Looking for AERODINÀMICA (Curs Total) test answers and solutions? Browse our comprehensive collection of verified answers for AERODINÀMICA (Curs Total) at atenea.upc.edu.
Get instant access to accurate answers and detailed explanations for your course questions. Our community-driven platform helps students succeed!
Consider a rectangular wing with span b = 15 m and chord c = 1,77 m, flying horizontally in steady atmosphere with velocity U∞ = 50 m/s, and air density ρ = 1.225 kg/m3. We can assume that Re >> 1, M << 1, and that we know the circulation distribution along the wing Γ(y):
where A = 0,73, B = 2,53, and C = 14,27 are dimensionless constants, and Γo = 17,7 m2/s. You are asked to compute, for this wing, the global lift L in [N]:
Note: For the computed results, provide at least 6 decimals, and use the coma "," as decimal separator.
The image shows a vortex line with horseshoe shape. The vortex line has different intensity per unit length depending on the considered segment/leg of the horseshoe, where 98 m/s. The vortex line follows the axis from O to point B ( ), and finally it goes from point B to point E. Compute the -axis component of the flow velocity [m/s] in a point located in the position 2,7 m, as induced by the vortex line segments AO, OB, and BE, when A and E are located in the infinite . Recall that the positive direction of the axis is perpendicular to the screen, pointing out of the screen (that is, toward ourselves)
Say that we have a 3D wing which is entirely built using only a single type of airfoil. The aspect ratio of the wing is AR=10,8. As per the relationship between the vs polar curve of the 3D wing and the vs polar curves of the 2D airfoils it is made of, what is the value of in [º] at which 0,81 for the 3D wing, if the value of at which 0,81 for the 2D airfoils is 4,3º?
Consider a rectangular wing with span b = 31,3 m and chord c = 1,49 m, flying horizontally in steady atmosphere with velocity U∞ = 73 m/s, and air density ρ = 1.225 kg/m3. We can assume that Re >> 1, M << 1, and that we know the circulation distribution along the wing Γ(y):
where A = 0,63, B = 3,75, and C = 16,6 are dimensionless constants, and Γo = 29,3 m2/s. You are asked to compute, for this wing, the global induced drag Di in [N]:
Note: For the computed results, provide at least 6 decimals, and use the coma "," as decimal separator.
Say we have a doublet with intensity 16 [m3/s], a source with intensity 38 [m2/s], and a vortex with intensity -17 [m2/s], all three located in the origin of the wind reference frame. You are asked to compute the axis component of the flow velocity in units [m/s], in the position 17,3 m and 9,6 m.
Note: Please, provide at least 4 decimals and use the comma "," as decimal separator.
The perturbation velocity component in the -axis, in [m/s], in x = -0.5 m, for a thickness problem with
Say we have an airfoil with leading edge (LE) and trailing edge (TE) located at 0 and 1.84 m, respectively. The pressure coefficient distribution in the upper surface of the airfoil is trapezoidal, with -0.32 constant for all values of between and 63% of the chord, and then ranging linearly from -0.32 at 63% of the chord to 0 at . On the other hand, the pressure coefficient distribution in the lower surface fits well a cosenoidal function with period equal to 0.57 times the chord, and amplitude 0.67, crossing the positive part of the ordinate axis in the leading edge with null slope. Please, compute the value of the airfoil’s global lift coefficient (with 3 decimals; and please, use the comma "," as decimal separator).
Consider a 2D airfoil of chord 0.5 m, flying in open atmosphere with velocity = 87 m/s, as shown in the image below. The pressure far downwind becomes uniform and equal in value to the pressure far upwind,
The measured component of the flow velocity is in the top boundary of the control volume, at in the bottom boundary of the control volume, at components are:
where 0.1, and height axis (see image below), you are asked to compute
For this purpose, you can assume that the , , and
Bear in mind that the velocity cannot be assumed to be horizontal far upwind and far downwind, while it is horizontal in the top and bottom boundaries of the control volume at axis velocity component far upwind:
and the following unknown axis velocity far downwind:
Finally, a ssume an unknown velocity in the form for all the points of the fluid domain where the velocity is unknown, with
Note: The results are in SI units with 2 decimals and the comma "," is used as decimal separator