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There are some instances relatively rare when price action is bound by two parallel trendlines: one below as support, and the other above as resistance. We will explore these channels in 8, but for now, let us see how to use the Trendline tool to track these channels. When you right-click on a trendline, one of the choices in the popup menu is Duplicate. Choosing this creates another trendline right next to the selected one (Figure 7.43), and the trendline will be the same length, color, and angle as the selected original. The handles of the duplicate will be preselected so you can move it immediately to the desired location. You do not have to leave the duplicate trendline parallel, since either of the two handles can be moved. But the most practical value of the Duplicate command is to create a parallel trendline for the purpose of drawing a channel pattern. As shown in Figure 7.44, dragging the parallel trendline to its destination makes the formation of a channel pattern simple.

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::::::

(15.145)

narration, recording, 146 Navigation pane, 155 New command, 14 New Quick Style, 56 Normal view (PowerPoint), 129, 144 notes, adding, 195

1 (K)

::: 1

Tc '

= 0.4406868

(15.146)

kTc = (2.269185)

FIGURE 7.43 Choosing the Duplicate function creates a parallel trendline of the same length and style with its handles preselected.

e- / kT,

(15.147)

~c,(O, T) = ~(:;J[ -log 11 - ~ I+ log (~:,) -

Page Break button, 67 page breaks, inserting, 67, 101 Page Layout tab, 52 page numbers, 66, 67

(15148)

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It approaches infinity logarithmically as IT - Tcl ~ O. A graph of the specific heat is shown in Fig. 15.6, together with the results in the Bragg-Williams and the Bethe-Peierls approximations for comparison. It is seen from (15.138) and (15.145) that the internal energy is continuous at T = Tc Thus the phase transition at T = Tc involves no latent heat.

= 2.88

L-~~_ _

/ / / / / /

FIGURE 7.44 Drag the parallel trendline to an appropriate location to form a channel pattern, which consists of two trendlines.

Fig. 15.7 Spontaneous magnetization of the two-dimensional Ising model. The curve is invariant under a reflection about the dotted line.

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To justify calling the phenomenon at T = Tc a phase transition, we must examine the long-range order, i.e., the spontaneous magnetization. This cannot be done within the calculations so far outlined, since we have set B = 0 from the beginning. To calculate the spontaneous magnetization we have to calculate the derivative of the free energy with respect to H at H = O. This calculation, carried out by Yang, * is as complicated as the one we have presented. The result, however, is simple. Yang shows that the spontaneous magnetization per spin is (T> (T<

(15.149)

*c. N. Yang,

page orientation, 100 page ranges in indexes, 69 page setup, 100 101 Page Setup dialog box, 53 panes (PowerPoint), 129 Paste button, 25 photo album presentations, 124 125 Picture Effects button, 35 pictures adding to slides, 140 compressing, 27 cropping, 32 33 editing, 34 35 inserting, 26 27 PivotTable view (Access), 159 PowerPoint adding objects to slides, 140 141 slide text, 132 text boxes to slides, 139 changing font, 134 137 slide layouts, 131 views, 128 129 creating presentations, 126 127 editing text, 133 inserting slides, 130 moving slide objects, 142 photo album presentations, 124 125 recording narration, 146 reorganising slides, 144 145 resizing slide objects, 143 running slide shows, 148 149 setting line spacing, 138 setting up slide shows, 147 presentations, 124 127, 137 presets, 41 Preview area, 49 primary key, 167 Print command, 20 Print Preview button, 21 Print Preview view (Access), 183

Phys. Rev. 85, 809 (1952).

The term critical phenomena refers to the thermodynamic properties of systems near the critical temperature Tc of a second-order phase transition, or near the critical point of a gas-liquid transition The term "second-order" is used here in the sense of "not first-order" We shall model after the Curie point in a ferromagnetic system The two phases on either side of the critical temperature have different spatial symmetries Above the critical temperature, where there is no magnetization, the system is rotationally invariant Below the critical temperature, when spontaneous magnetization occurs, the magnetization vector defines a preferred direction in space, destroying the rotational invariance Since a symmetry is either present or absent, the two phases must be described by different functions of the thermodynamic variables, which cannot be continued analytically across the critical point.

.net ean 13 reader

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You may know how pqScan . NET barcode scanner software read EAN - 13 barcode from image; you may get APIs for reading EAN - 13 in . NET application.

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