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Change values in the field box to edit the resolution you want to apply to gradients and gradient meshes n Convert All Text to Outlines If you intend to convert text to outlines, you can see a preview for how text objects are affected in complex regions When printing a file, you ll want to avoid globally converting text to outlines, as the files are more difficult to print and small text on output devices that print at lower resolutions may appear unsatisfactory n Convert All Strokes to Outlines Converts all strokes to outlines Just as is the case with text converted to outlines, the files will take longer to print if you convert strokes to outlines n Clip Complex Regions The boundaries between vector objects and raster objects change as you move the slider Some objects remain in vector form according to the degree of rasterization you apply.

(4.19) (4.20) (4.21) (4.22)

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(6.18)

32 BURCH S INTERFEROMETER EMPLOYING TWO MATCHED SCATTER PLATES This interferometer was rst described by Burch (Burch 1953, 1962, 1969) and later reviewed by several authors, for example, by Rubin (1980) An arrangement to test a convergent lens working with unit magni cation is illustrated in Figure 31 A lens forms an image of a small source S at S0 on the lens The magni cation of the lens under test has to be extremely close to one A partially scattering plate R1 is located in front of a lens to be measured at twice its focal length The lens under test forms an image of the scattering plate R1 at another identical scatter plate R2, which is rotated 180 with respect to the rst plate, so that there is a point to point coincidence between R2 and the image of R1.

A part of the light incident on the scatter plate R1 passes through it without scattering and arrives at S0 Since this beam touches the lens only at a small region around S0 , it is not affected by the errors of the lens surface This beam acts as the reference beam Some of the incident light is, however, scattered by R1 and lls all of the aperture of the lens This beam picks up the errors of the mirror and is the measured light beam Let us consider a ray incident at a point A on the scatter plate R1 The directly transmitted ray (solid line in Fig 31) follows the path AS0 A0 and encounters a scattering center at A0 that is identical to the one at A.

This option ensures the boundaries between the vector and raster objects fall within clipping paths preventing artifacts appearing outside the path boundaries As with any illustration artwork, the more clipping paths used in a file, the more difficult the printing n Preserve Overprint Preserves all overprints assigned in the document n Page Range Apply the settings to all pages or select a page range n Apply to PDF After making your choices from the various options, click the Apply button You can save the PDF document and all the transparency flattening is saved with the document..

This ray is scattered at A0 and gives rise to a cone of rays, one of which will follow the same path as the ray scattered on the rst plate but not on the second The rays scattered at A (dotted lines) that ll the aperture of the lens under test, arrive at the image A0 and pass through R2 without scattering We thus have two mutually coherent beams emerging from R2 One beam is directly transmitted by R1 and scattered by R2, and the second is scattered by R1.

Adjustment layers permit you to apply this same technique without adding pixels to RAM. Create a new adjustment layer with the Levels option selected. After the Levels dialog box appears, press Enter to ignore it. Now select Multiply or Screen from the blend mode pop-up menu in the Layers palette. The adjustment layer serves as a surrogate duplicate of the layers below it, mocking every merged pixel. And it doesn t add so much as a K to the file size. It s an image-editing miracle layers without the pain.