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In the backscattering direction, ks = -kid, so that Os = ()i and 1>s = 7f + 1>i. The scattering properties of the particles are described by the scattering amplitude f(&, 73) from direction 73 into direction &. Propagation in region 1 is described by the effective propagation constant K, which shall be approximated by K = k + iKel2, where k is the background wavenumber and is the same as the wavenumber of regions 0 and 2, and K e is the coherent wave extinction rate. The thickness of the slab can be normalized by the optical



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Clicking on Clone (Figure 2.20) will create another instance of ProphetCharts. To create extra charts, click the Clone button located in the lower-left corner of the applet for each new instance. The chart created will indeed be a clone of the original chart. Perhaps you don t want it to be identical, but instead you want to see the same symbol with a different style. If you do, instead of clicking on the word Clone, click the down-pointing arrow next to Clone. This will bring up a list of all the chart styles you have created, and you can choose any of them. This can be quite handy if you are closely monitoring a stock. For example, if you were looking at the past ve years of daily data on a stock, and you want to see live market activity on it, you might create a clone of the past two days on a minute-by-minute basis (Figure 2.21). If you had such a chart style available, clicking that style name would create a new chart with that style.

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Figure 8.4.1 Geometric configuration of the problem: a plane wave incident upon a slab of particles, the scattering properties of which are aniHotropic.

I(G(1", 1"'))1 2 = exp( -"'cl 1" - 1"'1)

167f 2 1r -

(8.4.3)

parallelogram shape indicating movement of the sides of the nave down in a vertical direction. The second explanation was that the sloping balconies themselves were exerting pressure on the exterior walls, causing them to crack at the balcony level and forcing the now-hinged wall to rotate outward. A sloped end condition would tend to push the exterior wall outward because

(8.4.4)

p(ii, f3)

= -11(ii, f3)1

(8.4.5)

We have covered a lot of ground in this chapter, including basic chart properties, different kinds of nancial instruments, viewing detailed data on a chart, searching for symbols, streaming, and cloning. In the next chapter, we will dig deeper into what else can contribute to a chart style and how we can save and manage these styles for easier, more productive technical analysis.

dii p(ii, /J)

J dii denotes integration over a solid angle 47f of direction ii. Let lin)

and I~n) denote, respectively, the nth-order ladder term and the nth-order cyclical term, and h and Ie denote, respectively, the sums of the ladder terms and the cyclical terms. The summation of ladder terms begins with n = 1, and the summation of cyclical terms starts with n = 2.

n ),

FIGURE 7-5 The sidewalls appeared to have settled, although diagonal settlement cracks were not visible.

(8.4.6)

~I~).

(8.4.7)

The first-order ladder term is, analogous to (8.2.16)

(1) 1L -

ProphetCharts has four areas that offer control: general settings, modules, menus, and the tool bar. The second of these, modules, will be covered indepth with this chapter. The module list is located on the left side of the ProphetCharts applet, and although it has a variety of functions, the principle is similar for each of them. That is, each module provides a list of choices, and each module can be either expanded or collapsed, depending on whether you are interested in it or not. You therefore can avoid cluttering your screen with items not currently of interest. Figure 3.1 shows what the module list looks like when all of the modules are collapsed: The arrows on the extreme left can be clicked to ex-

eiK 1') 1 '

(8.4.8)

(8.4.9) (8.4.10) (8.4.11) (8.4.12)

""e sec () . 2 '

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