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Variational formulation and unique solvability A variational formulation of the form (1.66) is obtained in the standard way. It is worth mentioning that it requires the components of f to be L -functions. Thus piecewise discontinuous coefficients corresponding to various materials are indeed possible, and the resulting potential still is a H1-function. The existence and uniqueness of solution is a consequence of the Lax-Milgram lemma, as it was described in Paragraph 1.2.8 (under the assumption that the part ru of d o corresponding to the Dirichlet boundary conditions is not empty). Calculation ofE After calculating the (continuous, elementwise-polynomial) distribution of the scalar electric potential (p. in the computational domain R,,, electric field E the is obtained via the relation (7.20). It is interesting to observe that the tangential component of E = -Vq< is continuous, i.e., E lies in the desired Hilbert space H(cur1).

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<dl> <dt>Capital</dt> <dd>Sum owed by a business to its owners. See Owner s Equity.</dd> <dt>Cash</dt> <dd>Total of currency, coins, money orders, checks, bank drafts, and letters of credit the firm has on hand or in bank accounts from which money can be drawn immediately.</dd> <dt>Cash Payments Journal</dt> <dd>Journal for recording payments made in cash.</dd> </dl>

When you use the Distance option to create a perspective view, the option automatically turns on a front clipping plane at the camera point.

The first thing you ll want to do with a blank video layer is give it a unique name that is descriptive of the element on that layer.

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A rule de nition contains underlined elements that represent the parts of the rule that you can edit. Figure 28-5, for example, shows a de nition with two editable elements: people or public group and speci ed. When you click such an underlined element, Outlook opens a dialog box in which you can specify the details. In this example:

(Parallelogram rules in z2(R )and L 2 ( 0 ) )

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where {h(p)} (h(p) = [h1p , h2p , . . . , hmp ]T ) are the impulse responses of channels with length M and (k) is the additive white Gaussian noise that is assumed to be statistically independent of the source signal s(k). Stacking N successive samples of the observation vector, i.e., X (k) = [xT (k), xT (k 1), . . . , xT (k N + 1)]T IRN , the model (9.12) can be reformulated as a system of linear algebraic equations X (k) = HN S(k) + V(k), where HN = and S(k) = V(k) = [s(k), s(k 1), . . . , s(k N M + 1)]T IRN +M [ T (k), T (k 1), . . . , T (k N + 1)]T IRN m . (9.16) (9.17) , (9.15) (9.14) (9.13)

FIGURE 9-2

Hence, the Kullback-Leibler divergence can be expressed by the di erence between H(y) and the marginal entropies Hi (yi ) as

5. Commit your edits. When you re satisfied with what you ve typed, you re ready to commit the type, which simply means telling Photoshop that you ve finished typing and you want to keep it. As usual, Photoshop gives you a myriad of ways to commit your type use whichever of the following methods feels right for you:

where chs is a dimensionless coefficient. However, if one tries to calculate chs from (7.78) and (7.163), one obtains a divergent integral expression for chs, indicating that the hard-sphere interaction is too singular for the present approach (see Exercise 182). For the nonvanishing entries of the friction matrix (7.161), we now have

satisfiable if it is satisfied for some model/world pair; unsatisfiable if it is not satisfied by any model/world pair;

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Checking Out How Video Systems Work 351 Generating the image 352 Dividing up the work 352 Creating pathways 353 Reviewing the video standards 353 Mastering the bus 355 Controlling the video card 356 Riding the video bus 356 Video BIOS 356 Interfacing the video system 357 Video and system resources 358 Video device drivers 358 The RAMDAC 358 Accelerating 3-D graphics 359.

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