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Distribution slicing

Strawberries and sliced bread were purchased from a local market. Damaged, non-uniform, unripe or overripe strawberries were removed and the selected fruits were stored for at least 2 h at 3°C to ensure their thermal equilibrium. Strawberries were selected for this study due to their rapid post-harvest deterioration, which constitutes a problem on their commercial distribution. Sliced bread was selected due to the increasing consumer demand for fresh bread with long shelf-life. [Pg.6]

A bond m which the orbitals overlap along a line connecting the atoms (the inter nuclear axis) is called a sigma (a) bond The electron distribution m a ct bond is cylm drically symmetric were we to slice through a ct bond perpendicular to the mternuclear axis Its cross section would appear as a circle Another way to see the shape of the elec tron distribution is to view the molecule end on... [Pg.60]

Clearly, the plot of Figure 8-3 contains information about the distribution of kinetic energies. From the rate of rotation of the discs and the distance between them we can calculate the velocity an atom must have to condense on a particular pie slice. From the atomic mass and its velocity, we learn the atom s kinetic energy. Figure 8-4 shows the result. At a temperature Tt... [Pg.131]

Figure 17. Steps in the constmction of a datacube of the nucleus of NGC1068 from observations with the integral held unit of the Gemini Multiobject Spectrograph installed on the Gemini-north telescope. The datacube is illustrated by a few spectra distributed over the field and equivalently by a few slices at a given radial velocity in the light of the [OIII]5007 emission line. Only a few percent of the total data content is shown. Figure 17. Steps in the constmction of a datacube of the nucleus of NGC1068 from observations with the integral held unit of the Gemini Multiobject Spectrograph installed on the Gemini-north telescope. The datacube is illustrated by a few spectra distributed over the field and equivalently by a few slices at a given radial velocity in the light of the [OIII]5007 emission line. Only a few percent of the total data content is shown.
Furthermore, in the more general case we are concerned with a variation of composition and sequence length distribution not only as a function of retention volume but within each chromatogram area segment (or "slice ) at each retention volume. A significant polydispcrsity of one of these properties within a chromatogram slice can easily invalidate the polymer analysis described above. [Pg.167]

Figure 20 shows an example of its use. As expected, the GPC 2 chromatogram of a fraction of a monodisperse standard (obtained by sampling it with GPC 2 at its peak) is narrower than the whole standard which in turn is narrower than chromatograms of slices of broad polystyrene distributions. In Figure 20, two examples of the latter show the difference obtained by improving resolution in GPC 1. [Pg.175]

Another sampling effect which deserves mention is that since the molecular weight distribution shifl towards higher molecular weights with conversion, a slice will not in general contain proportionate amounts of polymer from all conversions. This dufting can be accounted for in the theoretical predictions by incorporating it into cumulation of the instantaneous property distributions (e.g. Equation 8). [Pg.177]

Fig. 2.9.2 Radiofrequency, field gradient and current distributions requires a three-dimen-ionic current pulse sequences for two-dimen- sional imaging sequence [see Figure 2.9.1(a)] sional current density mapping. TE is the Hahn and multiple experiments with the orientation spin-echo time, Tc is the total application time of the sample relative to the magnetic field of ionic currents through the sample. The 180°- incremented until a full 360°-revolution is pulse combined with the z gradient is slice reached. The polarity of the current pulses... Fig. 2.9.2 Radiofrequency, field gradient and current distributions requires a three-dimen-ionic current pulse sequences for two-dimen- sional imaging sequence [see Figure 2.9.1(a)] sional current density mapping. TE is the Hahn and multiple experiments with the orientation spin-echo time, Tc is the total application time of the sample relative to the magnetic field of ionic currents through the sample. The 180°- incremented until a full 360°-revolution is pulse combined with the z gradient is slice reached. The polarity of the current pulses...
Fig. 3.3.9 Velocity encoded imaging (upper) and radial velocity distribution (lower) for a flow of water at 2.93 mm3 s- through the fixed bed reactor, taken in the same slice as for Figure 3.3.8. (a) Spherical glass beads of 2 mm in diameter and (b) cylindrical pellets with average equivalent diameter of 2.2 mm. Fig. 3.3.9 Velocity encoded imaging (upper) and radial velocity distribution (lower) for a flow of water at 2.93 mm3 s- through the fixed bed reactor, taken in the same slice as for Figure 3.3.8. (a) Spherical glass beads of 2 mm in diameter and (b) cylindrical pellets with average equivalent diameter of 2.2 mm.
Fig. 5.1.8 MRM maps of velocity (bottom row) resolution is 54.7 im per pixel (128 x 128 -and T2 magnetic relaxation (top row) as a pixels) in plane, so the data reflect pore scale function of biofilm growth time (left to right), spatial distributions of velocity over a 1000-pm Day 1 shows the clean porous media. Spatial slice and biomass over a 200-gm slice. Fig. 5.1.8 MRM maps of velocity (bottom row) resolution is 54.7 im per pixel (128 x 128 -and T2 magnetic relaxation (top row) as a pixels) in plane, so the data reflect pore scale function of biofilm growth time (left to right), spatial distributions of velocity over a 1000-pm Day 1 shows the clean porous media. Spatial slice and biomass over a 200-gm slice.

See other pages where Distribution slicing is mentioned: [Pg.430]    [Pg.430]    [Pg.430]    [Pg.111]    [Pg.112]    [Pg.112]    [Pg.590]    [Pg.650]    [Pg.111]    [Pg.112]    [Pg.112]    [Pg.430]    [Pg.430]    [Pg.430]    [Pg.111]    [Pg.112]    [Pg.112]    [Pg.590]    [Pg.650]    [Pg.111]    [Pg.112]    [Pg.112]    [Pg.35]    [Pg.630]    [Pg.644]    [Pg.135]    [Pg.190]    [Pg.131]    [Pg.90]    [Pg.1050]    [Pg.905]    [Pg.210]    [Pg.188]    [Pg.239]    [Pg.86]    [Pg.335]    [Pg.4]    [Pg.293]    [Pg.18]    [Pg.26]    [Pg.27]    [Pg.257]    [Pg.275]    [Pg.441]    [Pg.469]    [Pg.504]    [Pg.523]    [Pg.526]    [Pg.538]    [Pg.544]   
See also in sourсe #XX -- [ Pg.430 ]




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