Project brief
Decisions and iterations
Prepare geometry
SpaceClaim shrink-wrapping converted the raw faceted OBJ into a watertight simulation body. Both bumper versions were processed for comparison.
Build comparable domains
A half-car symmetric wind-tunnel domain used approximately 99,000 cells and prism-layer inflation. The inlet was set to 20 m/s.
Solve and inspect flow
Steady-state RANS k-ε results were reviewed with velocity, pressure, and pathline figures. I checked the residual history alongside the flow fields before comparing the cases.
Interpret a near-neutral result
The model predicted a drag difference of only 0.25%. That is too small to distinguish from geometry, mesh, and solver uncertainty, so the two bumper designs performed similarly in this study.
Results and context
These are CFD predictions. A mesh-sensitivity study and physical measurements would be needed to judge whether such a small difference persists outside this setup.
Technical details
Mesh and boundary conditions
Both versions used a half-car symmetry domain, approximately 99,000 cells, prism inflation, a 20 m/s inlet, standard k–ε RANS, stationary no-slip road/body walls, and a pressure outlet. The report gives a roughly 0.92 m² reference area.
Solver and convergence
Both cases ran 500 iterations. Turbulence, velocity, and momentum residuals converged; continuity stabilized without meeting the strict residual target. That residual behavior matters when judging the small difference between cases.
Force breakdown
The report gives Cd 0.29271 stock and 0.29199 modified, a relative difference near 0.25%. Its Cl values, −0.02968 and −0.04659, are model predictions. The force tables list 66.21 N stock and 66.30 N modified despite the lower modified Cd. Reference area and half-car normalization need checking before those forces can be compared directly.
Project values and components
| Stock Cd | 0.29271 |
|---|---|
| Modified Cd | 0.29199 |
| Drag delta | −0.25% (neutral) |
| Inlet velocity | 20 m/s |
| Mesh cells | ~99,000 |
| Turbulence model | RANS k-ε |