

Study with the several resources on Docsity
Earn points by helping other students or get them with a premium plan
Prepare for your exams
Study with the several resources on Docsity
Earn points to download
Earn points by helping other students or get them with a premium plan
Homework assignment on 2-D Panel Methods - Aerodynamics - MIT
Typology: Exercises
1 / 2
This page cannot be seen from the preview
Don't miss anything!


16.100 Homework Assignment # 3 Due: Monday, September 26th, 9am
Problem 1 (70%) Useful reading: Anderson: Section 3.14, 3.16, 4.5, 4.
u ⋅ n = 0 is enforce v v d
X 0.12c α
c
Consider the isosceles triangle airfoil with 12% thickness as shown above. A simple potential flow model for the flow over the triangle is to place point vortices at each of the three nodes and then determine the strengths (i.e. the circulations Γ i ) which satisfy flow tangency at three control
points. For this model, let the control points be located at the midpoints of the three edges of the triangle.
a) Set-up the 3x3 system of equations that expresses u ⋅ n = 0 v v at the control points.
b) Show that the 3x3 matrix for this system is singular (i.e. it has at least one zero eigenvalue).
c) The singularity of the matrix can be removed by applying another condition in addition to flow tangency. Since the solution that is often of interest is attached flow in which the flow leaves the trailing edge smoothly and does not wrap around the trailing edge (i.e. the flow that satisfies the Kutta condition). Any non-zero value of the circulation at node 3 would imply the flow wraps around the trailing edge (note: the velocity becomes infinite at a point vortex and therefore cannot be counteracted by the other point vortices). Thus, in this simple flow model, the Kutta condition would require that Γ 3 = 0 .Replace the flow tangency condition at the control point between nodes 2 and 3 with the Kutta condition. What is the solution for Γ 1 andΓ 2 that satisfies the remaining flow tangency conditions and the Kutta condition as a function of the freestream angle of attack?
d) Calculate and plot the lift coefficient as a function of angle of attack from –5 to +5 degrees. What is the lift slope and what is the angle of zero-lift? Note: use the Kutta-Joukowski theorem to find the lift.
Problem 2 (30%) Useful reading: Anderson: Section 2.6, 3.
y = +∞
x = x 0 y = −∞ x^ = x 1
a) Using the integral form of the momentum equation, show that the lift (per unit span) is related to the amount of the airfoil turns the flow and is given by the following formula:
x x 0 x x 1
b) The velocity a few chords away from a lifting airfoil is well approximated by the freestream and a point-vortex,
where Γ∞ is a constant. Using this assumed velocity field and the result from part a), determine the lift (per unit span) for this flow (you may assume incompressible flow). Does this result look familiar?