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Microsoft Word offers you several ways to control how you view your document. For example, the Zoom tool enables you to control the magnification of your document. You can change the zoom setting by using the Zoom slider or the Zoom buttons. You can also choose from five different views: Print Layout, which displays margins, headers and footers; Outline, which shows the document s outline levels; Web Layout, which displays a Web page preview of your document; Full Screen Reading, which optimises your document for easier reading; and Draft, which omits certain elements such as headers and footers.

(t > 0) (t < 0)

(17.42)

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It is also helpful, after a channel violation, to watch for the formation of new patterns, since the channel by de nition has become a pattern of the past. Looking at Figure 8.13 once again, the prices formed a clear topping pattern spanning nearly a year once prices cut beneath support in October. In addition, you can see prices moving from $36 to $46 even after this pattern failure, since prices were clinging to the underside of the former support line before they succumbed to the new pattern s direction. Another interesting thing about channels is that they often represent temporary changes in trend. Figure 8.14 offers a real-life example. At the beginning of the chart, the stock was moving down badly, descending from $15 to $8.50 per share. Following this weakness, the stock began a countermove lasting nearly two years, and the prices nearly tripled. Once the channel was broken, the descent in prices began anew. What s particu-

from which we deduce that the heat capacity has a finite discontinuity at t = 0:

(t> 0) (t < 0)

(17.43)

To obtain the correlation length in the same approximation we consider the response of m(x) to a "test source" H(x) = -;\8(x), with ;\ ~ eventually. Thus

+ uom 4 + ;\m(x) 8(x)] (17.44)

Note that we have replaced l'Vml 2 by -m'V 2m by performing a partial integration, discarding the surface term at infinity on the assumption that m ~ at infinity. The saddle-point approximation now leads to a partial differential equation:

(17.45)

In this example, Draft view displays the text without graphics or other elements. You can also switch views using the View buttons at the bottom of the program window.

For t > 0, the solution in the absence of source is m = 0. Hence we expect m(x) to be of order ;\, which is supposed to be the smallest parameter in the equation. Thus we can neglect the cubic term and solve the equation by taking Fourier transforms of both sides, obtaining, in the notation of (17.9),

FIGURE 8.14 This channel was entered into when the stock was much weaker. The channel represents a time of consistent strength.

m(k) =

m(x)

;\j(dk):

---.

(17.46)

~ = ro- 1/ 2 =

(a ot)-1/2

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