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Circles square

Fig. 30.17. Square symbols are the actual objects and circled squares are the marked objects. Open circles are artificial points (adapted from Ref. [34]). Fig. 30.17. Square symbols are the actual objects and circled squares are the marked objects. Open circles are artificial points (adapted from Ref. [34]).
Fig. 1. Oxygen abundances as a function of the activity index, Rx, derived from X-ray data (left-hand panels) and the excitation temperature Texc (right-hand panels). The bottom panels show the difference between [O/Fe] yielded by the OI triplet at about 7774 A and the [OI] A6300 line. Filled circles RS CVn binaries ([2] and [3]), filled squares field subgiants [3], filled triangles Pleiades stars, open triangles Hyades stars, open circles, squares and hexagons disk dwarfs. The source of the literature data for the open cluster and Galactic disk stars can be found in [4]. Fig. 1. Oxygen abundances as a function of the activity index, Rx, derived from X-ray data (left-hand panels) and the excitation temperature Texc (right-hand panels). The bottom panels show the difference between [O/Fe] yielded by the OI triplet at about 7774 A and the [OI] A6300 line. Filled circles RS CVn binaries ([2] and [3]), filled squares field subgiants [3], filled triangles Pleiades stars, open triangles Hyades stars, open circles, squares and hexagons disk dwarfs. The source of the literature data for the open cluster and Galactic disk stars can be found in [4].
In Fig. 3.20, the experimental transition curves (circle, square, and diamond markers for LP0S. LP07, and LP06 modes, respectively) are plotted together with the Lorentzian fitting, while the fitting parameters are shown in Table 3.1. [Pg.62]

Figure 13.31 Potential shifts caused by the donor/acceptor interaction between ring 2 and dumbbell-shaped component 326+ when they are assembled in rotaxane 316+. Circles, squares,... Figure 13.31 Potential shifts caused by the donor/acceptor interaction between ring 2 and dumbbell-shaped component 326+ when they are assembled in rotaxane 316+. Circles, squares,...
Figures 3.42 through 3.44 (pp. 122 and 123) compare the spectral moments yo, yi, computed from first principles (solid curves) for the fundamental band of hydrogen, of the systems H2-H2 and H2-He, with the existing measurements (dots, circles, squares, etc.). The agreement is well within the experimental uncertainties of such measurements. Figures 3.42 through 3.44 (pp. 122 and 123) compare the spectral moments yo, yi, computed from first principles (solid curves) for the fundamental band of hydrogen, of the systems H2-H2 and H2-He, with the existing measurements (dots, circles, squares, etc.). The agreement is well within the experimental uncertainties of such measurements.
Figure 1. Adsorption isotherms for Xe in A1P04-31 at T = 100, 200, and 300 K (circles, squares, and diamonds respectively) as computed with GCMC simulations. Solid curves are fits to the data using the LUD isotherm. Figure 1. Adsorption isotherms for Xe in A1P04-31 at T = 100, 200, and 300 K (circles, squares, and diamonds respectively) as computed with GCMC simulations. Solid curves are fits to the data using the LUD isotherm.
Figure 16. The prehistory probability distribution of the escape trajectories for the parameters as in Fig. 13. The circles, squares, and triangles show single periods of the saddle cycies of periods 5 (S5), 3 (S3), and 1 (SI), respectively [173]. Figure 16. The prehistory probability distribution of the escape trajectories for the parameters as in Fig. 13. The circles, squares, and triangles show single periods of the saddle cycies of periods 5 (S5), 3 (S3), and 1 (SI), respectively [173].
Figure 12 Normalized diffraction efficiency measured from a PR material of compound 1 as a function of time during the grating erasure. The circles, squares, and triangles are experimental measurements with the grating spacings of 1.1, 1.9, and 4.4 xm, respectively, at an applied field of 77 V/ im. The lines are theoretical fittings using a biexponential function Eq. (42). The inset is its enlarged plot. (Reprinted from Ref. 27. Copyright 2000 The American Physical Society.)... Figure 12 Normalized diffraction efficiency measured from a PR material of compound 1 as a function of time during the grating erasure. The circles, squares, and triangles are experimental measurements with the grating spacings of 1.1, 1.9, and 4.4 xm, respectively, at an applied field of 77 V/ im. The lines are theoretical fittings using a biexponential function Eq. (42). The inset is its enlarged plot. (Reprinted from Ref. 27. Copyright 2000 The American Physical Society.)...
The resulting function also possesses other interesting properties. The function preserves the total mean of the features from one object because the values of the features change the amplitudes, whereas only the number of features changes the frequencies. Also variances for one object are maintained. Distances between two functions reflect dissimilarities between the objects. The example of the circle, square, and triangle in Section 5.2.2 demonstrates the quality of this method. Eight features are included in each FOURIER curve. The circle and the square resemble each other more than the triangle (Fig. 5-9). [Pg.149]

