Form · Study 191
Catenary
A hanging chain solves its own equation —
a·cosh(x/a)
, no algebra required. The parabola everyone guesses runs close, and wrong. Invert the sag and you get Gaudí's arch:
compression is tension, flipped
.
Parameter
a
—
Sag
s
—
px
Parabola gap
Δ
max
—
px
Chain − fit · rms
—
px
State
TENSION
the chain — links & gravity
a·cosh(x/a) — the fit
same-anchor parabola — the guess
their disagreement
Tension