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HIGH-ENERGY X-RAY FLUORESCENCE of this sample using the L lines, as can be seen in Figure 5.5.9(b). In addition, without such light elements, possibly 14 rare earth elements (from La to Lu except for Pm) and 42 peaks (L , L 1 , and L 2 lines for each element if we neglect the L line) are present in the XRF spectrum within the small energy region of 5.288 keV (=9.938 4.650). In contrast, in the energy region above 20 keV, there are no peaks other than the K lines of the heavy elements. Moreover, the energy difference between La K 1 (33.4418 keV) and LuK 1 (52.3889 keV) is ca. 19 keV, which is large enough to distinguish each rare earth element under the resolution of a pure Ge SSD, as is demonstrated in Figure 5.5.9(a). Certi ed values for the rare earth elements have not been reported for SRM612 glass, but information values (in ppm) are given as follows: Ag(21), Ba(41), La(36), Ce(39), Nd(36), Sm(39), Eu(36), Gd(39), Dy(35), Er(39), and Yb(42). The intensity of the peak of each element in Figure 5.5.9(a) appears to be qualitatively consistent with these information values. This suggests that the present technique is applicable for the nondestructive total determination of rare earth elements as well as for other heavy elements, such as Hf and Ta, at the ppm level.19

To nd this point, consider what happens to the impedance along the transmission line Along the transmission line, the amplitude of the re ection coef cient remains the same, because the amount of re ected power remains the same, but the phase relationship between the re ected and incident elds changes constantly Thus, the total electric eld and the total magnetic eld change, so the resistive and reactive components of the impedance change This is illustrated in Figure 318 The mismatch does not improve along the transmission line, but a point exists where the resistance is exactly equal to Z0 At that point a capacitance can be added to cancel the inductance.

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The while loop allows you to iterate through a block of code multiple times until a defined condition is met. The format of the while loop is:

unmanageable That s why corporate nancial statements are consolidated from the statements of divisions, subdivisions, and smaller and smaller organizational units Yet until very recently this could not be easily done with simulations: Their results could not be added up I will explain this property of simulations more precisely in later chapters, but for now let s return to the ladder analogy Consider a rm that has two divisions, each facing its own uncertainties We will model each division as its own ladder, and model the entire rm as the two ladders joined by a wooden plank Now suppose that by shaking either ladder by itself you would predict a 10 percent chance of its falling over A reasonable estimate of the chance of both ladders falling over at once is 10 percent times 10 percent, or 1 percent.

But when the two ladders are connected by the plank, all bets are off Now if either ladder falls, the plank may drag the other ladder down with it Thus, the chance of both falling at once goes from 1 percent to more like 20 percent! To simulate the entire enterprise, you can t simply shake each ladder individually and add up the results Instead you need to assemble both ladders and the plank rst, then shake the whole thing, as shown in Figure 31 But, again, as with the single gargantuan nancial statement spreadsheet, this just isn t practical for a large organization, let alone for a whole industry.

In The Failure of Risk Management: Why It s Broken and How to Fix It (Wiley, 2009), Doug Hubbard notes this problem as follows: [T]he lack of collaboration within rms makes another important step of risk management 5 almost impossible a cooperative initiative to build models of industrial, economics and global risks across organizational boundaries..

-nB(Tc)

Moving along the transmission line, the amplitude of the re ection coef cient remains constant, because the re ected power stays constant, so the move is represented as traveling around the constant r circle, that is, the constant re ection coef cient circle This traveling is equivalent to rotating around that circle, and the phase of the re ection coef cient, and therefore the impedance, changes Matching is achieved by moving along the transmission line to the intersection of the r circle and the unity-resistance circle At this intersection, the resistive part of the impedance is 50 V and the inductance can be canceled with a matching capacitance A summary of the matching procedure follows: 1 Locate mismatch on the Smith Chart 2 Determine wavelength position of mismatch 3 Move down the transmission line toward the generator until the p circle intersects the unity-resistance circle..