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| # Datasheet for the Automotive Underbody Panel Impact Dataset | |
| ## Motivation | |
| The dataset supports research on mesh-based surrogate modeling of transient | |
| impact response. It was created to evaluate whether neural operators can map a | |
| finite-element mesh and impact/material conditions to spatially distributed | |
| displacement and shell von Mises effective-stress trajectories. | |
| ## Composition | |
| - 3 fixed automotive floor-panel geometries. | |
| - 500 independent LHS cases per geometry; 1,500 cases total. | |
| - 17 aligned states per case. | |
| - Nodal displacement: three Cartesian components. | |
| - Shell-element von Mises effective stress: one scalar per element and state, | |
| taken as the maximum over all through-thickness integration points. | |
| - Impact position, three-dimensional velocity, mass ratio, and material | |
| parameters are stored per case. | |
| - Static graph topology and shell element-to-node connectivity are provided per | |
| geometry. | |
| - One fixed 400/50/50 train/validation/test partition with seed 12345. | |
| Exact tensor shapes are specified in `schema.json` and geometry metadata files. | |
| ## Stress definition | |
| The `effective_stress` target is exported from LS-PrePost using `etime 9`, | |
| labeled `Effective Stress (v-m), ip#max`. For each shell element and retained | |
| state, it stores the maximum von Mises equivalent stress across all | |
| through-thickness integration points. The integration-point index producing | |
| the maximum is not retained. Values are reported in MPa. | |
| ## Condition definitions and units | |
| The simulations use a tonne--mm--s--N consistent unit system. Coordinates and | |
| displacements are in mm, time is in s, velocity is in mm/s, mass is in tonne, | |
| density is in tonne/mm^3, and stress and Young's modulus are in MPa. | |
| The paper-level inputs map to released fields as follows: | |
| - p is `impact_xyz`, the centroid of a selected eligible panel shell; | |
| - v is `velocity_xyz`, the rigid impactor's initial translational velocity; | |
| - mu is `mass_ratio`, a dimensionless scale factor in [0.75, 1.25]; | |
| - E is `material_young_mpa`, the rigid-impactor Young's modulus; | |
| - nu is `material_poisson`, the rigid-impactor Poisson ratio. | |
| The impact speed is sampled in [1732.05, 5196.15] mm/s. Theta is sampled in | |
| [0, 15] degrees from global +Z, and phi is sampled in [0, 360] degrees in | |
| global XY from +X toward +Y. Cartesian velocity is computed from speed and | |
| these two angles. The three material categories are discrete rigid-impactor | |
| E/nu pairs: (70000 MPa, 0.33), (110000 MPa, 0.34), and | |
| (210000 MPa, 0.30). | |
| Mass ratio scales the generator's reference impactor mass and density: | |
| `impactor_mass = 0.01 tonne * mu` and | |
| `impactor_density = 5.205e-5 tonne/mm^3 * mu`. The mass field is the nominal | |
| mass recorded by the generator. | |
| ## Collection and simulation process | |
| Conditions were generated with a seven-dimensional constrained Latin hypercube | |
| over position X/Y, speed, mass ratio, theta, phi, and material class. Eligible | |
| impact positions are panel-shell centroids at least 80 mm from the topological | |
| outer boundary. Normalized LHS position coordinates are mapped to unused | |
| eligible centroids, so Z is inherited from the selected shell and is not an | |
| independent continuous coordinate. Among 128 trial designs, the normalized | |
| maximin design is retained. `metadata/LHS_DESIGN.md` records the exact | |
| geometry-specific batching and seeds. | |
| The simulations were executed with LS-DYNA SMP single precision R12 through | |
| ANSYS v221 `lsdyna_sp.exe`, using `ncpu=8` and `memory=400m`, on panel geometry | |
| derived from the 2020 Nissan Rogue finite-element model Version 3. The rigid | |
| spherical-shell impactor has radius 12.5 mm, thickness 0.1 mm, ELFORM 2, | |
| SHRF 0.833333, NIP 3, and a 5.0-mm initial gap. Panel outer-boundary nodes are | |
| fixed in all six degrees of freedom. Impactor--panel interaction uses automatic | |
| surface-to-surface contact with static and dynamic friction coefficients of | |
