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Lined fitting

Cu/ Zn0/Si02 catalyst obtained with different doses of 5 keV Ne" ions (see insert, spectra are shifted vertically for clarity). Catalyst reduction temperature 700 K. Solid lines fitted Gauss peaks [3.147]. (b) The relative coverage of Cu and ZnO on the silica-supported catalyst, reduced at 700 K, as a function of the ion dose [3.147]. [Pg.158]

A simple bellows has the advantage that it is an in-line fitting and requires no packing, as does the sliding joint... [Pg.342]

As the pump provides flow, it transmits a force to the fluid. When the flow encounters resistance, this force is changed into pressure. Resistance to flow is the result of a restriction or obstruction in the flow path. This restriction is normally the work accomplished by the hydraulic system, but there can also be restrictions created by the lines, fittings or components within the system. Thus, the... [Pg.595]

For any distribution, the cumulative hazard function and the cumulative distribution junction are connected by a simple relationship. The probability scale for the cumulative distribution function appears on the horizontal axis at the top of hazard paper and is determined from that relationship. Thus, the line fitted to data on hazard paper... [Pg.1050]

The least-square straight line fit through points at — 1, 0, 1 is... [Pg.95]

St Line Fit 2mm Model I Model III St Line Fit 2mm Model I Model III Density Det Vet det 5 (kbar)... [Pg.845]

Fig. 7.72 Pt (99 keV) Mossbauer spectrum of the one-dimensional conductor K2[Pt(CN)4] Bro.3o 3H20 at 4.2 K (source Au in platinum at 4.2 K). The solid line represents a single Lorentzian line fitted to the measured spectrum. The dashed line represents the best fit using a sum of two Lorentzian lines with an intensity ratio of 85 15 and with the isomer shifts of the spectra of K2[Pt(CN)4]-3H20 and K2[(Pt(CN)4Br2] (from [333])... Fig. 7.72 Pt (99 keV) Mossbauer spectrum of the one-dimensional conductor K2[Pt(CN)4] Bro.3o 3H20 at 4.2 K (source Au in platinum at 4.2 K). The solid line represents a single Lorentzian line fitted to the measured spectrum. The dashed line represents the best fit using a sum of two Lorentzian lines with an intensity ratio of 85 15 and with the isomer shifts of the spectra of K2[Pt(CN)4]-3H20 and K2[(Pt(CN)4Br2] (from [333])...
The denominator in (3.1) can be simplified because the statistical uncertainty of the baseline, hN o, is negligible in practice when the spectra are simulated with numerical line fit routines. The stochastic emission of y-rays by the source leads to a Poisson distribution of counts with the width AA = and since is small, the denominator of (3.1) can be written as ... [Pg.542]

Figure 3.20. TR spectra of fluoranil in 2-propanol obtained (after band fitting and deconvolution) at various time delays (Ap nip 355 nm, Apj bs 416 nm) (a) 10 ns, (b) 50ns, (c) 100ns, (d) 150ns, (e) 250ns, (f) 500 ns, (g) 1.3 ps, (h) 3.0 ps, [a] dots - original spectra and line-fitted spectra, [b] after the deconvolution of each band - the bands indicated as lines belong to the ketyl radical and the bands indicated as dots belong to the radical anion. See text for more details. (Reprinted from reference [91]. Copyright (1997), with permission from Elsevier.)... Figure 3.20. TR spectra of fluoranil in 2-propanol obtained (after band fitting and deconvolution) at various time delays (Ap nip 355 nm, Apj bs 416 nm) (a) 10 ns, (b) 50ns, (c) 100ns, (d) 150ns, (e) 250ns, (f) 500 ns, (g) 1.3 ps, (h) 3.0 ps, [a] dots - original spectra and line-fitted spectra, [b] after the deconvolution of each band - the bands indicated as lines belong to the ketyl radical and the bands indicated as dots belong to the radical anion. See text for more details. (Reprinted from reference [91]. Copyright (1997), with permission from Elsevier.)...
Cununing GL, Rollett JS, Rosotti FJC, Whewell RJ (1972) Statistical methods for the computation of stability constants, I. Straight-line fitting of points with correlated errors. J Chem Soc Dalton Trans 23 2652-2658... [Pg.651]

The first aspect of the Y+CH3OH reaction that will be discussed is that of non-reactive (NR) scattering, which is common to all reactions studied in our laboratory. Non-reactive TOF spectra for the Y + CH3OH reaction are shown in Fig. 9, recorded at m/e 89 (Y+). The solid-line fits to the experimental data are actually the sum of two processes, represented by dotted and dashed lines. The dotted line corresponds to inelastically-scattered Y... [Pg.229]

