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A tree topology is similar to bus topology except that tree networks contain branches with multiple nodes. As in bus topology, all signals traverse the entire bus length. The advantage is that it requires less cabling than ring or star topology. However, if any device is broken, the sequence is disrupted and the entire network goes down. Therefore, bus or tree topologies are not used today.

(9.35)

heat and mass transfer becomes large, and this is thought to be reasonable. Results for heat of pyrolysis and temperature for maximum decomposition rate are given in Tables 15.16 15.21. The heat of pyrolysis depends on the differences in the chemical structure of the material. The weight loss due to the volatiles released during the pyrolysis exhibits itself as an endotherm, which goes though a wellde ned minima. They correspond to the respective volatile loss that evolves from cellulose, polypropylene, or polystyrene. As for the temperature for maximum decomposition rate compare the results obtained with TGA with DSC results. The peak of the DSC curves evolves earlier than the peak from the TGA data. This may be due to the mass transfer limitations. The rate-controlling step (reaction

-4 0

Initially the table will use its rst eld as its primary key. To make it use both the FirstName and LastName elds instead, select the Indices tab as shown in Figure 16-10. Click and drag the LastName eld into the Index Columns area on the lower right.

0.02 0.015 0.01 0.005

This further modi cation of the BPD is widely used (Baltasar et al., 2001; Hess and Hess, 1998; Lagace et al., 1995). Here, the greater curve of the stomach is resected, leaving the lesser curvature, pylorus and rst part of duodenum in continuity as a tube for anastomosis to the alimentary limb of distal ileum. Thus, the proximal gastric pouch of the BPD is replaced by a lesser curvature gastric tube of 150 250 ml capacity that, at least initially, restricts food intake. The biliopancreatic limb is again joined to the distal ileum (Figure 18.5). By preserving the pylorus, the duodenal switch avoids both the dumping syndrome and marginal

12.3. IMAGING OF THE INTERFERENCE PATTERN IN NON-NULL TESTS An aberrated wavefront continuously changes its shape as it travels; therefore, if the wavefront is aspherical, the interference pattern will also continuously change as the beam advances as shown in Figure 12.5. Since the errors of an instrument are represented by wavefront distortions on the pupil, the interferogram should represent the wavefront deformations at that place. The problem is even worse if the wavefront travels twice through the optical system during the test. For example, when testing a lens with any of the con gurations as described in 2, the wavefront travels twice through the lens; the second time, it travels after being re ected from the small mirror in front of the lens. If the aberration is small, the total wavefront deformation is twice the deformation

HVL of the beam), the thickness of the tissue layer in the primary beam, and the entrance exposure. The amount of entrance exposure for a given film/screen combination will obviously be quite a bit higher to allow for absorption in the tissue thickness being imaged, and is a function of the same parameters, which can be represented as an absorption factor (AF). Values of AF are listed in Table 15-12 for combinations of tissue thickness and HVLs of x-ray beams and are accurate to 10% for source to skin distances of 45 90 cm. All other factors related to x-ray beam quality (e.g., kVp) are incorporated in the HVL determination; thus, the estimate of entrance skin exposure for the patient depends on an accurate determination of the HVL of the incident beam.

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