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Scattering timing sequence

Figure 2. LV-Raman scattering timing sequence. The LV signal, both raw and with conditioning and the LV validation pulse, are shown on the time scale 0-7 l>sec. The resultant laser pulse occurs after an additional adjustable delay, which was set for these experiments at about 10 psec in order to allow slow seed particles to escape from the test volume. Figure 2. LV-Raman scattering timing sequence. The LV signal, both raw and with conditioning and the LV validation pulse, are shown on the time scale 0-7 l>sec. The resultant laser pulse occurs after an additional adjustable delay, which was set for these experiments at about 10 psec in order to allow slow seed particles to escape from the test volume.
Special attention should be paid to one-sided deviation from the control limits, because systematic errors more often cause deviation in one direction than abnormally wide scatter. Two systematic errors of opposite sign would of course cause scatter, but it is unlikely that both would have entered at the same time. It is not necessary that the control chart be plotted in a time sequence. In any... [Pg.211]

Fig. 10.7 100 SERS spectra of CV displayed in the time sequence of measurement. Scattering volume 30 pL that contains an average of 0.5 crystal violet molecule. Each spectrum is acquired in 1 s. (Reprinted with permission from Ref [13].)... Fig. 10.7 100 SERS spectra of CV displayed in the time sequence of measurement. Scattering volume 30 pL that contains an average of 0.5 crystal violet molecule. Each spectrum is acquired in 1 s. (Reprinted with permission from Ref [13].)...
Fig. 14 Time sequence of a time-resolved small-angle scattering experiment Using a stopped-flow apparatus, the data acquisition time, can be synchronized with the mixing pulse time length, t, ... Fig. 14 Time sequence of a time-resolved small-angle scattering experiment Using a stopped-flow apparatus, the data acquisition time, can be synchronized with the mixing pulse time length, t, ...
Fig. 8.7. Time sequence of cold NO from 90 to 130/is after the peak of the scattering off of Ar. Fig. 8.7. Time sequence of cold NO from 90 to 130/is after the peak of the scattering off of Ar.
A feature of PC spreadsheets is that the position of rows or columns can be changed at the touch of a key, so the sequence of the rows of activities can be rapidly altered, and the position of the columns varied to preserve the diagonal pattern of crosses. This exercise can be executed a number of times to reduce the scatter of the stars away from the diagonal line and reduce the communicating distances between the activities. This has been carried out, and the result is shown in Table 7.2, where it can be seen that the stars are clustered more closely around the diagonal line. The list now shows the activities arranged in a preferred order of sequence. [Pg.74]

Fig. 16 (a) 2D-SAXS images of a 32.5 wt% solution of SI in toluene under an electric field of 3 kV/mm at different temperatures. The arrow in the first image indicates the direction of the electric field vector, (b) Azimuthal scattering intensity after background subtraction and normalization. The curves correspond to the sequence of images in (a), (c) Order parameter P% (filled circles) and temperature (solid line) as functions of time. Numbers 1-4 correspond to scattering patterns shown in (a) and (b). Adapted with permission from Macromolecules [72]. Copyright 2009 American Chemical Society... [Pg.26]


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Scattering time

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