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a factor of 10 50. The disadvantage of this method is that most of the mass spectral information for the component is lost. This is not much better than having a gas chromatograph with a ame ionization detector. For, in trace-level work, any component that has an ion with the same mass as the one being scanned and the same retention time will be mistaken for the component of interest. These small peaks are called chemical noise. On the other hand, with a tandem (dual-stage) mass spectrometer system, the chemical noise can be reduced almost to zero, lowering the limit of detection signi cantly. In tandem mass spectrometry (as the name implies), a second mass spectrometry stage is added to the rst. This allows the analyst to select one of the fragment ions from the rst mass spectrum for further fragmentation. Now, we have a mass spectrum of an ion, whereas in single-stage mass spectrometry we have a mass spectrum of a molecule. Recalling the discussion earlier about selected ion monitoring, one can now apply this same principle to tandem mass spectrometry. With this technique, one selects the most abundant fragment ion from the rst mass spectrum for secondstage fragmentation. This is called the parent ion. A mass spectrum is obtained; from this spectrum, one selects the most abundant ion to monitor in the same manner as SIM. This is called the daughter ion. Now, when the sample is chromatographed, only those peaks will show up at the desired retention time that contain the daughter ion originating from the parent ion that was selected from the original mass spectrum. This greatly reduces the signal background or chemical noise. F.1.19 X-Ray Fluorescence (XRF)

How Radar Works The radar scanner rotates at approximately 24 revolutions per minute, and while it does this, it transmits pulses of microwave energy. The time interval between each pulse is long enough to allow a pulse to travel out to the maximum range of the radar and back to the scanner. This means that the radar is listening for about 99.9% of the time and transmitting for less than 0.1%. Although each pulse may be 2 or 4 kilowatts, the average power is only 2 to 4 watts. Measuring Range If one of these pulses strikes a solid object the pulse is re ected back to the scanner and the time taken for the return journey is used to calculate the distance of the target from your boat.

See for an interesting overview and comments: http://online.anu.edu.au/people/Roger.Clarke/SOS/ Asimov.html.

P1: KOA/FFX WY050-05

Figure 7.2 Gaussian noise samples demodulated from a (notional) carrier. [Source: Meikle, H.D., Modern Radar Systems, Norwood, Massachusetts: Artech House, 2001.]

Figure 26.9 Commonly obtained data from 3-D multiple sclerosis (MS) CAD results. The data include the original 3-D MRI data set: (A) MRI FLAIR image; (B) CAD detected multiple lesions; (C) radiologist identi ed lesions (normally not shown in the results, depicted here for comparison purpose only); (D) color-coded MS lesions on a 2-D image; (E) on two slices; (f ) on all slices; (G) quantitative results of all 26 lesions detected by CAD; (H ) three oblique views of 2-D images with all 26 MS overlaid. Green color shows the ventricles. (Data: courtesy of Drs. A. Gertych and B. Guo; and Guardian Technology, Inc.)

dual-frequency performance of the antenna with various slot dimensions. From the results, it is observed that, although all the dimensions of the V-shaped slot can affect the dual-frequency performance, the higher operating frequency f 2 is most sensitive to a variation in the distance ds between the slot s upper edge and the patch edge. On the other hand, the lower resonant frequency f 1 is relatively insensitive to variations in the slot dimensions. By varying ds from 5 to 16 mm in the present design, dualfrequency operation with a frequency ratio in the range 1.488 1.834 is obtained. For a xed value of ds , one can ne tune the dual-frequency operation by adjusting the dimensions ( 1 , 2 , w 1 , w 2 ) of the V-shaped slot.

The table shows the relative risk of various cancers, in men and women with BMI 35 40 kg/m2, as compared with the normal-weight population with BMI 18.4 24.9 kg/m2. Adapted from Calle et al. (2003).

12

When the equations together with their boundary conditions cannot be solved explicitly, and no analytical solution is available, a numerical solving scheme must be implemented The solving schemes belong to two main categories: deterministic and stochastic In the rst approach, the charged particles in the semiconductor are approximated by a singleparticle gas, where the motion of each particle is driven by deterministic forces that are the same for each particle in the gas; all particles in the gas are identical In some cases, the charged particles are approximated by two gases, one for high-energy and one for low-energy particles The equations are solved once by exact calculations (in numerical sense), and the macroscopic quantities of interest are computed for the whole gas.

xz = [cos(ws,) sin(ws,) cos(2wsn) sin(%s,).