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distance d between point A and the feed position increases with increasing loading resistance. In this experiment, the slot length was selected such that the required antenna length L for operating in the 800-MHz band was less than 0 /8. The antenna height was chosen to be less than 0.01 0 for low pro le. In this case, modi ed PIFA parameters were selected as L = 40 mm (about 0.115 0 ; 0 = 34.88 cm at 860 MHz), W = 25 mm, = 20 mm, w = 2 mm, and h = 3.2 mm (about 0.0092 0 ). Figure 3.42 shows the measured return loss for the modi ed PIFA with various loading chip resistors. The case denoted R = 0 is for the modi ed PIFA with a shorting pin. Table 3.9 lists the resonant frequency and impedance bandwidth for a modi ed PIFA with various loading resistances. The results for a regular PIFA (no slot in the patch and R = 0 ) are shown for comparison. It is clearly seen that, by meandering the patch, the resonant frequency of the PIFA is reduced to 872 MHz, about 0.67 times that (1298 MHz) of a regular PIFA. However, due to the antenna size reduction, the impedance bandwidth is decreased from 0.9% to be 0.6% for the modi ed PIFA with R = 0 . This smaller impedance bandwidth is due to the thin air-substrate thickness here. It is also observed that, with increasing loading resistance, the impedance bandwidth is signi cantly enhanced. For the case with R = 6.8 , the impedance bandwidth is 11.2%, about 12.4 times that (0.9%) of a regular PIFA. It is also seen that the feed position for impedance

The drawing used in the following exercise on creating boundaries, ab16-e.dwg, is in the Drawings folder on the CD-ROM.

with type 2 diabetes, dyslipidaemia and cardiovascular disease ( 10). Worsening obesity is also accompanied by increasing ectopic triglyceride deposition in the liver and in skeletal and cardiac muscle, and appears to contribute to cardiometabolic risk (s 11 and 12). Conversely, weight loss is accompanied by shrinkage of the expanded fat depots. Certain factors preferentially decrease visceral depots, including exercise, caloric restriction, the antiobesity drug rimonabant (apparently a speci c effect of cannabinoid CB1 receptor blockade) and bariatric surgery. This may explain why these treatments improve insulin sensitivity and cardiovascular risk more than might be expected for the degree of weight loss. Various diseases can modify the distribution of body fat. Inherited and acquired lipodystrophies are characterized by the failure to develop, or the loss, of fat in speci c distributions. The anatomical predilection of these conditions is unexplained. For example, all adipose tissue is absent from birth in congenital generalized

A close-up of this interface is shown in Figure 1453(b) Because of refraction, the test beam is incident on the part at a large angle For a 417 angle of incidence and an index of 15, the angle of incidence at the test surface is 86 This is close to the critical angle of the prism There are two bene cial consequences to this con guration First, the sensitivity of the test is reduced by the cosine of the angle of incidence At 86 , the sensitivity is 7% of the normal incidence sensitivity; a fringe represents 7 waves of surface height change instead of a half wave It is as if the surface is tested with a longer wavelength.

175 meters to 780 meters (usually for FDDI)

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The second bene t is that almost everything, including a ground surface, is highly re ective at this angle of incidence, and a variety of different materials and samples can be used If the angle of the light in the prism is slightly changed, the optical path length in the air gap will change much more than the path in the glass This tilt when used produces the phase shift between the reference and test beams Systems are available with up to a 200 mm aperture, and have been applied to testing silicon wavers and machined or ground parts The clear drawback to a system such as this is the need for the large precision glass prism.

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Distance measuring interferometers (DMIs) are capable of providing position readout with a resolution of better than a thousandth of a wavelength (less than a nanometer), and have found extensive use in the area precision machine control (Dukes and Gordon, 1970; Steinmetz et al, 1987; Smythe et al, 1987; Steinmetz, 1990) Most DMIs use heterodyne techniques (Section 14143), and a basic system is diagramed in Figure 1454 The two output frequencies from the source are orthogonally polarized, and the polarizing beamsplitter splits the frequencies into the reference and test arms of the interferometer The two corner cubes return these two beams to the detector, where the polarizer at 45 allows them to interfere.

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