The distribution of forces on a wing in flight are both complex and varying. This image shows the forces for two typical airfoils, a symmetrical design on the left, and an asymmetrical design more typical of lowspeed designs on the right. This diagram shows only the lift components, the similar drag considerations are not illustrated. The aerodynamic center is shown, labeled "c.a."
The torques or moments acting on an airfoil moving through a fluid can be accounted for by the net lift applied at some point on the airfoil, and a separate net pitching moment about that point whose magnitude varies with the choice of where the lift is chosen to be applied. The aerodynamic center is the point at which the pitching moment coefficient for the airfoil does not vary with lift coefficient (i.e. angle of attack), so this choice makes analysis simpler .^{[1]}

{dC_m\over dC_L} =0 where C_L is the aircraft lift coefficient.
In other words, the aerodynamic center is the point on the airfoil where the incremental lift (due to change in Angle of Attack) will act. And, since the lift force generated due to change of angle of attack passes through this point, the moment generated about this point will be zero. The concept of the aerodynamic center (AC) is important in aerodynamics. It is fundamental in the science of stability of aircraft in flight.
For symmetric airfoils in subsonic flight the aerodynamic center is located approximately 25% of the chord from the leading edge of the airfoil. This point is described as the quarterchord point. This result also holds true for 'thinairfoils'. For nonsymmetric (cambered) airfoils the quarterchord is only an approximation for the aerodynamic center.
A similar concept is that of center of pressure. The location of the center of pressure varies with changes of lift coefficient and angle of attack. This makes the center of pressure unsuitable for use in analysis of longitudinal static stability. Read about movement of centre of pressure.
Role of aerodynamic center in aircraft stability
For longitudinal static stability: {dC_m\over d\alpha} <0 and {dC_z\over d\alpha} >0
For directional static stability: {dC_n\over d\beta} >0 and {dC_y\over d\beta} >0
Where:

{C_z = C_Lcos(\alpha)+C_dsin(\alpha)}

{C_x = C_Lsin(\alpha)C_dcos(\alpha)}
For A Force Acting Away at the Aerodynamic Center, which is away from the reference point:

X_{AC} = X_{ref} + c{dC_m\over dC_z}
Which for Small Angles cos({\alpha})=1 and sin({\alpha})=\alpha, {\beta}=0, C_z=C_LC_d*\alpha, C_z=C_L simplifies to:

X_{AC} = X_{ref} + c{dC_m\over dC_L}

Y_{AC} = Y_{ref}

Z_{AC} = Z_{ref}
General Case: From the definition of the AC it follows that

X_{AC} = X_{ref} + c{dC_m\over dC_z} + c{dC_n\over dC_y}

.

Y_{AC} = Y_{ref} + c{dC_l\over dC_z} + c{dC_n\over dC_x}

.

Z_{AC} = Z_{ref} + c{dC_l\over dC_y} + c{dC_m\over dC_x}
The Static Margin can then be used to quantify the AC:

SM = {X_{AC}  X_{CG}\over c}
where:

C_n = yawing moment coefficient

C_m = pitching moment coefficient

C_l = rolling moment coefficient

C_x = Xforce ~= Drag

C_y = Yforce ~= Side Force

C_z = Zforce ~= Lift

ref = reference point (about which moments were taken)

c = reference length

S = reference area

q = dynamic pressure

\alpha = angle of attack

\beta = sideslip angle
SM = Static Margin
References

^ Benson, Tom (2006). "Aerodynamic Center (ac)". The Beginner's Guide to Aeronautics. NASA Glenn Research Center. Retrieved 20060401.
See also
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