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Research Report
keisuke58 edited this page Feb 27, 2026
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Research confirms that modern payload fairings for Epsilon (Enhanced/S) and H3 launch vehicles are Carbon Fiber Reinforced Polymer (CFRP) Sandwich Structures.
- Face Sheets: CFRP (Carbon Fiber/Epoxy). High specific stiffness.
- Core: Aluminum Honeycomb. High crushing strength and stiffness-to-weight ratio.
- Manufacturing: Often Out-of-Autoclave (OOA) or filament wound (for monolithic parts), but fairings are typically large sandwich shells made in halves. Kawasaki Heavy Industries (KHI) and Beyond Gravity (formerly RUAG) are key manufacturers.
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Diameter:
- Epsilon: ~2.6m (Max diameter).
- H3: ~5.2m (Standard fairing).
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Structure:
- Cylindrical section + Ogive nose.
- Construction: Two half-shells (Clamshell) held by separation bolts.
Implication for Modeling:
- The simulation MUST model a sandwich structure (Shell-Solid-Shell or Homogenized Shell).
- Anisotropy: CFRP face sheets are highly anisotropic. Wave velocity depends on propagation direction relative to fibers.
- Curvature: The cylindrical geometry causes mode conversion and focusing/defocusing of guided waves, unlike flat plates.
- Leaky Waves: In sandwich structures, wave energy often leaks from the skin into the core and the opposite skin.
- High Attenuation: The honeycomb core (and adhesive layer) acts as a damper. High-frequency waves (>100 kHz) attenuate rapidly compared to monolithic plates.
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Modes:
- Global Modes: Flexural waves of the entire sandwich (low frequency).
- Skin Modes: Rayleigh-like waves confined to the skin (high frequency). This is preferred for detecting skin-core debonding.
- When the skin separates from the core (debonding), the local boundary condition changes from "supported" to "free".
- Trapped Energy: Waves entering the debonded region often get "trapped," causing amplitude amplification and ringing (standing waves) within the debonded skin.
- Velocity Change: Phase velocity decreases in the debonded region (thin plate vs. sandwich).
Standard CNNs fail on curved surfaces due to distortion in 2D projection. GNNs operate directly on the non-Euclidean manifold.
- Nodes: Finite Element nodes or sensor locations.
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Edges: Connected if geodesic distance < threshold
$R$ , or k-Nearest Neighbors.
To make the GNN "geometry-aware," node features must include:
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Coordinates:
$(x, y, z)$ (Global position). -
Surface Normals:
$(n_x, n_y, n_z)$ . The change in normal vectors between neighbors encodes local curvature.- Insight from StructGNN: Explicitly encoding structural properties (stiffness, mass) into the graph improves physics compliance.
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Material Direction: Vector defining the fiber orientation
$(v_1, v_2, v_3)$ at each node.
- StructGNN / Physics-GNN: Architectures that mimic the mass-stiffness matrix operations.
- GraphSAGE / GAT: Standard inductive frameworks. Good for learning local wave scattering patterns.
- Kernel GNN: specialized for continuous manifolds.
FEM data is "clean" and idealized. Real experimental data has:
- Sensor coupling variability.
- Environmental noise.
- Manufacturing variability (thickness variations, resin rich zones).
- Source Domain: Abaqus Simulation (Rich labels, infinite data).
- Target Domain: Open Guided Waves Dataset (Limited labels, real physics) / Future Epsilon Test Data.
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Method: Domain Adversarial Neural Networks (DANN) or Transfer Component Analysis (TCA).
- Align the feature distributions of FEM and Experiment in a latent space.
- Train the classifier on FEM features, ensuring they are indistinguishable from Experimental features.
- Refine Abaqus Model: Switch to "Composite Layup" tool in Abaqus to model Skin-Core-Skin sandwich explicitly.
- Frequency Selection: Target 50-100 kHz range where "Skin Modes" begin to dominate but attenuation is manageable.
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GNN Prototype: Build a simple GraphSAGE model using
$(x, y, z, \text{time_series})$ as input to predict defect location.