Piper J-3 Cub — a rectangular wing that worksvsDownwind glide foil — high aspect reference front wing

root section usa35b → e818 · dihedral 1.00° → -2.50° · area 16577850 mm² → 121109 mm² · tip chord 1545 mm → 48 mm · te thickness 3 mm → 0 mm · mac 1545 mm → 104 mm

units

These analyses are not directly comparable

The geometry comparison below is unaffected — it is a comparison of shapes, not of runs.

  • Piper J-3 Cub — a rectangular wing that works
  • Downwind glide foil — high aspect reference front wing

What changed

PropertyPiper J-3 CubDownwind glide foilChange%
Geometry
Span10730 mm1240 mm-9490 mm-88.4%
Root chord1545 mm130 mm-1415 mm-91.6%
Tip chord1545 mm48 mm-1497 mm-96.9%
Sweep parameter0.0009.717+9.717—
Dihedral1.00°-2.50°-3.50°-350.0%
Tip twist0.00°-2.50°-2.50°—
TE thickness3 mm0 mm-3 mm-93.3%
Sections4030-10-25.0%
Tip cap reach0.3000.400+0.100+33.3%
Derived
Aspect ratio6.94512.696+5.751+82.8%
Area16577850 mm²121109 mm²-16456741 mm²-99.3%
Taper1.0000.369-0.631-63.1%
MAC1545 mm104 mm-1441 mm-93.3%
Sections
Root sectionusa35be818changed—
Shapedeviation at matched span fractions, 64 samples
Chord deviation (max)1497 mm
Chord deviation (RMS)1448 mm
Twist deviation (max)2.50°
Dihedral deviation (max)121 mm
Tip cap deviation (max)5051 mm

Performance

CoefficientsDimensionless — how good the shape is, independent of size and speed.
Spanwise

withheld — “Piper J-3 Cub” integrates to CL 0.002 against the polar’s CL at the same α (this analysis predates the loading reporting its own) 0.330 (0.01×); “Downwind glide foil” integrates to CL 0.061 against the polar’s CL at the same α (this analysis predates the loading reporting its own) 0.446 (0.14×). A loading that does not integrate back to its own wing’s CL is not a coarse curve, it is a wrong one.

Drag polar
0.2000.3000.4000.5000.6000.7000.8000.0100.0150.0200.0250.0300.035CDCLPiper J-3 CubDownwind glide foil

mixed fluids (air, water (sea))

data
CDPiper J-3 CubDownwind glide foil
0.0090.2310.293
0.0100.2580.328
0.0110.2770.355
0.0110.2910.371
0.0130.3300.423
0.0130.3450.446
0.0150.3780.480
0.0170.4370.550
0.0190.4570.577
0.0210.5110.612
0.0270.6050.680
0.0350.7140.775