Thank you Altea.
What would be interesting would be chart showing the increase in drag as the angle of attack changes.
Also what would be interesting is the angle of attack the 109 needed to get the 1.7 CL
SR - all (er, many) of the airfoil lift and drag profiles for WWII era wings can be found in Theory of Wing Sections by Abbott and Von Doenoff - 1949. My copy was $4.00 in 1965.
Most of the airfoil section charts include CL vs AoA as well as Moment Coefficients and many have comparisons for smooth to rough airfoil effects. There are many airfoils plotted out as function of chord as well showing the pressure distribution as a function of Chord.
The 1.7 CL IIRC was around 16 degrees for the 109 slat deployment at CLmax - but Soren and Kurfurst (and probably Altea) would know for sure.
The 51 wing under optimal conditions would 'break' around 14-15 degrees.
Predicting how drag would change as function of AoA - in the context of manueveing AoA - needs wind tunnel data to develop the Drag Polar throughout the velocity range... and even then it is less precise for high bank angle drag as 99% of all wind tunnel drag is set with airframe symmetrical to the stream tube (i.e 'heading directly into the wind')
When an a/c turns in curvilinear flight the Parasite drag must include control deflections (aileron, rudder and elevator) trim drag as well as attempt some fudge factor for the increase in span wise flow properties over the wing.
When many of the computer gamers engage in these performance discussions they a.) calculate the Induced drag (easily) because the may pick a velocity, look up the wing dimensions, pick a gross weight, assume a wing geomerty efficiency factor, use the appropriate density for the altitude of interest ----> Out pops INDUCED DRAG for high speed level flight.
b.) At the top speed of that a/c for a specific altitude, they pick the Hp denoted for that run and convert to Thrust with the key assumption being the propeller efficiency. There is a component of Propeller Disk Drag embedded in Parasite/Form Drag but often discounted as too difficult to find data for it in Wind Tunnel tests.
c.) Using the Thrust calculated in b.) and the Induced Drag calculated in a.) then the Force Equation of Thrust = Induced Drag + Parasite/Form Drag can be solved for that velocity to obtain Total Parasite Drag (all Drag components other than Induced Drag due to lift).
NOTE: This result is 'true' for level flight at the velocity and Hp and altitude at MAX speed - in which there is no excess thrust to accelerate the airframe any faster.
All this (Induced and Parasite/Form Drag for Total Drag is valid at the extreme 'right' of the Drag Polar chart I presented - at max velocity. For all velocities less than max the Total Drag of the system is less and less until that point where Induced Drag and Parasite Drag 'cross over' near the middle of the Velocity range.
At the instant of time that the airplane rolls into a turn, all the initial Drag information goes out the window.
As the bank angle increases, the CL increases as a function of Bank angle, the CD of the wing changes with the 'new AoA' required for the higher CL and All the Parasite Drag components change (friction Drag reduces, form drag could increase due to major flow separation, form drag due to aileron and elevator and rudeer control gaps decrease, parasite drag of radio mast, etc devrease as velocity decreases) and Trim Drag increases due to the control deflections required to sustain Bank and turn and angle of attack.
At some point in time the limits of Bank Angle, Lift required for the Weight of the A/C, and the Velocity will reach equilibrium in the turn.
ALL the initial values calculated from Max Speed have degraded. At this moment in time the aircraft is operating at the velocity and AoA just short of stall, the power available is equal to power supplied.
At this point an assumption may be made that Induced Drag for this velocity in calculable by assuming that spanwise flow contributions for banked flight are negligible (not necessarity true). Thrust may also be calculated if Hp available in this flight config is reliable (probably true).
But remember - Parasite Drag/Form Drag is NOT what was used at the beginning of this exercise as the velocities are significantly less in the max turn than they were at top velocity, same altitude, and ALL of the Parasite/Form Drag components(friction,radio mast, radiator cowling, separation form drag at high AoA, etc) are 'tweaked', particularly the Form and Trim Drag at high AoA.
Looking at the Drag Polar Chart the Total Drag of the system has been
lowered (moved to 'left on the curve') as a result of lower velocity but without the Drag Polar OR the engineering estimates for Form Drag/Parasite drag components you have no way to accurately re-calculate these components of drag in this new 'high trim' (elevator, aileron and rudder deflection) state.
The CD0 of the wing at minimum drag or the airframe at top speed are not useful for any condition of high AoA banked flight.
For the same reasons the CLmax at stall is less useful for banked flight as all these data are collected for level flight conditions with a singe set of control positions that are not likely to be the same as a high speed highly banked turn.
I hope some of this makes sense.