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The objective of this section is to derive basic adaptive learning algorithms that perform an update of the external (output) parameters W = [C, D] in the demixing model. It should be noted that for any feed-forward dynamical model, the internal parameters represented by the set of matrices [A, B] are xed and they can be explicitly determined on the basis of the assumed model. In such a case, the problem is reduced to the estimation of external (output) parameters but the dynamical (internal) part of the system can be established and xed in advance. In fact, the separating matrix W = [C, D] IRm (m+M ) can be estimated by any learning algorithm for ICA, BSS or BSE discussed in the previous chapters, assuming that the sensor vector has the form x = [ T , xT ]T = [ 1 , 2 , . . . , M , x1 , x2 , . . . , xm ]T IRM +m . In other words, our objective in this section is to estimate the non-square full rank separating matrix W for a memoryless system with (M + m) inputs and m outputs. The basic idea is to use the gradient descent approach to minimize suitably design cost functions. We can use several criteria and cost functions discussed in the previous chapters. To illustrate the approach, we use the minimization of the Kullback-Leibler divergence as a measure of independence of the output of the signals. In order to obtain an improved learning performance, we de ne a new search direction, which is related to the natural gradient, developed by Amari [21] and Amari and Nagaoka [42].

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If you make the keyboard available for user navigation, the Esc key will also be available for stopping the program. A utility is available that disables the Esc key at www.mvps.org/skp/noesc.htm.

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Category: Proo ng AutoCorrect options Change how PowerPoint corrects and formats text as you type Ignore words in UPPERCASE Ignore words that contain numbers Ignore Internet and le addresses Flag repeated words Enforce accented uppercase in French Click the AutoCorrect Options button here to access and con gure AutoCorrect, as described in 8. Use these check boxes to adjust the spelling check, as described in 8. The options here affect all Of ce applications.

For this exercise, use the Rug.obj file found in the Photoshop CD containing the bonus content. To access this file, insert the bonus content CD and navigate to Goodies 3D models Rug.

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Suppose that the brightness values of neighboring pixels are 10 and 20. If you set the Threshold value to 5, Photoshop reads both pixels, notes that the difference between their brightness values is more than 5, and treats them as an edge. If you set the Threshold value to 20, however, Photoshop passes them by. A low Threshold value, therefore, causes the Unsharp Mask filter to affect a high number of pixels, and vice versa. In the top row of images in Figure 10.19, the high Threshold values result in tiny slivers of sharpness that outline only the most substantial edges in the flower s petals. As the Threshold value is lowered incrementally in the second and third rows, the sharpening effect takes over more and more of the petals, ultimately sharpening all details uniformly in the lower-right example.

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Zooming does not affect the actual size of objects. 9 covers changing the actual size of objects, known as scaling.

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5. (Optional) To keep the source formatting for the slide(s), mark the Keep Source Formatting check box. Otherwise, the content of the slides inserted will adjust to the destination presentation s master slide settings.

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To illustrate the ideal gas behavior of our hard-sphere gas, we calculate the pressure on the walls of a container (see Figure 7.1). If Nj is the number of particles that has a positive velocity component vj toward the right wall, the fraction v j A t / L , of those particles will be reflected at the wall during the time interval At, where L, denotes the size of the cubic container. The momentum transfer to the wall by a reflected particle with velocity vj is 2mvj. The total momentum transferred to the wall per unit time, divided by the area of the wall, then gives the pressure (7.1) If we note that C jNj = N / 2 because only half of the particles have a positive velocity component toward the right wall and that, on average, the square of each velocity component is one third of the square of the full velocity vector in threedimensional space, we obtain N 2N1 p = -m- 1 (v2) = ---m v 3 3V2 or the law of Boyle and Mariotte in the form 2 pV = -E. 3 An alternative implication of (7.2) is

The second most important thing to understand about PHP syntax is that it applies only within PHP. Because PHP is embedded in HTML documents, every part of such a document is interpreted as either PHP or HTML, depending on whether that section of the document is enclosed in PHP tags.

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