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Comparison of reproduceability

The comparison of reproduceability of diameters of dots in the highlight areas between the Photopolymer Plate and zinc plate from a negative film, showed 90-95% for the Photopolymer Plate and about 75% for a zinc plate because the latter showed color loss. (See Fig. 15)... [Pg.275]

Comparison of Reproduceability of Halftones between the Photopolymer Plate and Powderless Etched Zinc or Magnesium Plate As shown in Fig. 16, the Photopolymer Plate will reproduce the halftone almost completely from the negative film. This is in comparison with photopolymer plates, zinc plates or magnesium plates which give much less reproduceability. [Pg.275]

Comparison of Reproduceability of Isolated Image Lines between the Photopolymer Plate and Powderless Etched Zinc or Magnesium Plate. [Pg.275]

Figure 16. Comparison of reproduceability of halftones between the metal plate and the Photopolymer Plate (9) the Photopolymer Plate (A) Zn plate (powder-less-etched) (O) Mg plate (powderless-etched)... Figure 16. Comparison of reproduceability of halftones between the metal plate and the Photopolymer Plate (9) the Photopolymer Plate (A) Zn plate (powder-less-etched) (O) Mg plate (powderless-etched)...
Table 3- Comparison of Reproduceability of Dot Diameters in Stereos made from Zinc Plate and the Photopolymer Plate... Table 3- Comparison of Reproduceability of Dot Diameters in Stereos made from Zinc Plate and the Photopolymer Plate...
The SI values can be used for comparing the pyrogram of an unknown sample and that of a known substance, and for determining the reproducibility of the pyrolysis system. Within the same laboratory, a similarity index of 95% for two consecutive Py-GC runs is possible using the Pyroprobe system. However, comparison of reproducibility as reported by different laboratories may not be justified, since individual groups have their own pyrolysis techniques. [Pg.410]

Figure Cl.5.4. Comparison of near-field and far-field fluorescence images, spectra and lifetimes for the same set of isolated single molecules of a carbocyanine dye at a PMMA-air interface. Note the much higher resolution of the near-field image. The spectmm and lifetime of the molecule indicated with the arrow were recorded with near-field excitation and with far-field excitation at two different excitation powers. Reproduced with pennission from Trautman and Macklin [125]. Figure Cl.5.4. Comparison of near-field and far-field fluorescence images, spectra and lifetimes for the same set of isolated single molecules of a carbocyanine dye at a PMMA-air interface. Note the much higher resolution of the near-field image. The spectmm and lifetime of the molecule indicated with the arrow were recorded with near-field excitation and with far-field excitation at two different excitation powers. Reproduced with pennission from Trautman and Macklin [125].
A comparison of Fig. 4 and Fig. 3 shows that this uncoupled QCMD bundle reproduces the disintegration of the full QD solution. However, there are minor quantitative differences of the statistical distribution. Fig. 5 depicts... [Pg.392]

Fig. 4. Comparison of the three types of tetracycline resistance where T represents the tetracycline molecule O, a tetracycline transporter and aaa/, the ribosome A shows the effect of tetracycline exposure on a sensitive cell B, the efflux of resistance where a cytoplasmic membrane protein ( D) pumps tetracycline out of the cell as fast as the tetracycline transporter takes it up C, the ribosomal protection type of resistance where the ribosome is modified by ( ) to block productive binding and D, the tetracycline modification type of resistance where t is an inactive form of tetracycline. Reproduced with... Fig. 4. Comparison of the three types of tetracycline resistance where T represents the tetracycline molecule O, a tetracycline transporter and aaa/, the ribosome A shows the effect of tetracycline exposure on a sensitive cell B, the efflux of resistance where a cytoplasmic membrane protein ( D) pumps tetracycline out of the cell as fast as the tetracycline transporter takes it up C, the ribosomal protection type of resistance where the ribosome is modified by ( ) to block productive binding and D, the tetracycline modification type of resistance where t is an inactive form of tetracycline. Reproduced with...
Fig. 19. Comparison of undeveloped grain (left) exposed and developed grain (center) and silver of a single unexposed grain that has transferred and developed to form a positive image deposit (97). Reproduced with permission of IS T, the Society for Imaging Science and Technology. Fig. 19. Comparison of undeveloped grain (left) exposed and developed grain (center) and silver of a single unexposed grain that has transferred and developed to form a positive image deposit (97). Reproduced with permission of IS T, the Society for Imaging Science and Technology.
A dynamic transition in the internal motions of proteins is seen with increasing temperamre [22]. The basic elements of this transition are reproduced by MD simulation [23]. As the temperature is increased, a transition from harmonic to anharmonic motion is seen, evidenced by a rapid increase in the atomic mean-square displacements. Comparison of simulation with quasielastic neutron scattering experiment has led to an interpretation of the dynamics involved in terms of rigid-body motions of the side chain atoms, in a way analogous to that shown above for the X-ray diffuse scattering [24]. [Pg.248]

