It is commorrly referred to as the molecular level. Johnstone (2000) describes this level simirltaneorrsly as the strength and weakness of the subject of cherrristry it provides strength through the intellectual basis for chemical explanatiorrs, but it also presents a weakness when novice students try to learn and rmderstand it. [Pg.173]

Fig. 3.2 Triangular velocity reference signal top) and drive error signal bottom) of a Mossbauer drive operating in constant acceleration mode. The error signal is taken from the monitor output F of the drive control unit (see Fig. 3.1). Usually it is internally amplified by a factor of 100. Here, the deviations, including hum, are at the 2%o level of the reference. The peaks at the turning points of the triangle are due to ringing of the mechanical component, induced by the sudden change in acceleration (there should be no resonance line at the extremes of the velocity range)... Fig. 3.2 Triangular velocity reference signal top) and drive error signal bottom) of a Mossbauer drive operating in constant acceleration mode. The error signal is taken from the monitor output F of the drive control unit (see Fig. 3.1). Usually it is internally amplified by a factor of 100. Here, the deviations, including hum, are at the 2%o level of the reference. The peaks at the turning points of the triangle are due to ringing of the mechanical component, induced by the sudden change in acceleration (there should be no resonance line at the extremes of the velocity range)...
Figure 3.18. Time dependence of the peak position of the 1570 cm Raman band of Sj trans-stilbene in chloroform solution (filled triangle). The time dependence of the anti-Stokes/Stokes intensity ratio is also shown with open circles. The best fit of the peak position change with a single-exponential function is shown with a solid curve, while the best fit of the anti-Stokes/Stokes intensity ratio is shown with a dotted curve. The obtained lifetime for both single-exponential decay functions was 12ps. (Reprinted with permission from reference [78]. Copyright (1997) American Chemical Society.)... Figure 3.18. Time dependence of the peak position of the 1570 cm Raman band of Sj trans-stilbene in chloroform solution (filled triangle). The time dependence of the anti-Stokes/Stokes intensity ratio is also shown with open circles. The best fit of the peak position change with a single-exponential function is shown with a solid curve, while the best fit of the anti-Stokes/Stokes intensity ratio is shown with a dotted curve. The obtained lifetime for both single-exponential decay functions was 12ps. (Reprinted with permission from reference [78]. Copyright (1997) American Chemical Society.)...
Figure 9.11 Thiophene adsorbed at 500 K on an H-atom pretreated MoS2 cluster (50 x 54 A2). Beam-like features at the metallic edge [scan line (i)] and the shifted intensity of the outermost edge protrusions relative to the clean edge (triangles refer to the clean edge). These shifts in intensity [line scan (ii)] are associated with changes in the local electronic structure after adsorption of thiophene observed with STM. All the images were taken at room temperature subsequent to thiophene adsorption at 500 K. (Reproduced from Ref. 34). Figure 9.11 Thiophene adsorbed at 500 K on an H-atom pretreated MoS2 cluster (50 x 54 A2). Beam-like features at the metallic edge [scan line (i)] and the shifted intensity of the outermost edge protrusions relative to the clean edge (triangles refer to the clean edge). These shifts in intensity [line scan (ii)] are associated with changes in the local electronic structure after adsorption of thiophene observed with STM. All the images were taken at room temperature subsequent to thiophene adsorption at 500 K. (Reproduced from Ref. 34).
EPA. 1990. Interim methods for development of inhalation reference concentrations. Research Triangle Park, NC U.S. Environmental Protection Agency. EPA/600/8-88/066F. [Pg.148]


See other pages where Reference triangle is mentioned: [Pg.21]    [Pg.21]    [Pg.176]    [Pg.33]    [Pg.19]    [Pg.5]    [Pg.208]    [Pg.181]    [Pg.480]    [Pg.1677]    [Pg.18]    [Pg.153]    [Pg.228]    [Pg.6]    [Pg.162]    [Pg.202]    [Pg.14]    [Pg.121]    [Pg.406]    [Pg.197]    [Pg.22]    [Pg.120]    [Pg.32]    [Pg.387]    [Pg.111]    [Pg.214]    [Pg.283]    [Pg.622]    [Pg.97]    [Pg.172]   
See also in sourсe #XX -- [ Pg.117 ]




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