| 0.15. A body acceleration of 9810 mm/s^2 acts in global +Z. Further details are | |
| given in `metadata/SIMULATION_PROTOCOL.md`. | |
| Raw solver databases and curve text are not included. Panel material and shell | |
| definitions remain those of the upstream Version 3 model. The exact LS-DYNA | |
| R12 sub-build is not retained for every released case. | |
| ## Preprocessing | |
| The released case tensors are the compact 17-state inputs to downstream data | |
| preparation. They have not been reduced to a single peak state. The accompanying | |
| `build_peak_targets.py` derives the paper task by selecting the state containing | |
| the largest valid nodal displacement magnitude and using stress from the same | |
| state. | |
| The solver requests D3PLOT output every 0.0002 s through 0.03 s. Compact | |
| conversion retains every tenth raw state and appends the final state. Both | |
| nodal and element fields use indices `[0, 10, 20, ..., 150, 151]` in every | |
| released case. The first 16 retained states have a nominal 0.002-s spacing; | |
| the appended terminal state can be much closer to index 150. Exact times are | |
| stored per case. | |
| Peak time `t*` is an argmax over valid nodes and these 17 retained states only. | |
| It is therefore a discrete, temporally quantized label rather than a | |
| continuous-time solver maximum. See `metadata/TEMPORAL_SAMPLING.md`. | |
| Some source nodes may require filled values; each case retains | |
| `raw_valid_node_mask`, `filled_node_mask`, `filled_node_count`, and | |
| `valid_node_mask` to make that processing explicit. | |
| ## Data quality | |
| The release validator checks: | |
| - exactly 500 cases per geometry; | |
| - geometry-specific displacement and stress shapes; | |
| - 17 states in each field; | |
| - finite displacement and stress values; | |
| - monotonic displacement and element time arrays; | |
| - exact alignment of displacement and stress time arrays; | |
| - valid static graph and shell-element connectivity; | |
| - complete and disjoint split coverage; | |
| - archive membership and SHA-256 case digests. | |
| The `floorfrontR` revision additionally requires the source stress quality | |
| audit described in `metadata/floorfrontR_DATA_NOTE.md`. | |
| ## Recommended uses | |
| - full-field transient surrogate modeling; | |
| - graph neural operators and mesh-based learning; | |
| - peak-event displacement/stress prediction; | |
| - temporal interpolation or sequence modeling within the released protocol; | |
| - controlled comparisons on fixed meshes; | |
| - simulation-based screening research. | |
| ## Out-of-scope or unsupported uses | |
| - safety certification or replacement of final CAE/physical testing; | |
| - claims of arbitrary-geometry generalization; | |
| - treating same-numbered cases across geometries as physical pairs; | |
| - claims about real-world crash response without external validation; | |
| - mixing earlier internal `floorfrontR` artifacts with this release; | |
| - interpreting the public test labels as a permanently hidden benchmark. | |
| ## Splits and benchmark integrity | |
| The full v1.1 release includes labels for train, validation, and test cases. | |
| Consequently, the test split reproduces the paper protocol but is not a hidden | |
| benchmark after publication. New benchmark work should define a separate | |
| private evaluation set or use an evaluation server. | |
| ## Personal and sensitive information | |
| The data contain no human participants, personal data, or user-generated | |
| content. The main reuse consideration is the documented provenance of the | |
| underlying vehicle mesh. | |
| ## Distribution and maintenance | |
| The archival host is the Hugging Face Hub, with a version tag. Changes to data | |
| files require a new dataset version. Metadata changes should be documented | |
| without silently replacing data. | |
| ## Licensing | |
| Project-authored code, documentation, metadata, and derived numerical results | |
| are released under the MIT License. The panel meshes are derived from the cited | |
| CCSA/NHTSA vehicle model; upstream attribution is preserved and the upstream | |
| model is not represented as MIT-licensed project-authored content. Provenance | |
| and attribution are documented in `THIRD_PARTY_NOTICES.md`. | |