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It becomes time-consuming and tedious to go through the process of applying and adjusting these studies every time. For this reason, ProphetCharts provides for study sets. A study set is simply a collection of technical studies (including all of its computation and appearance parameters) housed under a name that you assign. You may, for example, create a study set named Three Moving Averages, and another one called Bullish Breakout System, and another called Bollingers with PSAR and MACD. What s important is that the names are distinct and meaningful to you, since study sets are your shortcut to applying what might otherwise be a very tedious application of settings. Creating a study set is done from either the Studies menu or the technical studies editor. In either case all you do, once you have set up the technical studies to your liking, is click Save Study Set (Figure 6.18). After you choose this option, a dialog box is presented (Figure 6.19) that lets you either enter a new name or save the set onto an existing name. The radio buttons in this dialog box control whether or not you are going to create a new study set with a new name (the default choice) or if you want to overwrite a previously-created study set (the second choice), in which case you ll need to choose the study set that you want to replace from the dropdown menu. Once you are done, you can click OK to save your study set.

where ( ) denotes ensemble average. The quantity MJ(O, T) is called the spontaneous magnetization. If it is nonzero the system is said to be ferromagnetic. Although a configuration of the system is specified by the N numbers Sl"" ,SN' the energy value (14.1) is in general degenerate. There is another wa~ of writing (14.1) that makes this manifest. In any given configuration of the lattice, let N + = total number of up spins N _ = total number of down spins

Outlook saves the information and displays the contact in the Contacts list. To edit contact details, you can double-click the contact to reopen the Contact window.

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Each nearest-neighbor pair is one of the three types ( + + ), (- - ), or (+ - ), where ( + - ) is not distinguished from (- + ). Let the respective number of such pairs be denoted by N ++' N __ , N +~. These numbers are not independent of each other, nor of N +' N _. A relation among them may be found as follows. Choose a particular lattice site with spin up and draw a line connecting it to all its nearest neighbors. There should be y lines drawn. Repeat this procedure for another site with spin up, and continue to do so until this is done for all sites with spin up. After the procedure is completed the total number of lines drawn is yN +. A construction of the kind described is illustrated in Figure 14.1 for a two-dimensional square lattice. The total number of lines drawn can also be counted by noting that between every ( + + ) pair there are two lines, between every ( + - ) pair there is one line, and between every ( - - ) pair there is no line. Hence yN + = 2N ++ + N +_. This relation remains valid if we interchange + and -. Therefore we have the set of relations

(14.7)

from which any three of the five numbers N +' N _, N ++' N __ , N +_ can be eliminated. If we choose to eliminate N +_, N __ , N ~, we have

(14.8)

2. N + N ++ -

If we compress a gas isothermally, it is supposed to start condensing at a point 0, as shown in the P- V diagram in Fig. 2.6. If we compress the system further, the pressure is supposed to remain constant. Actually the pressure will sometimes follow the dotted line shown in Fig. 2.6; along this dotted line the system is not

..,.

FIGURE 6.18 To preserve the technical studies you have used into a single set, choose Save Study Set from the Studies menu.

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