Fig. 4. Plot of log k vs. AG for the forward (solid symbols) and the back (open symbols) electron-transfer reactions (Eq. 3 and Eq. 4, respectively). Circles, squares, and triangles refer to Mn+ = Cr(bpy)3+, Rh-(phen)j+, and Ir(Me2phen)2Cl2, respectively. The curves are calculated by using Eq. (2) (full line) and the Marcus free energy relationship (Eq. 1, broken line), according to standard kinetic equations [61]... Fig. 4. Plot of log k vs. AG for the forward (solid symbols) and the back (open symbols) electron-transfer reactions (Eq. 3 and Eq. 4, respectively). Circles, squares, and triangles refer to Mn+ = Cr(bpy)3+, Rh-(phen)j+, and Ir(Me2phen)2Cl2, respectively. The curves are calculated by using Eq. (2) (full line) and the Marcus free energy relationship (Eq. 1, broken line), according to standard kinetic equations [61]...
Figure 12. TL-CD signal for ((-), circles), ((+), squares) and ((+/-), triangles) Co(en)33+ measured at 532 nm using the differentially arranged, TL configuration. Figure 12. TL-CD signal for ((-), circles), ((+), squares) and ((+/-), triangles) Co(en)33+ measured at 532 nm using the differentially arranged, TL configuration.
Fig. 3. Circles, squares, triangles and crosses are the QE of supply as a function of electric field for PVK films of different thickness. The solid line is the Onsager expression for <2>0 = 0.11 and... Fig. 3. Circles, squares, triangles and crosses are the QE of supply as a function of electric field for PVK films of different thickness. The solid line is the Onsager expression for <2>0 = 0.11 and...
Fig. 12 Plots oflog k vs. A G° from entries nos. 2 (aromatic amines and ethers open and filled circles, triangles) and 3 (aliphatic amines semi-filled circles, squares) of Table 12. The upper and lower curve have been drawn with AG (0) = 3 and 5 kcal mol-1... Fig. 12 Plots oflog k vs. A G° from entries nos. 2 (aromatic amines and ethers open and filled circles, triangles) and 3 (aliphatic amines semi-filled circles, squares) of Table 12. The upper and lower curve have been drawn with AG (0) = 3 and 5 kcal mol-1...
Fig. 62. Correlation of the Flory-Huggins Interaction Parameter, /, for polystyrene-liquid systems at 25 °C with the relative swelling power (C) of the corresponding liquid at 23 °C as a function of the volume fraction (v) of the polymer in the system. The /-data at v = 1.0, 0.8, 0.6, 0.4, 0.2, and 0.0 are represented respectively by the symbols star, circle, square, triangle pointing upward, triangle pointing downward, and narrow oval. The /-data determined experimentally are represented by the filled symbols, whereas those obtained by interpolation or by extrapolation as noted in Fig. 61 are represented by the corresponding empty symbols... Fig. 62. Correlation of the Flory-Huggins Interaction Parameter, /, for polystyrene-liquid systems at 25 °C with the relative swelling power (C) of the corresponding liquid at 23 °C as a function of the volume fraction (v) of the polymer in the system. The /-data at v = 1.0, 0.8, 0.6, 0.4, 0.2, and 0.0 are represented respectively by the symbols star, circle, square, triangle pointing upward, triangle pointing downward, and narrow oval. The /-data determined experimentally are represented by the filled symbols, whereas those obtained by interpolation or by extrapolation as noted in Fig. 61 are represented by the corresponding empty symbols...
Despite their popularity, many criticize the elongation ratio and aspect ratio for their inability to truly reflect the shape of a particle as both the elongation and aspect ratios are equal to 1 for any symmetrical shape such as a circle, square, etc., since the length and breath is the same for these symmetrical shapes (42,43). [Pg.59]

