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Hi Brandon,
Thank you for your response. I would like to address or raise questions regarding the following :
(1)Yes, I used CDtot for comparison and found that the deviation primarily originates from CD0. However, as per your previous response, when using a 3D wing to simulate a 2D airfoil, I have employed a very high aspect ratio. I further examined the parameters near the wing root and found CD in the lod file, which refers to CDi. Although the CDi near the wing root is indeed smaller than the CDi of the whole wing, its effect on CDtot is almost negligible. In the history file, I found CD0, but it is not related to the spanwise position. Therefore, I still have doubts about the deviation in the CDtot data.


(2)Following your suggestion, I ran the panel method and captured a Cp slice. However, as shown in the figure below, it is clear that this solution is problematic. Considering that the low spanwise resolution might be the cause, I attempted to increase the num-u to 1000. However, this led to extremely slow computational iterations, and I ultimately killed the solver.

(3)For cp, the panel method obtains cp, while vlm obtains dcp, what is the difference between them, I can find the upper surface cp and lower surface cp in the NASA report, if I try to compare, should I use the panel method.
(4)As you mentioned, it is not recommended to use a 3D wing to simulate a 2D airfoil. Therefore, I would like to know if there are any classic and general 3D validation cases within the Reynolds number range of 200,000 to 500,000. Ultimately, my objective is to validate the fidelity of the Vortex Lattice Method (VLM). I am aware that its fidelity is slightly lower than that of CFD methods. However, the current results of CDtot show that it is not only low fidelity but appears to be distorted.
(5)If there are no 3D validation cases available, do you have any other suggestions for validating the E387 airfoil?
(6)Is it really the inherent defect of VLM that causes the deviation of CDtot?
Best regards