Kister discusses his comparison tests in great detail and presents Figures 20 and 21 for comparison of capacity and efficiency. We quote from his summary as follows (Reproduced with permission of the American Institute of Chemical Engineers, copyright 1994 AlChE, all rights reserved) ... [Pg.92]

Fig. 1.32. (a) Molecular graphs and electron density contours for pentane and hexane. Dots on bond paths represent critical points, (b) Comparison of molecular graphs for bicycloalkanes and corresponding propellanes. (Reproduced from Chem. Rev. 91 893 (1991) with permission of the American Chemical Society.)... [Pg.58]

FIGURE S.30 Comparison of ambient levels of t h maximum ozone, annual average of total suspended particulate matter (TSP), and sulfur dioxide in selected cities from around the world to illustrate the v tacion in these levels from countr)i to country with respect to the United States. [Reproduced from the National Air Quality and Emission Trends Report (1992), with permission.] ... [Pg.252]

Figure 9-18. Overall comparison of efficiency for "state-of-the-art random and structured packing with trays at 24-in. spacing. Reproduced with permission of the American Institute of Chemical Engineers Kister, H. Z., Larson, K. F., Yanagi, T. Chemical Engineering Progress, V. 90, No. 2 (1994) p. 23 all rights reserved. Figure 9-18. Overall comparison of efficiency for "state-of-the-art random and structured packing with trays at 24-in. spacing. Reproduced with permission of the American Institute of Chemical Engineers Kister, H. Z., Larson, K. F., Yanagi, T. Chemical Engineering Progress, V. 90, No. 2 (1994) p. 23 all rights reserved.
Figure 15.7 (b) Comparison of the photoinduced absorption spectra for near steady stale (millisecond) and ultrafast (picosecond) lime domains for P30T/C composite films. The picosecond photoinduced spectra arc taken at 300 K at various delay limes after a 2.01 eV 100 Is pump pulse for P3OT and P30T/C,., (reproduced by permission of World Scientific from Ref. I7 ). [Pg.587]

