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Cascaded window

Figure 2-1 S3. The ViewerLite shows an elaborate depiction of hemoglobin on the right-hand side, with the amino acids in a cascade window on the left. Figure 2-1 S3. The ViewerLite shows an elaborate depiction of hemoglobin on the right-hand side, with the amino acids in a cascade window on the left.
Figure 9.3. The Cascaded window of the OPUS user interface. Figure 9.3. The Cascaded window of the OPUS user interface.
Since only ratios of liquid to window susceptibilities were determined by these methods we have determined the ratios of x in f.s., BK-7 and a-quartz (47) and have performed a cascading experiment to determine a-quartz x relative to its x (33) More detailed analysis of methods and results are available in the papers cited. [Pg.49]

Fig. 49. Cascade electrodes. S, substrate P, press-plate H, screw for maintaining electrode carrier E against press-plate P W, W, W", windows of the successive buffer vessels. Fig. 49. Cascade electrodes. S, substrate P, press-plate H, screw for maintaining electrode carrier E against press-plate P W, W, W", windows of the successive buffer vessels.
As the substrate is pressed against the front window of each buffer vessel, the paper is fed with buffer, while the free overflow at the back of each compartment to the one below avoids the building up of hydrostatic pressure even if the electrode is very high. Each front window bears the same pressure of a few millimeters of buffer, and the buffer can be fed at any desired rate without danger of flooding the curtain. That the cascade electrodes provide correct hydrodynamic qualities can be proved by the perfectly perpendicular chromatography of eosin spots on a curtain field of 60 X 60cm (Fig. 50). [Pg.105]

FIGURE 17.4. Differential particle size distrihution of B(a)P carhon black aerosol (100 pg/m ). Subsequent to exposure, substrate post-weights were recorded and entered into the Win-CIDRS (Windows-Cascade Impactor Data Reduction Program) to generate the particle size distribution for the particulate aerosol. From Hood et al. (2000). [Pg.233]

Table 4.4 shows how the main patterns of bursting occur in the model when parameter moves across the domain of complex periodic oscillations. Bursting occurs after the system has passed a domain of chaotic behaviour, which is itself reached beyond a cascade of period-doubling bifurcations issued from a simple periodic solution. A few narrow windows of chaos separate the first patterns of bursting observed. [Pg.139]

To illustrate the important notion that there exists a window of the ratio (Vi/1 2) producing oscillations, let us divide by 2 in the case of fig. 10.6. We see from eqns (10.5)-(10.6) that when the maximum rate of enzyme Ej in the minimal cascade model of fig. 10.4 is so halved, the threshold in the first cycle cannot be reached at any finite value... [Pg.441]

Figure 7.18. Traces from the 2D absorption-mode 7-resolved spectrum of menthol 7.1. (a) A region from the ID proton spectrum, (b) the 02 projection of the titled 2D spectrum showing proton-decoupled resonances and (c) the corresponding traces through the/i multiplets in the 2D spectrum. The multiplets for protons 3 and 4 are not fully decoupled for reasons described in the text. The data were acquired with a total acquisition time of 1 s in both t2 and fi using a 60Hz/i window. The selective 180° pulse was a 50 ms Q3 Gaussian cascade, and the gradient strength was 1% of the maximum 53 G cm 0 The broadband 180° pulses were BIPs (720.50.20) applied for 100 Xs at a Bi field strength of 20 kHz. Figure 7.18. Traces from the 2D absorption-mode 7-resolved spectrum of menthol 7.1. (a) A region from the ID proton spectrum, (b) the 02 projection of the titled 2D spectrum showing proton-decoupled resonances and (c) the corresponding traces through the/i multiplets in the 2D spectrum. The multiplets for protons 3 and 4 are not fully decoupled for reasons described in the text. The data were acquired with a total acquisition time of 1 s in both t2 and fi using a 60Hz/i window. The selective 180° pulse was a 50 ms Q3 Gaussian cascade, and the gradient strength was 1% of the maximum 53 G cm 0 The broadband 180° pulses were BIPs (720.50.20) applied for 100 Xs at a Bi field strength of 20 kHz.

See other pages where Cascaded window is mentioned: [Pg.87]    [Pg.87]    [Pg.2]    [Pg.294]    [Pg.730]    [Pg.200]    [Pg.701]    [Pg.182]    [Pg.182]    [Pg.104]    [Pg.183]    [Pg.54]    [Pg.99]    [Pg.268]    [Pg.632]    [Pg.269]    [Pg.6414]    [Pg.869]    [Pg.765]    [Pg.49]    [Pg.148]    [Pg.17]    [Pg.340]    [Pg.21]    [Pg.366]    [Pg.141]    [Pg.500]    [Pg.353]    [Pg.103]    [Pg.109]    [Pg.58]    [Pg.198]    [Pg.6413]    [Pg.291]    [Pg.190]    [Pg.30]    [Pg.12]    [Pg.142]    [Pg.72]    [Pg.427]    [Pg.349]    [Pg.351]   
See also in sourсe #XX -- [ Pg.73 ]




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