Fig. 11. Time-of-flight spectra for YH2 and YOCH3 products at indicated lab angles for the Y+CH3OH reaction at con = 28.1 kcal/mol. TOFs have been scaled to the same number of scans. Solid-line fits generated using the CM distributions shown in Fig. 12. Fig. 11. Time-of-flight spectra for YH2 and YOCH3 products at indicated lab angles for the Y+CH3OH reaction at con = 28.1 kcal/mol. TOFs have been scaled to the same number of scans. Solid-line fits generated using the CM distributions shown in Fig. 12.
Fig. 15. Newton diagram in velocity space for Y+cyclopropane at Eco = 18.5 kcal/mol. Larger solid circle corresponds to maximum velocities for YCH2 products, while smaller solid circle and smaller dotted circle correspond to maximum velocities for Y-propyne and Y-allene products, respectively. Lab angular distributions for YCH2 (open squares) and YC3H4 (open circles) recorded under identical collision conditions. Solid-line fits to lab angular distributions generated using CM distributions in Fig. 17. Fig. 15. Newton diagram in velocity space for Y+cyclopropane at Eco = 18.5 kcal/mol. Larger solid circle corresponds to maximum velocities for YCH2 products, while smaller solid circle and smaller dotted circle correspond to maximum velocities for Y-propyne and Y-allene products, respectively. Lab angular distributions for YCH2 (open squares) and YC3H4 (open circles) recorded under identical collision conditions. Solid-line fits to lab angular distributions generated using CM distributions in Fig. 17.
Fig. 16. Sample TOF spectra recorded at indicated lab angles for (a) YCH2 and (b) YC3H4 products from collisions of Y + cyclopropane at Econ = 18.5kcal/mol (open points). Solid-line fits generated using CM distributions in Fig. 17. Fig. 16. Sample TOF spectra recorded at indicated lab angles for (a) YCH2 and (b) YC3H4 products from collisions of Y + cyclopropane at Econ = 18.5kcal/mol (open points). Solid-line fits generated using CM distributions in Fig. 17.
Figure 16. Appearance curve of Na+ from CID of Na+N-methylacetamide. The calculated curve (solid line), fitted using experimental points from 1.4-4.0 eV, corresponds to n = 1.25 and E0 = 1.69 eV (38.9 kcal/mol). The cross section model in equation 50 is used. From Klassen, J. S. Anderson, S. G. Blades, A. T. Kebarle, P. J. Phys. Chem. 1996, 100,14218, with permission. Figure 16. Appearance curve of Na+ from CID of Na+N-methylacetamide. The calculated curve (solid line), fitted using experimental points from 1.4-4.0 eV, corresponds to n = 1.25 and E0 = 1.69 eV (38.9 kcal/mol). The cross section model in equation 50 is used. From Klassen, J. S. Anderson, S. G. Blades, A. T. Kebarle, P. J. Phys. Chem. 1996, 100,14218, with permission.
Fig. 42 Double-logarithmic dependence of first-order reflection peak, q, on total degree of polymerization, N. o AB diblocks A2B2 miktoarm stars. Solid lines fitting results for power law scaling of q N a, with a = 0.73 0.04 and 0.70 0.04 for linear and stars respectively. From [120]. Copyright 2000 American Chemical Society... Fig. 42 Double-logarithmic dependence of first-order reflection peak, q, on total degree of polymerization, N. o AB diblocks A2B2 miktoarm stars. Solid lines fitting results for power law scaling of q N a, with a = 0.73 0.04 and 0.70 0.04 for linear and stars respectively. From [120]. Copyright 2000 American Chemical Society...
Fig. 4.10. (A) Schematic of percentage weights of glycerol in composite solvents corresponding to array of fluorescein solutions of varying viscosity (B) fluorescence lifetime (C) rotational correlation time images of this array and (D) plot of the rotational correlation time as a function of viscosity for this sample array exited at 470 nm the straight line fit yields a fluorophore radius of 0.54 nm for fluorescein. Adapted from Fig. 2 of Ref. [64]. Fig. 4.10. (A) Schematic of percentage weights of glycerol in composite solvents corresponding to array of fluorescein solutions of varying viscosity (B) fluorescence lifetime (C) rotational correlation time images of this array and (D) plot of the rotational correlation time as a function of viscosity for this sample array exited at 470 nm the straight line fit yields a fluorophore radius of 0.54 nm for fluorescein. Adapted from Fig. 2 of Ref. [64].

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