Fig. 4.1.15 Comparison of the luminescence and fluorescence emission spectra of natural aequorin (left panel) and recombinant e-aequorin (right panel) the luminescence spectra of Ca2+ -triggered reaction (dark solid lines), the fluorescence emission spectra of the spent solution containing 2 mM Ca2+ (dashed lines), and the luminescence spectra of the spent solution after addition of coelenterazine (light solid lines). Reproduced with permission, from Shimomura, 1995d. the Biochemical Society. Fig. 4.1.15 Comparison of the luminescence and fluorescence emission spectra of natural aequorin (left panel) and recombinant e-aequorin (right panel) the luminescence spectra of Ca2+ -triggered reaction (dark solid lines), the fluorescence emission spectra of the spent solution containing 2 mM Ca2+ (dashed lines), and the luminescence spectra of the spent solution after addition of coelenterazine (light solid lines). Reproduced with permission, from Shimomura, 1995d. the Biochemical Society.
Figure 10.15 Comparison of the fit of the Debye heat capacity equation for several elements. Reproduced from K. S. Pitzer. Thermodynamics. McGraw-Hill, Inc., New York, 1995, p. 78. Reproduced with permission of the McGraw-Hill Companies. Figure 10.15 Comparison of the fit of the Debye heat capacity equation for several elements. Reproduced from K. S. Pitzer. Thermodynamics. McGraw-Hill, Inc., New York, 1995, p. 78. Reproduced with permission of the McGraw-Hill Companies.
Fig. 10. Comparison of the measured refractive indices for PET film with values calculated from the orientation functions determined from n.m.r. assuming transversely isotropic structural units. I, Experimental points predicted values. Reproduced from Polymer by permission of the publishers, Butterworth Co (Publishers) Ltd. (C)... Fig. 10. Comparison of the measured refractive indices for PET film with values calculated from the orientation functions determined from n.m.r. assuming transversely isotropic structural units. I, Experimental points predicted values. Reproduced from Polymer by permission of the publishers, Butterworth Co (Publishers) Ltd. (C)...
The simple fitting procedure is especially useful in the case of sophisticated nonlinear spectroscopy such as time domain CARS [238]. The very rough though popular strong collision model is often used in an attempt to reproduce the shape of pulse response in CARS [239]. Even if it is successful, information obtained in this way is not useful. When the fitting law is used instead, both the finite strength of collisions and their adiabaticity are properly taken into account. A comparison of... [Pg.188]

Verification of this structure is provided by the comparison with calculated intensity curves. In Fig. 6 curve A represents the model described above and curve B a similar model with the C=C bond distance equal to 1.38 A., as given by the original table of covalent radii. Each of these curves reproduces closely the qualitative aspect of the photographs curve A also shows quantitative agreement, whereas curve B shows a systematic difference of about 3%. The quantitative comparison of measured ring diameters and r values for the maxima and minima of curve A is shown in Table VIII. [Pg.649]

Figure 2. The binding and dissociation of FLPEP and receptor on intact neutrophils at 37 C The data are plotted as the specific binding of FLPEP (pmoles/10 cells) on a log plot versus time. Experimental details 10 cells/mL were exposed at time 0 to 1 nAf FLPEP. At 15, 30, 60, or 120 s, antibody to fluorescein is added to each sample. Fluorescence is monitored continuously during the additions. The data ate derived from a point-by-point comparison of the fluorescence measured under conditions of receptor binding and receptor blockade. Data are representative of observations in more than 10 separate experiments. (Reproduced with permission from reference 22. Copyright 19S7 Journal of Biological Chemistry.)... Figure 2. The binding and dissociation of FLPEP and receptor on intact neutrophils at 37 C The data are plotted as the specific binding of FLPEP (pmoles/10 cells) on a log plot versus time. Experimental details 10 cells/mL were exposed at time 0 to 1 nAf FLPEP. At 15, 30, 60, or 120 s, antibody to fluorescein is added to each sample. Fluorescence is monitored continuously during the additions. The data ate derived from a point-by-point comparison of the fluorescence measured under conditions of receptor binding and receptor blockade. Data are representative of observations in more than 10 separate experiments. (Reproduced with permission from reference 22. Copyright 19S7 Journal of Biological Chemistry.)...
Data of Badder and Brooks (24). Figure 7 shows the comparisons of EPM with the experimental data obtained by Badder and Brooks (2A) in a CSTR (run C-24). The reactor feed contained 22.8% styrene, 0.64% emulsifier (sodium dodecylsulfate), and 0.39% initiator (ammonium persulfate). The residence time was 114 min. The initial reactor charge was water and emulsifier. In this case the size of the primary precursors was varied slightly from its baseline value of 1 nm to 0.8 nm. Although the experimental data show some scatter, EPM reproduces very well both the transient and steady state... [Pg.375]


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Reproducibility

Reproducible

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