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16.61 Aerospace Dynamics Spring 2003 Derivation of lagrangian equations Basic Concept: Virtual Work Consider system of N particles located at(, x2, x,,.x3N )with 3 forces per particle(f. f, f..fn). each in the positive
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16.61 Aerospace Dynamics Spring 2003 Example Given: Catapult rotating at a constant rate(frictionless, in the horizontal plane) Find the eom of the particle as it leaves the
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CoRIoLIS ACcELERAT0 EMYSTIF∈p CONSIOER CASE oF CONSTANT ROTA ToN.No AT0 N OF MME⊙AGUA,ANDc°srAT RADIAL VELOCITY ( As sEEN IN THE RomTIwG 仅AAE
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《流体动力学》(英文版)lecture 13
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1 Definitions The details of the velocity profile u() at any x location are rarely significant in engineering applications. The most significant quantities are integral thicknesses which describe the mass Alux, momentum flux, and kinetic energy flux in the shear layer:
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Ba5IS FOR INTEGRAL BL METNopS rescaling of u an Example: Falkner- Skan profile
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《流体动力学》(英文版)lecture 1
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11. 4 PRANDTL-GLAUERT COMPRESSIBILITY CORRECTION The methods that approximately take into account of the effects of compressibility by correct the Incompressible flow results Is called compressible corrections
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This chapter mainly deal with the properties of two-dimensional airfoils at mach number above 0.3 but below 1, where the compressibil ity must be considered
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本节要点只有 一、计算通过正激波的流动特性变化
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