panel-methodlisted
Install: claude install-skill ashfordeOU/aero-agent-skills
# Surface Panel Method (aerodynamics/cfd/panel-method)
Use when the task is a surface panel method for incompressible
potential flow: discretizing an airfoil or body into source or doublet
panels, applying the Neumann or Dirichlet boundary condition, enforcing
the Kutta condition, or computing the pressure distribution and force
coefficients.
## Domain quick reference
- Panel methods replace the body surface with flat panels carrying
constant-strength singularities. Source panels model thickness and
non-lifting bodies; doublet panels (or vortex panels) model lifting
surfaces; the singularity strengths are the unknowns of a linear
system assembled from influence coefficients.
- Neumann boundary condition (source panel method): the total velocity
normal to the surface is zero at each control point (panel midpoint),
sum_j A_ij sigma_j = -(V_inf dot n_i), with the source self-influence
A_ii = 1/2. The source panel method reproduces the analytic cylinder
pressure coefficient Cp = 1 - 4 sin^2(theta) to machine precision
for an inscribed polygon.
- Dirichlet boundary condition (doublet panel method): the interior
velocity potential is zero at each control point, sum_j D_ij mu_j =
-phi_inf_i with D_ii = 1/2. The doublet strength equals the surface
velocity potential, so the surface velocity is the surface derivative
of the doublet distribution.
- Kutta condition: for a lifting body with a sharp trailing edge, the
tangential velocities on the upper and l