# 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`.