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The total equity is equal to $1,350 $50 + $1,500 = $2,800 Because the position is still open the trading power of the account is determined as total equity less the total initial margin on all open positions The trading power $2,800 $1,350 = $1,450 permits us to buy one more contract than the one we already have As events develop further this clearly makes sense The first part of.

This assumption is so powerful that it is often invoked in the hope that it will be good enough for a rst approximation, despite the fact that it is a poor match for the full physical reality The area of turbulent study that holds the greatest interest for engineers is turbulent shear ow This ow is a modi cation of completely homogeneous ow to allow for shear stresses and mean velocity gradients Usually, one or two of the Reynolds shearing stresses are zero Turbulent shear ow in turn may be divided into ows that are nearly homogeneous in the direction of ow and those that are inhomogeneous in the direction of ow It has been found experimentally that the nearly homogeneous ows are those that are bounded, as in pipe ow, while the inhomogeneous shear ows are unrestricted systems, such as jets.

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It can be seen from Equations 2.34 to 2.37 that, if l = 0, the equations will be identical to the corresponding equations for the explicit method and will become those for the implicit method if l = 1. In the Crank Nicholson scheme, l = 0.5, which will be unconditionally stable. Tri-diagonal matrix algorithm In using the backward or the Crank Nicholson scheme, the temperatures at the next time step at various nodes have to be determined by solving simultaneously a set of linear equations, as shown in Equations 2.33 and 2.38. Note, however, that the coef cient matrix in each of these equations is a tri-diagonal matrix, which can be solved ef ciently using the tri-diagonal matrix algorithm (TDMA) described below.

Longitudinal homogeneity (or homogeneity in the direction of ow), arises from the fact that in pipe ow, turbulence is generated along the wall and there is no decay Longitudinal decay arises from the dispersion of momentum and.

Now take the divisor (851) and divide it by the remainder (115): 7 1 115 p ( 9 6 6 805 851 -46 115

Index . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 897

before height in the filename, this trick saves me the time it would take to reopen Director, load the movie, and choose Modify Movie to check the measurements in the Movie Properties dialog box. The alternative to keeping track of the Director movie s dimensions is to choose File Save as Shockwave Movie in Director; this creates an HTML file with all the necessary parameters including width and height that can be inserted into Dreamweaver. You ll find a detailed description of this process later in this chapter.

Caution I recommend that, in most situations, you opt to trim your images when exporting frames as files. But here s an exception to watch out for: If a button in one frame has a drop shadow, its trimmed size will be slightly larger than the non-drop shadow buttons. Swapping it forces it to fit the smaller button s image space, which causes a jagged, amateurish swap display.

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1. Select a cell and apply all the formatting that you want to include in the new style. You can use any of the formatting that is available in the Format Cells dialog box. 2. After you format the cell to your liking, choose Home Styles Cell Styles, and choose New Cell Style. Excel displays its Style dialog box, along with a proposed generic name for the style. Note that Excel displays the words By Example to indicate that it s basing the style on the current cell. 3. Enter a new style name in the Style Name box. The check boxes display the current formats for the cell. By default, all check boxes are checked. 4. If you don t want the style to include one or more format categories, remove the check(s) from the appropriate box(es). 5. Click OK to create the style and to close the dialog box.

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