NASA Technical Note

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National Aeronautics and Space Administration., 1960
 

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Page 21 - Braslow, Albert L.; and Knox, Eugene C.: Simplified Method for Determination of Critical Height of Distributed Roughness Particles for BoundaryLayer Transition at Mach Numbers From 0 to 5.
Page 26 - AMES RESEARCH STAFF : Equations, Tables, and Charts for Compressible Flow. NACA Rep. 1135, 1953. ( Supersedes NACA TN 1428.
Page 21 - Turbulent Flat-Plate Theory for Determining Values of Turbulent Aerodynamic Friction and Heat-Transfer Coefficients.
Page 10 - The Heat Transfer and Pressure Loss in Fluid Flow Through Randomly Packed Spheres,
Page 11 - Spangenberg, WG: Heat-Loss Characteristics of Hot-Wire Anemometers at Various Densities in Transonic and Supersonic Flow.
Page 21 - A Summary of Viscosity and Heat Conduction Data for He, A, H2, 02, N2, CO, C02, H20, and Air.
Page 11 - Stalder, Jackson R., Goodwin, Glen, and Creager, Marcus 0.: Heat Transfer to Bodies in a High-Speed Rarefied-Gas Stream.
Page 29 - VENANT (1870) [13] stated the law that the directions of the increments of the principal strains coincide with the directions of the principal stresses.
Page 11 - INTRODUCTION In recent years there has been an increasing interest in the use of LIDAR (laser radar) as an active optical remote sensor.
Page 21 - Ames Research Staff: Equations, Tables, and Charts for Compressible Flow. NACA Rep. 1135, 1953. (Supersedes NACA TN 1428.) 10.

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