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that children born in the early twenty rst century may have their life expectancy shortened as a result of the escalating epidemic of obesity. Among obese children, the overall lifetime risk for developing type 2 diabetes may now be as high as 33%, rising to 50% among certain ethnic minorities in the USA, while life expectancy may be reduced by up to 13 years because of diabetes (Olshansky et al., 2005).

Figure 8.14 Genetic obesity syndromes in rodents related to leptin and the proopiomelanocortin (POMC) neurones in the hypothalamus, which are important in mediating leptin s appetite-suppressing action.

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x + m4) + 3 sin( m 4 - x)],

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The drawing used in the following exercise on editing solid faces, ab24-11.dwg, is in the Results folder on the CD-ROM.

Figure 6-12: PDFMaker offers many features from Office applications not available from other PDF creators.

141 INTRODUCTION The single biggest change in all types of instrumentation over the past 30 years or so has been the integration of computers into the measurement system Interferometry is no exception, and the prime manifestation of this situation has been the development of phase shifting interferometry (PSI) Unlike many of the techniques discussed elsewhere in this book, PSI is not a speci c optical hardware con guration, but rather a data collection and analysis method that can be applied to a great variety of testing situations While the analysis of static interferograms has bene ted from computerization, it suffers from the need to nd fringe centers, and the resulting trade-off between precision and number of data points Data is collected only along the fringe centers, and most analyses need the data on a regular grid, therefore requiring interpolation.

10000 170 30 1100 330 400 100 1600 13 37 4 1100 390 390 7100 200 300 280 470

This low spatial sampling along the fringe centers also limits the lateral resolution of the method With a static interferogram, an additional piece of information is also required to determine the polarity of the wavefront PSI electronically records a series of interferograms while the reference phase of the interferometer is changed The wavefront phase is encoded in the variations in the intensity pattern of the recorded interferograms, and a simple point-by-point calculation recovers the phase The need to locate the fringe centers is eliminated, as are the associated problems While the earliest reference to this technique dates back to 1966 (Carre, 1966), the development of PSI techniques really began in the early 1970 s (Crane, 1969; Bruning et al 1974; Wyant, 1975; Johnson and Moore, 1977; Hardy et al 1977; Stump, 1979; Bruning, 1978; Moore, 1973; Massie, et al 1979).

calculated eigenmodes regarding to the two dioptric powers of the thermal lens of Nd:YALO are shown in Fig. 3.33. The design of this resonator is to be found in the peculiarities of PCRs: The degeneracy of modes in PCRs can lead to eigensolutions that build focuses on surfaces of the optical elements in the resonator which would lead to damage of these elements. This resonator design with a pinhole at the position of the beam waist and the rods aperture as second mode-selecting aperture does not allow for other than the transverse fundamental mode to come above threshold [66]. It particularly does not allow for any mode with a focus on one of the SBS-resonator elements. The mode diameter on the start resonator mirror is less crucial since the intensity in this resonator part is low. Furthermore, this set of apertures lifts the mode degeneracy in a way that a large transverse fundamental mode volume is realized, since this is the eigensolution with the lowest round-trip loss. The SBS resonator is not an ideal PCR. To some extent, it is an SBS-PCR as discussed in Section 6.3 with a mode injected from the start resonator. This mode is more or less perturbed compared to the eigenmode of the SBS resonator. But guaranteed by apertures the eigenmode of the SBS resonator is close to the one of the start resonator. The pinhole in the resonator acts at least partially as a spatial lter. A fraction of the lens duct will have a focal length equal to the distance between laser rod and pinhole. Therefore, in addition to the condition of matching the curvatures at