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16.2 Referring to the sketch, approach the critical point along BC (i.e., t equation of state, i.e., the density n as a function of p.

16.3 Continuing with the last problem, approach the critical point separately from the gas and from the liquid phases at t < 0 (paths Ie and 2C in the sketch). The paths are shown in the P-T diagram in the accompanying sketch. Assume that the Gibbs free P

T 678.86

0.649 1.577 2.776 0.845 1.535 2.215 3.665 5.034 6.145 7.211 6.099 9.287 11.793 13.945 15.405 16.474

T 614.41

19.43 20.00 20.77 21.67 22.36 22.89 25.34 25.83 26.40 26.83 27.21

FIGURE 8.5 This is a more extreme example of showing the future, since this Fibonacci time series has its next data point decades away.

4,160 10,070 17,775

1,820 3,230 6,015 10,070 14,210 17,775

Note: You can also move an object by cutting it from its current location and pasting it in the desired spot. For help, refer to the section Cut, Copy and Paste Data in 2.

2,290 4,160 6,015 10,070 14,210 17,775 21,315

3,230 6,015 10,070 14,210 17,775

1,355 3,230 6,015 10,070 14,210 17,775

number per unit mass (emu/g). hFrom P. Weiss and R. Forrer, Ann. Phys. (Paris) 5,153 (1926). The data have been reanalyzed by J. S. Kouvel and M. E. Fisher, Phys. Rev. 136, A1626 (1964). They obtained the following critical exponents: y = 1.35 0.02, 8 = 4.22.

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energy of the fluid has a singular part satisfying separate scaling forms in the two phases:

where p (t) are the values of (P - Pc)/P along the paths. Close to transition line and near t = 0, we can take them to be the same linear function of t: p (t) "" ct, where c is a constant. Show how the latent heat varies with t.

In 7, you learned how to use and draw trendlines. The tool next to the trendline tool, which is the channel tool (Figure 8.6), lets you draw two parallel trendlines easily in order to bound price data in a channel pattern. Channel patterns are rarer than trendline patterns, simply because it is much easier to nd prices bouncing off a consistent support or resistance level than it is to nd prices bouncing within both support and

16.4 The accompanying graph shows the magnetization M vs. magnetic field H for nickel, as measured by Weiss and Forrer in 1926. Some numerical values are listed in Table 16.6. Given that T,. = 627.2 K, f3 = 0.368, and 8 = 4.22, select data from a few temperatures above and below T, to verify the scaling form

M - ItIPJ( (H/ltIP8)

614.41 616.30 618.18 620.06 621.94 623.82 625.69 627.56 629.43 631.30 633.16 635.00

After you insert an object such as a piece of clip art or a photo from your hard drive into a Word document, an Excel worksheet, a PowerPoint slide or a Publisher brochure, you may find that the object appears upside down or inverted. To rectify this, you can rotate or flip the object. For example, you might flip a clip art image to face another direction or rotate an arrow object to point elsewhere on the page. Alternatively, you might rotate or flip an object that you place in an Office 2010 file simply to change the appearance of that object.

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