MIT Daedalus 88 — the 34 m human-powered wingvsPiper J-3 Cub — a rectangular wing that works

root section dae11 → usa35b · tip section dae31 → — · tip chord 762 mm → 1545 mm · sweep parameter 0.484 → 0.000 · tip twist -1.50° → 0.00° · te thickness 2 mm → 3 mm

units

These analyses are not directly comparable

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

  • MIT Daedalus 88 — the 34 m human-powered wing
  • Piper J-3 Cub — a rectangular wing that works

What changed

PropertyMIT Daedalus 88Piper J-3 CubChange%
Geometry
Span34100 mm10730 mm-23370 mm-68.5%
Root chord1050 mm1545 mm+495 mm+47.1%
Tip chord762 mm1545 mm+783 mm+102.8%
Sweep parameter0.4840.000-0.484-100.0%
Tip twist-1.50°0.00°+1.50°-100.0%
TE thickness2 mm3 mm+2 mm+100.0%
Tip cap reach0.2500.300+0.050+20.0%
Derived
Aspect ratio36.6676.945-29.722-81.1%
Area31712462 mm²16577850 mm²-15134612 mm²-47.7%
Taper0.7261.000+0.274+37.8%
MAC939 mm1545 mm+606 mm+64.5%
Sections
Root sectiondae11usa35bchanged—
Tip sectiondae31—changed—
Shapedeviation at matched span fractions, 64 samples
Chord deviation (max)783 mm
Chord deviation (RMS)622 mm
Twist deviation (max)1.50°
Dihedral deviation (max)204 mm
Tip cap deviation (max)11707 mm

Performance

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

withheld — “MIT Daedalus 88” integrates to CL 0.120 against the polar’s CL at the same α (this analysis predates the loading reporting its own) 0.913 (0.13×); “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×). 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
0.4000.6000.8001.001.201.400.0150.0200.0250.0300.0350.040CDCLMIT Daedalus 88Piper J-3 Cub

air, ρ = 1.225 kg/m³

data
CDMIT Daedalus 88Piper J-3 Cub
0.0120.4440.326
0.0130.4610.330
0.0130.4920.336
0.0130.5490.349
0.0140.6160.364
0.0150.6720.378
0.0150.6970.383
0.0160.7940.410
0.0170.8580.437
0.0190.9130.457
0.0211.020.511
0.0231.060.529
0.0271.200.605
0.0291.250.627
0.0361.420.729
0.0391.490.759