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(Pt!C j lp2) = e- i (P\-P2) r/ C p(P1,P2)

(5.3.55)

(5.3.56a)

(5.3.56b)

3.4 Coherent Potentict.l (CP)

(5.3.56c)

dfj CjE(C)

(5.3.57)

covered bridge built at Old Salem. This paper will discuss the development of the design for the Old Salem Bridge and the application of covered bridge technology to both the preservation of historic structures and the construction of modern transportation structures.



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From (5.3.57) it can be concluded that no J dfjC j is the mass operator for discrete scatterers under the quasi-crystalline approximation. For a sparse concentration of scatterers, it is reasonable to assume that the particle positions are independent of each other. The conditional probability p(rjlrl) can be approximated by p(rjlrt} = p(rj) = I/V~o that the pair correlation function becomes g(r) = 1, and h(r) = 0 and H(p) = o. It follows then that (5.3.56) gives





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cheap. That is simply a result of the prices being adjusted to take account of the splits. If the chart showed the actual price for every day of the stock s history, the chart would be useless for a technician, because it would have huge gaps in the price every time a split took place. Using split-adjusted data is essential for analyzing the chart, which explains why a stock that traded for $75 in 1974 might show up with a price of $1 during the same timeframe when you examine its graph in the present day. As you have read earlier in this book, the length and strength of a pattern are often related. 3M Corporation provides a remarkable example of a very large cup with handle pattern and its resulting price movement. Figure 10.4 shows a cup being formed from 1974 through 1983 and a handle being formed from 1983 to 1986. Although this is an exceptionally wellformed pattern, even a pattern this good isn t smooth. We are, after all, not looking at a drawing of a physical cup. This is price movement measured over thousands of days, so you can expect a relatively high amount of noise. The experienced chartist learns to lter this out so the pattern is easy to discern. The resistance (on a split-adjusted basis) was at about $1.03, which was hit in 1974, 1983, and 1986. Figure 10.5 shows one of those kinds of charts that make a person wish for a time machine 3M increased eighty- ve fold in price. A $10,000

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(5.3.58a) (5.3.58b)

C p (Pl,P2) = T p (Pl,P2)

in this limit. Hence the dispersion relation of QCA of (5.3.51) reduces to that of EFA if we set g(r) = 1.

3.4 Coherent Potential (CP)

The idea of coherent potential (CP) originates from the observation that in the derivation of the multiple scattering equations, the background medium dyadic Green's operator is used. The potential operator U is proportional to k~ - k 2 and is a measure of the difference in permittivity from the background medium. However, as the concentration of particles increases, the coherent wave will be propagating in an effective medium K, and the scattering potential is a result of the difference in wavenumber from K rather than k. The idea of coherent potential is to introduce the Green's operator with wavenumber K and is analogous to the nonlinear approximation in random medium theory of 4. Consider the N-particle scattering equation,

(5.3.59)

Suppose that the basic equation (5.3.59) is rewritten by adding and sub-

Why build a covered bridge at Old Salem As a tourism destination, Old Salem needed a pedestrian overpass structure to enhance and blend with its cultural landscape and historic architecture. The choice of a covered bridge conforms to the traditional technology of covered bridge building in North America. At the same time, it was important to Old Salem planners, such as John Larson, that the structure not be mistaken for an original artifact. To differentiate, the bridge is clad with transparent panels that give a modern appearance while exposing the traditional interior construction.

tracting an operator now(p) on the left-hand side of the equation. Then,

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