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molecules remain inside the particles. After the lm is applied, water is lost by evaporation, the particles move closer together, and eventually come into contact. Then the polymer molecules diffuse across the former boundaries of the particles in a process called coalescence. Many latex paints contain coalescing agents, which are oxygenated organic solvents that are selected to partition in an optimum way to promote interparticle diffusion during coalescence. A different strategy for reversing binder water interaction is used in the socalled water-soluble or water-dispersible systems. The same thermoset binder components used in solvent-borne systems are modi ed by introducing hydrophilic groups such as carboxylic acid groups. The acid groups are neutralized by amine groups from aminoalcohols such as dimethylaminoethanol (DMAE). The ionic sites contribute more to solubilization and/or dispersion than do the COOH groups alone. During heat cure, part of the amine is driven off and often some of the COOH groups react with the crosslinker. Both of these changes help convert the system from a slightly hydrophilic dispersion to a hydrophobic cure lm. Latex systems are pure white like whole milk, but waterdispersible systems are often completely clear like a true solution. They look like solutions (thus the term water soluble ), but rheology and other studies indicate that they actually consist of very small particle dispersions [12, 13]. The particles are too small to scatter visible light. Usually there are too few ionic or other solubilizing groups for dispersion in water alone, and coupling solvents are used along with water. The term coupling solvent is applied to solvents that tend to prevent phase separation in systems that contain both hydrophilic and hydrophobic components. Most coupling solvents are alcohol ethers such as propylene glycol monomethylether (I). As the structure suggests (I) HOCH2 CH(CH3 )OCH3

Now you need to invoke your serializer. The following XSQL page will apply only the serializer to the XSQL datagram. Since no stylesheet is specified, no XSLT transformation will be performed prior to invoking the serializer.

Beside these most important parameters, other characteristics such as low speckle noise wavefront generation, conjugate beam delity, and material reliability may also contribute to the selection of the good material for an optimum operation of the nonlinear mirror in a full-scale laser system. Nonlinear optical phase conjugation undoubtedly offers a great potential for energy scaling of laser sources, and several comprehensive books or review papers exist on this subject, on both the basic and applied aspects of this eld [22 33].

insert a Torus Public Sub DrawTorus() declare variables Dim dCenter(0 To 2) As Double Dim dRadius1 As Double Dim dRadius2 As Double Dim myTorus As Acad3DSolid set center of torus to 0,0,0 dCenter(0) = 0# dCenter(1) = 0# dCenter(2) = 0# dRadius1 = 10# dRadius2 = 2# torus radius tube radius

Figure 9-12: You can create a linear gradient in the quick mask mode to make the Capitol (left) fade out of the lava (right).

The AMP has gathered a group of like-minded music podcasters who are dedicated to promoting independent labels. Techpodcasts.com (http://techpodcasts.com) is a website where those interested in technology can review a centralized directory of technology podcasts covering a wide variety of topics. You will find detailed descriptions of the shows, biographies of the affiliates, and a calendar of scheduled tech podcast releases. The site imports participants show notes and has links to their sites. In addition, many of the tech podcasters are available to help individuals and groups launch their own podcasts. Members provide feedback and advice to fellow members. As I am a member of the website, I do have some bias about the site s usefulness, but overall, it is great to see what can be accomplished when a group of like-minded people work together and share common values and goals that will attract sponsors and underwriters. Figure 3-7 shows the front page of their extensive site.

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where = [ (1) (2)]T R2 . (b) Find the eigenvalues of M. Find the solution to (11.P.4). (c) Take from (b) and multiply it by constant such that 2 (k) = k=1 1 (i.e., replace by the normalized form ). (d) Using the normalized vector from (c) (i.e., ), nd (k/2) for all k Z. [Comment: Computation of the Daubechies 4-tap scaling function is the rst major step in computing the Daubechies 4-tap wavelet. The process suggested in (d) may be continued to compute (k/2J ) for any k Z, and for any positive integer J . The algorithm suggested by this is often called the interpolatory graphical display algorithm (IGDA).] 11.12. Prove the following theorem. Suppose A Rn n and A = AT . Then A > 0 iff A = P T P for some nonsingular matrix P Rn n . 11.13. Let A Rn n be symmetric with eigenvalues 0 1 n 2 n 1 . Show that for all x Rn 0 x T x x T Ax n 1 x T x. [Hint: Use the fact that there is an orthogonal matrix P such that P T AP = (diagonal matrix of eigenvalues of A). Partition P in terms of its row vectors.] 11.14. Section 11.3 presented a method of computing eAt by hand. Use this method to (a) Derive (10.109) (in Example 10.9). (b) Derive (10.P.9) in Problem 10.23.