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Engineering & Technology · Vehicle Systems & Mobility Engineering

Vehicle structures, crash behaviour and occupant factors

A body shell must carry service loads, protect occupied space and manage a crash pulse. Making every region equally rigid would not satisfy all of those functions. The occupants and their restraints are part of the system.

Review mechanisms and machine design, fluids, electrical power and machines, and control and automation. Use newtons, joules and watts; 1 kWh=3.6 MJ. Speed in m/s equals speed in km/h divided by 3.6. These lessons provide engineering reasoning, not driving, repair or equipment-setting instructions.

Back to the chapter

After reading, you can

Connect structure, deformation and occupant motion without converting a simple energy calculation into a safety rating.

01

Give structural regions different functions

Normal driving loads pass through suspension attachment points and the body or frame. Stiffness affects deformation and handling interfaces; strength limits damaging loads; fatigue concerns repeated service. Material selection also affects joints, corrosion, repair and manufacturing variation. Strength per mass alone cannot determine the most suitable structure.

During a collision, controlled deformation can dissipate energy while structural load paths help preserve the occupant compartment. Direction, overlap, impact partner and intrusion can change which paths participate. A result for one barrier configuration does not establish performance for all collisions. Electrical isolation, stored fuel or battery energy and post-impact access add other system concerns.

02

Use work and momentum with care

Translational kinetic energy relative to a chosen frame is .5 mv². If a resisting force dissipates a specified energy E over a displacement s, its displacement-averaged magnitude is E/s. This average does not identify the peak force or the time history. Different force–deformation shapes can have the same area under the curve.

Impulse is change in momentum, the integral of force over time. A longer appropriate deceleration interval can reduce average force for a fixed momentum change, but the occupant is not a rigid copy of the whole vehicle. Body regions, restraint engagement, posture, excursion and contact geometry determine loads. Simple vehicle averages cannot predict injury.

Energy fixes an average force, not an injury outcomeOriginal translational energy is divided by assumed stopping deformation; the resulting curve is not a crashworthiness model.0.250.50.7510200400600800Assumed stopping deformation s / mMean resisting force / kNFixed supplied translational energy: 200 kJIllustrative work account only; no injury or rating prediction
A 1000 kg mass at 20 m/s has 200 kJ. If all is dissipated through displacement s, mean resisting force is 200/s kN with s in metres: 800 kN at .25 m, 400 at .5 m, 200 at 1 m. Peak force, pulse duration, compartment intrusion and occupant loads are not determined.
03

Evaluate people and structures together

Seats, belts, airbags and interior geometry interact to manage occupant motion. Restraints must work with the surrounding structure and the occupant population; adult and child bodies differ. Visibility, seating position, reach and understandable controls also influence the human interaction before a crash. Protection of pedestrians, cyclists and other road users extends the design boundary beyond the cabin.

Engineers use component tests, sled tests, full-vehicle tests and validated structural and occupant models with defined configurations. Test devices provide particular measurements rather than a direct description of every person. Keep model uncertainty, repeatability, configuration changes and relevant impact modes in the evidence. A calculated energy reduction is useful for reasoning but does not substitute for those comparisons.

Two deformation distances, one supplied energy

For an original simplified mass 1000 kg travelling 20 m/s into a fixed stopping system, translational energy is .5×1000×20²=200000 J, or 200 kJ. If all of it is dissipated over .50 m, mean resisting force is 400 kN. At 1.00 m, the same work account gives 200 kN. The figure shows this inverse relationship.

The initial momentum is 20000 kg m/s. If the entire mass stops with a supplied time-averaged resisting force 200 kN, impulse implies .10 s. That statement alone does not prove a constant 200 kN during deformation or a 1 m displacement; force averages over time and over distance are generally different. Occupant restraint loads, intrusion, rebound, rotation and injury are not specified by this exercise.

Try the reasoning

  1. Does half the mean vehicle force establish half the injury risk?

    Show the answer and reasoning

    No. Injury depends on body-region loads, pulse shape, intrusion, restraints and occupant factors.

  2. Can two structures absorb equal energy but have different peak forces?

    Show the answer and reasoning

    Yes. Equal areas under force–deformation curves do not fix their shapes.

  3. Why retain impact configuration with a test result?

    Show the answer and reasoning

    Direction, overlap, speed, partner and occupant setup change what the result can support.

What to carry forward

Treat structural energy management and occupant response as coupled evidence questions.

References

Teaching resources and research supporting this lesson’s explanations and examples.

  1. OpenStax2 sources
    1. University Physics1 §7.2: Kinetic EnergyOpenStaxTeaching resourceopenstax.orgRead source
    2. University Physics1 §9.2: Impulse and CollisionsOpenStaxTeaching resourceopenstax.orgRead source
  2. Crashworthiness: structure, occupant motion and test configurationsNHTSATeaching resourcenhtsa.govRead source