Understanding Airfoils: An In-Depth Guide
Airfoils
General Values:
NACA 2412
Conservation of Mass: ṁ1 = ṁ2 (ρ1*V1*A1 = ρ2*V2*A2)
#1: Chamber (0.02 * cord length)
Bernoulli’s Principle:
#2: Chamber Location (0.4 * cord length)
Dynamic Pressure (q): q = (1/2) * ρ * V^2
#3+4: Max Thickness (0.12 * cord length)
Ideal Gas Law: P = ρ / (R * T)
Lift Coefficient (cL): cL = L / (q * span * cord)
Gas Constant (R): R = (8.314 / M), where M is the molar mass of the gas. For air, R = 287 (m^2/(s^2K))
Drag Coefficient (cD): cD = D / (q * span * cord)
Total Pressure (Po): Po = P (static) + P (dynamic) = Ps + (1/2) * ρ * V^2
Lift and Drag per Unit Span (D’, L’): D’, L’ = cL, cD * q * c
Dynamic Viscosity (μo): μo = 1.71 x 10^-5 kg/(m*s)
Reynolds Number (Re): Re = ρ * V * c / μ
Standard Temperature (To): To = 273K
Solution Steps:
- Find Re, pitch, and dynamic pressure (q).
- Find the lift coefficient (cL).
- Solve for lift per unit span (L’) and drag per unit span (D’).
Mean Cord:
Compressibility
Forces
Mach Number (M): M = V / a
Speed of Sound (a): a = sqrt(KRT), where K = 1.4 and R = 287
Normal Force and Axial Force Coefficients (Cn and An): Cn and An = A, C / (q * s)
Steady Flow: d/dt = 0
Mass Flux (mdot): mdot = cρ
2D Flow: d/dz = 0
Scaling (Similarity)
Geometric Scaling: Lm / Lp = constant
Kinematic Scaling: Vm / Vp = constant, cDm = cDp
Dynamic Scaling: Re, M are constant
Navier-Stokes (Incompressible)
Wind Tunnels
x-direction:
Ideal Gas: Find ρ
Constant Mass: Relate V1 and V2
Bernoulli’s Principle: Solve for V2
Isentropic Flow: Use V1, M, and P0
y-direction:
Total Pressure (Po): Po = pitot reading
z-direction:
Isentropic Flow (for more accurate M): , where γ = 1.4 and M is the Mach number.
Average Pressure (P): P = (Px + Py + Pz) / 3
Bernoulli’s Principle
P + (1/2) * ρ * V^2 = constant
Sutherland’s Law: (Reference Values)
Viscous Shear:
1. Inviscid Flow: τ = 0
2. Incompressible Flow: ρ = constant (M∇ * V) + 2μ(du/dx)
3. Steady Flow: d/dt = 0
Shear Stress (τyy): τ(yy) = λ * (∇ * V) + 2μ(dv/dy)
4. Flow Along Streamline or Irrotational Flow: (Plug points into streamline and see if they are the same, ∇ x V = 0)
Shear Stress (τzz): τ(zz) = λ * (∇ * V) + 2μ(dw/dz)
Flow Patterns
Couette Flow “Sliding Surface”
Incompressible: ρ = constant
Steady: d/dt = 0
2D: d/dz = 0
Fully Developed: Flow velocity is symmetric
Viscous: V(y=0) = 0; V(y=h) = Vinf
-∇P = 0