Journal of the Society of Motion Picture Engineers (1930-1949)

Record Details:

Something wrong or inaccurate about this page? Let us Know!

Thanks for helping us continually improve the quality of the Lantern search engine for all of our users! We have millions of scanned pages, so user reports are incredibly helpful for us to identify places where we can improve and update the metadata.

Please describe the issue below, and click "Submit" to send your comments to our team! If you'd prefer, you can also send us an email to mhdl@commarts.wisc.edu with your comments.




We use Optical Character Recognition (OCR) during our scanning and processing workflow to make the content of each page searchable. You can view the automatically generated text below as well as copy and paste individual pieces of text to quote in your own work.

Text recognition is never 100% accurate. Many parts of the scanned page may not be reflected in the OCR text output, including: images, page layout, certain fonts or handwriting.

538 SHAFER November given knife-edge position y, between the limits — w to +w of the light source then gives I(z) for a given light-source size, 2w, and given knifeedge position, 2/1. Fig. 13 shows a maximum contrast at w = 6.25 X 10 ~2 mm. This is the half width R of the Airy disk of the system, which is the distance from the optic axis to the first value of y for which G(y) = 0, for a free 10,000. 1,000. -10 •« -G -4 10 -2 0 2 4 6 Z-cm Fig. 12— Effect of source size on the lightintensity distribution in the image of a disturbance of Fig. 5. A = 10, a = 1, </> = 0.125 X,/ = 250 cm. The knife-edge cutoff position is at the optic axis. aperture in Fig. 9 (a) . This distance is given by the / ratio of the system and the wavelength of light used R g X {• (28) The abscissas of Figs. 12 and 13 can be nondimensionalized by expressing w or 2/1 in terms of R. The ideal light-source size for maximum contrast is 2w = 2R. This value for a practical schlieren system is much too small to be realized.