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Absorbing a frontal crash.

In a frontal crash, the front rail must fold like an accordion. It turns the impact energy into plastic deformation and protects the cabin. In a team of five, we simulated three tube shapes, then five materials, to find the best energy absorber.

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The three absorbers at the end of the crush

The three shapes at the end of the crush, von Mises stress.

Impact speed
216 km/h
Crush distance
300 mm
Shapes tested
3
Materials
5
Phase 1 · Shapes

Three shapes, one crash.

Three 1,000 mm tubes in AA6063-T5 aluminium, fixed at one end and hit at 60 m/s at the other. Only the cross-section changes: a diamond inspired by a front rail, a closed hat profile, and a square tube with internal walls.

P1
Multi Cell Tube3.7 kJSquare, inner walls · peak 40 kN
P2
Rail Crush3.2 kJDiamond section · peak 25 kN
P3
Curved Beam3.1 kJClosed hat · peak 21 kN
Von Mises stress0 → 200 MPa · 0.5× slow motion

Force during the crush

Multi Cell TubeRail CrushCurved Beam
Force (kN)Crush distance (mm)
010203040050100150200250300Crush distance (mm)
  • Multi Cell TubeA 40 kN peak at the first fold, then a regular accordion collapse. Each inner wall adds corners, and the corners are what absorb the energy.
  • Rail Crush3.2 kJ on paper, but almost a third is artificial (hourglass) energy from the C3D8R solid mesh. Less reliable result.
  • Curved BeamThe beam buckles in global bending: the force drops close to zero and 1.7 kJ is still kinetic energy at the end of the crash.
Phase 2 · Materials

Five materials on the Multi Cell.

The best shape was then tested with five alloys, under the same crash conditions. Titanium absorbs more than three times the energy of the reference aluminium.

Ref.
Aluminium AA6063-T53.7 kJScale 0 → 200 MPa
Max
Titanium Ti-6Al-4V12.4 kJScale 0 → 1,050 MPa

Energy absorbed during the crash

Ti-6Al-4V304 steelAA5052-H32AA6063-T5Mg AZ31B
Energy (kJ)Time (ms)
024681012051015202530Time (ms)

Energy absorbed

Ti-6Al-4V
12.4 kJ
304 steel
7.4 kJ
AA5052-H32
4.5 kJ
AA6063-T5
3.7 kJ
Mg AZ31B
3.7 kJ

Energy per kilo of material

Ti-6Al-4V
×2.1
Mg AZ31B
×1.5
AA5052-H32
×1.2
AA6063-T5
×1.0
304 steel
×0.7

With the same geometry, the part mass is proportional to the density. Index 1 = AA6063-T5 aluminium.

Summary

The right trade-off for a production car.

MaterialEnergyPeak forceDensityEnergy / kg
Ti-6Al-4V12.4 kJ66 kN4.43 g/cm³×2.1
304 steel7.4 kJ66 kN7.90 g/cm³×0.7
AA5052-H324.5 kJ58 kN2.68 g/cm³×1.2
AA6063-T53.7 kJ40 kN2.70 g/cm³×1.0
Mg AZ31B3.7 kJ37 kN1.77 g/cm³×1.5

Titanium absorbs the most, but with a 66 kN peak that is hard on the occupants, and a cost far too high for a production car. Stainless steel absorbs twice as much as aluminium but weighs three times more: it loses as soon as you look per kilo.

  • AA5052-H32+22% energy for the same mass as the reference alloy: the best trade-off for production cars.
  • Magnesium AZ31BSame energy as aluminium, one third lighter: a real option for lightweight design.
  • Titanium Ti-6Al-4VThe benchmark for pure performance, kept for motorsport and aerospace.

Team project (5 students), Computational Structural Mechanics module, ESILV 2025–2026. Models based on the Dassault Systèmes Crash workshops and Fang et al. (2015).

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