Initializing 3D Canvas...

Minimal Surfaces & Catenaries

3 min read•1 page

Minimal Surface Principles:

1. Vanishing Mean Curvature: H = 0 everywhere across the 2-manifold interior. 2. Negative Gaussian Curvature: K = κ_1 κ_2 = -κ_1^2 ≤ 0 produces pure saddle (anticlastic) geometry. 3. Uniform Stress Tensor: Surface tension is constant and isotropic in every tangent direction.
python
1import numpy as np
2
3def solve_minimal_surface_dirichlet(vertices, fixed_boundary_indices, L_cot, max_iter=30):
4 """
5 Solves Plateau's problem for minimal surfaces (zero mean curvature H = 0).
6 Minimizes Dirichlet energy E(V) = 0.5 * Tr(V^T * L_cot * V) by iteratively
7 relaxing interior vertices to the cotangent-weighted average of their 1-ring neighbors.
8 """
9 V = np.array(vertices, dtype=float, copy=True)
10 fixed_set = set(fixed_boundary_indices)
11 free_ids = [i for i in range(len(V)) if i not in fixed_set]
12
13 for _ in range(max_iter):
14 for i in free_ids:
15 # Off-diagonal entries of L_cot hold negative cotangent weights -w_ij
16 row = L_cot[i].copy()
17 diag = row[i]
18 row[i] = 0.0
19 if abs(diag) > 1e-12:
20 V[i] = -np.dot(row, V) / diag
21 return V

Minimal Surfaces (Plateau's Problem & Soap Films): A soap film spanning a wire boundary naturally contracts to minimize its surface area due to isotropic surface tension. Mathematically, this satisfies Plateau's problem: the mean curvature vanishes everywhere (H = (1 / 2)(κ_1 + κ_2) = 0), creating saddle geometry where principal curvatures are equal and opposite. Frei Otto utilized physical soap films to pioneer lightweight tensile membrane architecture (e.g. 1972 Munich Olympic Stadium).

Catenoid Waist Radius c
0.70
4 min read•1 page

Catenary Principles:

1. Hyperbolic Cosine: Exact mathematical solution y = a cosh(x/a). 2. Zero Bending Moment: Line of thrust coincides exactly with the centroidal axis of the structure. 3. Inversion Duality: Pure gravity tension transforms into pure structural compression.
python
1import math
2
3def catenary_curve(x_span=4.0, sag=1.5, num_nodes=25):
4 """
5 Computes exact hyperbolic cosine catenary curve y(x) = a * (cosh(x / a) - 1)
6 by solving a * (cosh(span / (2a)) - 1) = sag via Newton-Raphson iteration.
7 Inverted (-y), this produces Hooke & Gaudi's pure compression arch (M = 0).
8 """
9 half_l = 0.5 * x_span
10 # Initial guess for catenary parameter a = H / w from parabolic approximation
11 a = (half_l ** 2) / (2.0 * max(sag, 1e-5))
12 for _ in range(15):
13 u = half_l / a
14 f_val = a * (math.cosh(u) - 1.0) - sag
15 df_da = math.cosh(u) - 1.0 - u * math.sinh(u)
16 a -= f_val / (df_da - 1e-12)
17
18 y_anchor = a * (math.cosh(half_l / a) - 1.0)
19 coords = []
20 for i in range(num_nodes):
21 x = -half_l + (i / (num_nodes - 1)) * x_span
22 y_hang = a * (math.cosh(x / a) - 1.0) - y_anchor
23 coords.append((x, y_hang, -y_hang)) # (x, hanging_y, inverted_arch_y)
24 return coords

Inverted Catenary Chains (Hooke & Gaudí): In 1675, Robert Hooke formulated his famous principle: "As hangs a flexible cable, so inverted stands the rigid arch." Because a flexible chain cannot resist bending, it self-organizes under gravity into a state of pure axial tension. Flipping this geometry 180° vertically yields the ideal structural arch where every cross-section is in pure compression with zero bending moments (M = 0). Antoni Gaudí used multi-tier stereostatic hanging models to design the Crypt of Colònia Güell and the Sagrada Família.

0=Hanging Tension, 1=Inverted Arch
0.00
Cable Sag / Arch Rise
1.60

Related Concepts