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Only the real part of Mp(k, Klb) for p = 0 contributes. Also note that g(r) = 0 for r < b. Other real and imaginary terms are smaller than the corresponding real and imaginary terms of Lp(k, Klb). Thus, in the Rayleigh limit, only the knowledge of the integral of g(r) - 1 is required rather than a detailed behavior of the pair-distribution function g(r) as a function of r. Substituting the low-frequency approximation in (6.1.50) gives

FIGURE 17-1 The acrylic panels provided a weathertight sidewall closure. (See 17 for discussion of the Old Salem Covered Bridge.)



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[e(k 1Z )

[-h(k2Z )

J Jdk~Me(ku,k~) + Jdk~Mh(ku,k~)] J Jdk~M:(ka,k~)+e(2z) Jdk~Mh(ka,k~)]

F(ku - k-l)F(k-l - ku)F(k-l - ka)F(ki-l- k-l)

(1.1.65a)

This consists of four integrals over dk u dk~ dka dk~. That requires taking the average of the product of F's. From





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The neckline drawn on this chart clearly shows a left shoulder, a head, a right shoulder (which has a lower high the than the left shoulder, always a good sign), and then a break below the neckline When the price gains strength and retraces back to the neckline, it touches the neckline virtually to the exact penny and then swiftly falls away This is a superb example of the H&S pattern at its best The aftermath of the H&S that was shown in Figure 127 is actually pretty impressive, in spite of the neckline violation that took place As Figure 129 illustrates, the descent in price was quite rapid and relatively.

(F(k u - k~)F(k~ - kn)F(k: - ka)F(kn - k:)) =

6(ku - kn)W(ku - k-L)6(ka - kn)W(k a - k-L)

FIGURE 18-1 The aqueduct consists of three equal spans of 66 feet. (See 18 for discussion of the Tohickon Aqueduct.)

-II -

+ 6(ku -

ka)6(k-L - k-L)W(ku - k-L)W(k-L - kn )

+ k-L -

kn - ku)W(k u -k-L)W(k-L - kn)

(1.1.65b)

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The first term of (1.1.65b) is that of the coherent wave. The second and third terms are proportional to 6(k u - k a ). We can subtract out the coherent intensity to form the incoherent intensity. That means we only include the second and third terms of (1.1.65b) with ku = ka. We have incoherent field (1.1.66) The power per unit area associated with the second-order incoherent field is

FIGURE 12.9 In spite of the imperfect behavior around the neckline, the H&S pattern performs well in this instance.

! Re (z .[~2) (r)

FIGURE 18-7 The completed aqueduct won a National Timber Bridge Award in 2002. (See 18 for discussion of the Tohickon Aqueduct.)

x\7 x~~2)* (r) )

2~ Re{l dk-L z . k dk~ W(k-L - k~)W(k~ x [IMe(k-L, k~)12

+ Me (k-L , k~)JvI:(k-L, -k~ + k n + k-L)

(1.1.67)

+ IJvh(k-L, k~)12 + Jvh(k-L, k~)Jvlh(k-L, -k~ + kn + k-L)]}

where J dk-L denotes integration over propagating waves only. In (1.1.67) the p coherent intensity has been subtracted out to form the incoherent intensity. The first two terms in the square bracket in (1.1.67) correspond to horizontally polarized scattered waves and the third and fourth terms correspond to vertically polarized waves. The first and third terms in the square bracket of (1.1.67) correspond to the second term of (1.1.65) while the second and fourth terms in (1.1.67) correspond to the third term of (1.1.65). Converting to angular integration as done in (1.1.42)-(1.1.44), we can calculate the bistatic scattering coefficients. Thus the horizontally polarized scattered wave bistatic coefficient is

ki-L)

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