. The axially symmetric potential flow about elongated bodies of revolution. Aerodynamics; Fluid mechanics. 30 As a check on the accuracy of the integration, if, (0) was also eval- uated by two other means, with the following results: Prom Gauss 7-ordinate formula \f> (0) = From Gauss 11-ordinate formula ^(0) = Prom exact integration ip (0) = It is seen that the 7-ordinate formula introduces an error in the fifth deci- mal place. The first step in the determination of if U) is to read the values of ^(t) from the graph, Figure 3- ^R sin 0 and U sin0d flare then ob-
. The axially symmetric potential flow about elongated bodies of revolution. Aerodynamics; Fluid mechanics. 30 As a check on the accuracy of the integration, if, (0) was also eval- uated by two other means, with the following results: Prom Gauss 7-ordinate formula \f> (0) = From Gauss 11-ordinate formula ^(0) = Prom exact integration ip (0) = It is seen that the 7-ordinate formula introduces an error in the fifth deci- mal place. The first step in the determination of if U) is to read the values of ^(t) from the graph, Figure 3- ^R sin 0 and U sin0d flare then ob- tained. #2(x) is then given by [58] and graphed in Figure 3. Repeated 0 V(x) -0^ ^0?r 106 l05 ^OA ^03 ^02 ^OJ Figure 3 - Comparison of Error Functions ^(x) from Iteration Formula and von Karman Method. Please note that these images are extracted from scanned page images that may have been digitally enhanced for readability - coloration and appearance of these illustrations may not perfectly resemble the original Landweber, L; David W. Taylor Model Basin. Washington, D. C. : David W. Taylor Model Basin
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