Membrane Deployment Dynamics Simulator

Structural stability and flutter boundary analysis for large-scale thin-film membrane deployment. Models natural frequencies, spin stabilization, and solar radiation pressure forcing to determine safe operating envelopes.

Membrane Parameters

100 m 500 m 1000 m
35 g/m² 42 g/m² 50 g/m²
0.1 N/m 5 N/m 10 N/m
0 (no spin) 0.25 RPM 0.5 RPM
0.01 0.05 0.10
1 kN/m ~30 kN/m 1 MN/m
0.3 AU 0.65 AU 1.0 AU
Applied Tension 1.00 N/m
Centrifugal Tension +0.072 N/m
Effective Tension 1.072 N/m

Diameter Sweep Mode

Sweeps diameter from 100-1000m to map the stability boundary. Shows minimum tension required for flutter-free operation at each size.

Stability Boundary Map

Run a simulation to see the stability boundary map

Analysis Results

Configure the membrane parameters and run the simulation to see stability analysis results.

Research Question Addressed

RQ-1-7

Large-scale membrane deployment dynamics

What are the structural stability limits for thin-film membranes at scale? How does spin stabilization interact with solar radiation pressure forcing? What minimum tension prevents flutter for membranes of 100-1000m diameter?

Simulation Methodology

This hybrid simulator combines pre-computed finite element modal analysis with real-time analytical plate theory for interactive parameter exploration.

  • Natural frequencies from Bessel function zeros (circular membrane plate theory)
  • Spin stabilization adds centrifugal tension: T_c = sigma * omega^2 * R^2 / 4
  • Flutter boundary: SRP forcing vs structural damping capacity
  • Monte Carlo applies manufacturing variations (+/-5% tension, +/-3% density)
  • Pre-computed FE grid (if available) provides more accurate eigenvalues

Key trade-off: larger membranes have lower natural frequencies and are more susceptible to flutter, requiring either higher tension or spin stabilization. Spin rate is limited by deployment mechanisms and structural fatigue.

Project Dyson — A volunteer-led nonprofit. All plans and research are publicly available.