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The Town lattice requires a wide bearing surface for the truss so that bottom chord, lattice, and connections are not overstressed. The general rule of thumb is that the truss should extend beyond the center of the bearing equal to the depth (height) of the truss. Town lattice trusses usually terminate at a built-up end post. If the end of the truss is close to the bearing point, the endpost may greatly affect the forces in the lattice braces and counter braces. Bearing blocks, bed timbers and bolster beams can be con gured to enhance the capacity of a Town lattice truss. The Auchumpkee Covered Bridge in Thomaston, Georgia, was originally built with very heavy double-cantilevered bolster beams that tapered down in depth from their supports. These were reused in Arnold Graton s 1996 reconstruction of the bridge that had been destroyed in a ood. The tapered con guration is not only visually pleasing, it provides a gentle transition between the main span and the supports. A Town lattice truss will be substantially stronger if the chord sticks are as long as possible. By scattering the end joints in the bottom chord in a rational manner, there is less chance that a joint will fall precisely at midspan or at the most critical point in the bottom chord. A more subtle consideration is load



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where we have used a shorthand notation: 0== r a , 1 == rl, 2 == r2, and so on, and the integration is implied over internal arguments. In (4.2.27) through (4.2.29), Q(O,l) and 1(1,2; 1',2') are the ma..'lS and intensity operators, respectively. By using (4.2.27) through (4.2.29), we have

-{ (V 81/;(0))

+ (k 2 -

k*2) ('lj;*(O)'ljJ(O)) }

[(\72 + k 2)('lj)(0)'ljJ*(0')) - (\7'2

+ k*2) ('lj)(0)'lj)* (0'))]

= ('ljJ*(O))Q(O, 1)('lj)(I))

+ (G*(O, 1'))1(0,2; 1', 2') ('ljJ (2)'ljJ *(2'))





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There are many terms used for these phenomenons A rounded top, as the name suggests, is price action at the upper end of a chart, and it is sometimes called a distribution top or an inverted saucer A saucer, which is typically at the low end of a chart s recent price range, is also referred to as a rounded bottom, a basing pattern, or a dish pattern Tops and bottoms are not always as clean and neat as saucers and tops, so we will begin by examining the more fundamental price breakouts, which are the progenitors of saucers and tops A breakout is the escape from a price range bounded by a lower line (support) and an upper line (resistance) Figure 91 illustrates a breakout pattern in which the price action had been around $7 to $9 for many months.

+ Q(O, 3)(G(3, 1))(G*(O, 1'))1(1,2; 1', 2') ('ljJ(2)'ljJ* (2'))

FIGURE 15-6 The original doublecantilevered bolster beams were reused at the Auchumpkee Creek Covered Bridge.

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- Q*(O, 1)('ljJ*(I)) ('ljJ(0)) - (G(O, 1))1(1, 2; 0, 2') ('ljJ(2)'lj)*(2')) - (G(O, 1))Q*(O, 3)(G*(3, 1'))1(1,2; 1', 2') ('ljJ (2)'ljJ* (2')) (4.2.30) Next we apply the Bethe-Salpeter equation of (4.2.29) to the second and the fifth terms all the right-hand side of (4.2.30) RHS of (4.2.30)

= ('lj)*(O))Q(O, 1)(1['(1))

+ (G*(O, 1'))1(0,2; 1', 2')('lj) (2)) ('lj;*(2'))

+ (G*(O, 1'))1(0,2; 1', 2')(G(2, 3))(G*(2', 3'))1(3, 4; 3', 4') ('ljJ(4)'ljJ*(4')) + Q(O, 3)(G(3, 1))(G*(O, 1'))1(1, 2; 1', 2') ('ljJ(2)'lj)* (2'))

- Q*(O, 1)('ljJ*(I)) ('ljJ(O)) - (G(O, 1))1(1,2; 0, 2') ('lj)(2)) ('ljJ*(2')) - (G(O, 1))1(1,2; 0, 2')(G(2, 3))(G*(2', 3'))1(3, 4; 3', 4')('lj) (4)'ljJ* (4')) - (G(O, 1))Q*(O, 3)(G*(3, 1'))1(1,2; 1', 2')('ljJ(2)'ljJ*(2')) (4.2.31)

Next we examine the integrated optical relation which is a result of integrating over the coordinate in (4.2.30) and (4.2.31). Upon this integration, all the arguments on the right-hand side of the equation are integration dummy variables. These dummy integration variables are then interchanged. By keeping the arguments of the second and third terms unchanged and interchanging arguments for the rest of the terms in the integration of (4.2.31), we have

dO{ (\7 5\,,(0))

When prices broke above the resistance line in mid-June, the stock swiftly moved up several hundred percent 207.

+ (k 2 -

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