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The non-linear nature of the simultaneous algebraic equations encountered in the numerical solution of the Navier-Stokes equations governing the flow of fluid, gives rise to the possibility of multiple solutions (1). However, only one of these numerical solutions will be a true representation of the actual physical flow field. It is, hence, necessary to monitor the convergence of the solution in order to detect and avoid physically meaningless solutions. In this chapter, the number of possible numerical solutions which may arise is examined using an alternative approach, which may also be confirmed with the more general technique known as Bezout's Theorem (2). A mid-cell back substitution technique is developed for monitoring solution convergence. The convergence technique developed here was originally intended for the computation of the flow fields in micron-sized passages. However, the technique may also be applied to general flow problems. The computational results obtained for micron-sized passageways have been compared with corresponding experimental flow data. A brief description of the experimental equipment is also presented.

are not cut from a single large prism but are made separately The angular shear is then equal to 2 a a0 , and the direction of shear is perpendicular to the vertex edges Figure 320 shows an arrangement for testing a lens at nite conjugates The prism is adjusted so that its back surface is approximately parallel to the image plane and is near it, with the principal ray of light passing near the center of the prism This adjustment should produce visible fringes The fringe width is very large when the source image lies on the back surface of the prism The fringe width can be decreased by moving the prism along the principal ray away from the source image.

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where G gbt13 kjE1 j2 ll is the steady-state increment of the common scattering of the wave E1, and kjE1 j2 l is the average-in-space intensity. Expressions (21) allow us to nd two solutions for parameter p by expanding the ~~ denominators into series in terms of small parameter qqm l=kG ! 1. Then, the P n n P n n solution for correlation functions kE1 E4 l n E1 E4 and kE2 E3 l n E2 E3 shows the possibility of their in nite growth. The oscillation threshold is determined by solving the transcendent equation that can be written by analogy with Eq. (13): A1 B exp(iB) A2 B where

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By translating the prism laterally parallel both to the image plane and to the direction of shear, any chosen fringe can be made to pass through any chosen point of the interferogram The adjustments of Saunders s prism are similar to those of a Wollaston prism To obtain high contrast fringes, the source size in the shear direction is kept small The recommended size of the cube is 10 15 mm Saunders (1957) also studied a wavefront-reversing interferometer that employed a modi ed Kosters double-image prism Figure 321 is a sketch of the arrangement for testing a lens with one conjugate at in nity The base of the dividing prism is spherical, and its center of curvature S0 coincides with the image point at which the lens is to be tested The observer s eye is located at S0 and the image of the source is S.

The ORDER BY clause gives a list of elds that the database should use to sort the results. The optional keyword DESC after a eld makes the database sort that eld s values in descending order. (The default order is ascending. You can explicitly include the ASC keyword if you want to make the order obvious.) The following query selects the CustomerId eld and the total of the Amount values for each CustomerId from the CreditsAndDebits table. It sorts the results in descending order of the total amount so you can see who has the largest balance rst.

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