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One success story with this technique was Safeway Stores (symbol SWY), shown in Figure 7.41. After a staggering rise in value, the stock started softening, and it fell beneath support in the rst half of 1999. In a few months, it had recovered some and was pushed up against the underside of its trendline. A short sale at that point would have yielded marvelous pro ts, since the stock was exhausted and didn t attempt such an assault on its trendline again. A close-up view of this event is shown in Figure 7.42, which also highlights how one must be somewhat discerning when watching price action around trendlines. On the very rst day of August, prices just barely peeked above the trendline. This did not mean that suddenly a new bull market was in place for the stock. Once the ascending trendline is broken, it cannot regain its stature as a reliable measure of upward price movement simply because prices manage to sneak to the other side. In this case, the trendline provided a valuable line in the sand that prices were prohibited from crossing. The prices did get across this line by a few pennies, but certainly not enough to stop looking at the short opportunity. This day in August established the high-water mark for the



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relocation, were addressed. The geotechnical investigation for the new lighthouse location included recommendations for site preparation and requirements for foundation support. Full-time testing and inspection was required in order to verify the continuity of subsurface conditions indicated in the geotechnical report and to monitor construction activities to verify that adequate foundation subgrade conditions were achieved. In addition to monitoring of the subsurface conditions, on-site geotechnical personnel provided in-place density tests of subgrade soils. The on-site monitoring provided information, on a continuous basis, to on-site personnel as to the motion and strains to which the lighthouse was being subjected and issue warnings if the established parameters had been approached or exceeded. Data was also compiled at three locations for various team members in Buffalo, Chicago, and Atlanta.

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f)', <p')Id(f)', <p', z)]

(3.5.19)

Equations (3.5.16) and (3.5.18) are the difference forms of the radiative transfer equations, while (3.5.17) and (3.5.19) are the differential forms.

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(1) The differential form of radiative transfer equations in (3.5.17) and (3.5.19) can be misleading since it suggests an equation of intensity changes at a point in space. However, as we see from previous sections, it is the wave equation which governs wave propagation in space. The result of the difference equation in (3.5.16) is obtained by assuming l D and >. < D lmfp. The conditions >. < D and l Dare necessary because in such a limit of a layer D, averaging can be taken over random particle positions and over a spatial extent of several to many wavelengths. The condition D lmfp is ne ~ded because it means that one can represent input and output relations of a thin layer D by the first- and second-order scattering solutions. Thus (3.5.17) has to be interpreted in the sense that the distance has been calibrated with the distance scale D. (2) In microwave remote sensing problems, usually A, l lmfp, so that it is possible to find a distance scale D such that >., l < D lmfp with the appropriate radiative transfer equation. However, in problems of strong localization, >. :::; [mfp, the distance scale D such that >., [ < D lmfp does not exist. (3) We are able to derive simple expressions for the phase function because of the isotropic scattering of the point particle models. In problems of complicated particle shapes and correlation of particle positions, it is generally difficult to analytically determine the phas ~ function. In Volume II, Monte Carlo methods have been employed to determine solutions

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