Piper PA-28 Cherokee — the Hershey-bar wingvsMIT Daedalus 88 — the 34 m human-powered wing

root section naca652415 → dae11 · tip section — → dae31 · aspect ratio 5.624 → 36.667 · span 9144 mm → 34100 mm · area 14868144 mm² → 31712462 mm² · dihedral 7.00° → 1.00°

units

These analyses are not directly comparable

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

  • Piper PA-28 Cherokee — the Hershey-bar wing
  • MIT Daedalus 88 — the 34 m human-powered wing

What changed

PropertyPiper PA-28 CherokeeMIT Daedalus 88Change%
Geometry
Span9144 mm34100 mm+24956 mm+272.9%
Root chord1626 mm1050 mm-576 mm-35.4%
Tip chord1626 mm762 mm-864 mm-53.1%
Sweep parameter0.0000.484+0.484—
Dihedral7.00°1.00°-6.00°-85.7%
Tip twist0.00°-1.50°-1.50°—
TE thickness3 mm2 mm-2 mm-50.0%
Tip cap reach0.3000.250-0.050-16.7%
Derived
Aspect ratio5.62436.667+31.044+552.0%
Area14868144 mm²31712462 mm²+16844318 mm²+113.3%
Taper1.0000.726-0.274-27.4%
MAC1626 mm939 mm-687 mm-42.2%
Sections
Root sectionnaca652415dae11changed—
Tip section—dae31changed—
Shapedeviation at matched span fractions, 64 samples
Chord deviation (max)864 mm
Chord deviation (RMS)703 mm
Twist deviation (max)1.50°
Dihedral deviation (max)264 mm
Tip cap deviation (max)12503 mm

Performance

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

withheld — “Piper PA-28 Cherokee” integrates to CL 0.007 against the polar’s CL at the same α (this analysis predates the loading reporting its own) 0.271 (0.03×); “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×). 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
0.4000.6000.8001.001.201.400.0150.0200.0250.0300.0350.040CDCLPiper PA-28 CherokeeMIT Daedalus 88

air, ρ = 1.225 kg/m³

data
CDPiper PA-28 CherokeeMIT Daedalus 88
0.0120.3440.444
0.0130.3520.492
0.0130.3620.549
0.0140.3710.591
0.0140.3750.616
0.0150.3890.697
0.0160.4100.794
0.0180.4430.890
0.0190.4490.913
0.0230.5061.06
0.0250.5371.13
0.0290.5801.25
0.0370.6661.43
0.0390.6871.49