Label each class with a different-type box (circle, square, diamond, etc.) and let arrows connect the boxes to show the sequence of information flow for your procedure. [Pg.64]

Fig. 1.37 Model of enhanceosome function during transcription activation. The requirement for only a single regulator or multiple transcriptional regulators, organized in the enhanceosome, may depend on the state of chromatin. In chromatin state 1, the promotor is covered by a nucleosome and binding of three regulators (circle, square, triangle) is required to achieve effective recruitment of chromatin modification complexes and to free the promotor for binding of the RNA polymerase ho-... Fig. 1.37 Model of enhanceosome function during transcription activation. The requirement for only a single regulator or multiple transcriptional regulators, organized in the enhanceosome, may depend on the state of chromatin. In chromatin state 1, the promotor is covered by a nucleosome and binding of three regulators (circle, square, triangle) is required to achieve effective recruitment of chromatin modification complexes and to free the promotor for binding of the RNA polymerase ho-...
Figure 3. Rate constants for the reaction of with N2 as a function of temperature. The HTFA," the NOAA (T), and NOAA (KE) data are shown as circles, squares and diamonds, respectively. See the text for a description of the predicted values. Figure 3. Rate constants for the reaction of with N2 as a function of temperature. The HTFA," the NOAA (T), and NOAA (KE) data are shown as circles, squares and diamonds, respectively. See the text for a description of the predicted values.
The linear algebra approaches used in first-order methods for pattern recognition are simple mathematical distance measurements in a multidimensional space. By using some examples of data plotted in a two-dimensional space resulting from an array of two sensors, simple relationships can be established that are identical in higher-dimensional spaces. In figure 11.3, the uppermost plot contains the responses of two sensors for pure samples with constant concentrations of three analytes denoted by circles, squares, and triangles. The two sensors have differential selectivity to the three analytes. The locations in this two-dimensional space of the analytes are physically separated from each other. The distribution of each cluster is caused by the combination of the measurement error of the two sensors. [Pg.299]

To Find the Square Surface or Area of a Circle. Square the radius (half the diameter), and multiply that by 3.14159 for small calculations is nearly the same as 3.14159. Thus, to find the area of a circle whose diameter is 8 feet The radius is 4 feet, this squared is 16 then 16 times 3.14159 is 50.265 square feet. If the diameter is 8... [Pg.341]

Diameter of Circle. Square Inches. Diameter of Circle. Sqnare Inches. [Pg.341]

Fig. 9. Experimental (circles, squares, diamonds) and calculated (curves) values for the atomic Fe and Co moments in disordered and ordered Fe-Co alloys. Fig. 9. Experimental (circles, squares, diamonds) and calculated (curves) values for the atomic Fe and Co moments in disordered and ordered Fe-Co alloys.
General Accurate Correlation Equation. Solutions are also available for various combinations of contact areas and flux tubes such as circle/circle and circle/square for the uniform flux, true isothermal, and equivalent isothermal boundary conditions [71]. [Pg.169]

Circle/square, uniform flux Circle/square, equivalent 1.08076 -1.24110 0.18210 0.00825 0.038916... [Pg.169]


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