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Figure 2.3 Global prevalence of obesity in men in 2005 showing the percentage of adults with BMI 30 kg/m2 in each country (upper panel). Data are age-standardized to WHO world population. Predicted prevalences in 2015 are shown in the lower panel. Maps available at www.who.int/globalatlas. Reproduced with kind permission of the WHO.

Appendix B Binding Atomic energy mass (MeV) (umu) 0 0 2.225 8.482 7.718 28.296 31.995 39.245 41.277 37.6 56.5 58.165 1.0086649 1.0078250 2.0141018 3.0160493 3.0160293 4.0026033 9 F 17 128.22 17.0020952 6.0151223 7.0160040 8.0224867 7.0169292 8.0053051 9.0121821 10.0135337 11.0216577 8.0246067 9.0133288 10.0129370 11.0093055 11 Na 21 163.076 20.9976551 12.0143521 10.0168531 11.0114338 12.0000000 13.0033548 23 181.725 22.9941249 24 198.257 23.9850419 25 205.588 24.9858370 26 216.681 25.9825930 27 223.124 26.9843407 28 231.628 27.9838767 34 285.566 33.9737620 35 298.21 37 317.1 34.9688527 36.9659026 36 306.789 35.9683069 38 323.208 37.9680106 39 331.282 38.9680077 22 174.145 21.9944368 23 186.564 22.9897697 24 193.523 23.9909633 25 202.535 24.9899544 26 208.151 25.9925899 10 Ne 18 132.153 18.0056971 15 P 19 143.781 19.0018798 20 160.645 19.9924402 21 167.406 20.9938467 22 177.77 21.9913855 23 182.971 22.9944673 24 191.836 23.9936151 16 S 30 243.685 29.9849030 31 256.738 30.9795544 32 271.781 31.9720707 33 280.422 32.9714585 34 291.839 33.9678668 35 298.825 34.9690321 36 308.714 35.9670809 37 313.018 36.9711257 29 239.285 28.9818014 30 250.605 29.9783138 31 262.917 30.9737615 32 270.852 31.9739072 33 280.956 32.9717253 18 137.369 18.0009377 19 147.801 18.9984032 20 154.403 19.9999813 21 162.504 20.9999489 Z A Binding Atomic energy mass (MeV) (umu) Z A Binding Atomic energy mass (MeV) (umu)

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We have seen that MS analysis of components of complex samples may be complicated by selective desorption of sample components at rates dependent, for example, on their surface activity (Section 4.1.3). By rst fractionating samples by HPLC ( 2) and following this with MS analysis, we can combine high-resolution chromatographic separation with high-resolution analysis (i.e. mass determination). This is called HPLC/MS or LC/MS. In such a system, MS can be regarded as essentially a detector for the LC system, but one which gives useful structural information about each component of the sample. An outline of the experimental arrangement used in LC/MS is shown in Figure 4.21. Although a variety of chromatography modes are possible for LC, in practice reversed phase chromatography

*CLOP P s = ( T )

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Note that this expression has a factor of cos2f, which is not included in the timeaverage holographic vibration fringes given by Eq. (16.39). The cos2f term is due to the phase of the speckles, and causes the secondary fringes to be noisy. For a sinusoidal object motion, Eq. (16.51) can be rewritten as

(3.10)

Lightness J is calculated from the achromatic signals of the sample and white using Equation 15.24. J = 100(A/Aw)cz (15.24)

The list isn t in 3NF because it violates the 3NF rule:

Tkinter can handle sophisticated GUIs without much trouble. You can use the layout managers and event handler to get your program s appearance and behavior just right. In this chapter, you: Handled various events. Created advanced widgets and dialogs. Used custom mouse cursors. In the next chapter, you learn all about the Curses module a good user interface choice for terminals on which graphics (and hence Tkinter) aren t available.

Room/FirstName/LastName and FirstName/LastName/Phone/CellPhone are the possible candidate keys. CellPhone can uniquely identify a row if it is not null. If CellPhone is null, we know Phone is not null because all students must have either a room phone or a cell phone. But roommates share the same Phone value so we need FirstName and LastName to decide which is which. (Basically Phone/CellPhone gets you to the Room.)

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In order to calculate an electron density map the intensity of each Bragg re ection, Ihkl , is converted into a structure factor, Fhkl (note; since this is a vector quantity on the Argand diagram, it is conventionally written hereafter in bold type). This has an associated amplitude (Figure 6.46; Section 3.1.1) denoted hereafter by |Fhkl |. These intensities, Ihkl , are directly measured by the detector (or recorded on photographic lm and then converted into intensity as

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