Fundamentals of Aerodynamics
Fundamentals of Aerodynamics
6th Edition
ISBN: 9781259129919
Author: John D. Anderson Jr.
Publisher: McGraw-Hill Education
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Chapter 3, Problem 3.10P

Prove that the velocity potential and the stream function for a uniform flow, Equations ( 3 . 53 ) and ( 3 . 55 ) , respectively, satisfy Liplace’s equation.

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Q1 (a) If a flow field is compressible, what can you say about the material derivative of density? What about if the flow field is incompressible? Explain your answer.
(a) State the equation describing the condition at streamline boundary for a two-dimensional flow with velocity V and displacement ds Using the equation, derive the equation of a streamline given by Eq. (4.1): ) (See attached images)   (b) A steady, incompressible, two-dimensional velocity field is given by Eq. (4.2) : (see attached images) Where: the x- and y-coordinates are in metres and the magnitude of the velocity is in m/s. Calculate the material acceleration at the points of (x = 2, y= 3)
Outer pipe wall Consider the steady, incompressible, laminar flow of a Newtonian fluid in an infinitely long round pipe annulus of inner radius R, and outer radius Ro. Assume that the pressure is constant everywhere there is no forced pressure gradient driving the flow, Pi = P2. However, let the inner cylinder be moving at steady velocity V to the right, essentially a piston. The outer cylinder is stationary. This makes an axisymmetric Couette flow. Use cylindrical coordinates and the equations of motion to generate an expression for the x-component of velocity u as a function of r. Ignore the effects of gravity. Fluid: p, H iP R; R, ƏP_ P2- P1 ax x2-X1

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Intro to Compressible Flows — Lesson 1; Author: Ansys Learning;https://www.youtube.com/watch?v=OgR6j8TzA5Y;License: Standard Youtube License