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Vehicle Crashworthiness and Occupant Protection - Chapter 3

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Finite Element Analytical Techniques<br />

<strong>and</strong> Applications to Structural Design<br />

necessary to account for the correct inertial response of the wheel. The wheel can<br />

become a major load path in offset or oblique frontal crash events. Therefore, the<br />

tire stiffness must be accurately simulated. The air in the tire is simulated using<br />

the airbag algorithms of the explicit codes, yielding the pressure of a constant<br />

amount of air in the tire as a function of the compressed volume, assuming<br />

isothermal or isentropic conditions. A remaining problem is in the material model<br />

of the tires themselves. Existing tire models are far too complex to be incorporated<br />

in full vehicle crash models, <strong>and</strong> research is needed to generate reasonable <strong>and</strong><br />

efficient approximations.<br />

The third primary system to be modeled for a full vehicle simulation is the steering<br />

system including the steering rack, steering column <strong>and</strong> steering wheel. For the<br />

steering rack <strong>and</strong> its connections to the wheel knuckle, the same remarks are valid<br />

as for the modeling of the front <strong>and</strong> rear axles. A correct modeling of outer contours<br />

releasing the correct degrees of freedom in the connections using joint <strong>and</strong>/or<br />

spring elements is usually considered sufficient. Rarely, a detailed model is built<br />

that couples the translational motion of the steering rack to the rotation of the<br />

wheels. This can be of importance in the study of frontal offset <strong>and</strong> oblique<br />

impacts. Very often, a steering rack model that is fixed to the subframe structure is<br />

used, thus effectively blocking the wheel rotation. The steering column is usually<br />

modeled as a set of cylindrical tubes sliding in each other. It is this sliding motion<br />

that simulates the telescopic deformation of the steering column as the dummy<br />

hits the steering wheel.<br />

To simulate the Cardan joints in the steering column, the exact geometry of the<br />

device is usually modeled with contact algorithms automatically accounting for<br />

the so-called stop-angles.<br />

Observation has shown that engine motion is crucial for the dummy response in<br />

the passenger compartment during a frontal impact. Engine motion, in turn, is at<br />

least partly determined by contacts with the structure <strong>and</strong> other components<br />

located under the hood. Consequently, these components must be modeled<br />

carefully <strong>and</strong> with mesh sizes that are not very different from the engine block<br />

mesh size. These components include the battery, radiator, air conditioning unit,<br />

automatic braking system unit, ventilators <strong>and</strong> electro-engines at the radiator,<br />

radiator bracket <strong>and</strong> light brackets. Some of these are mild steel structures <strong>and</strong><br />

can be modeled as such. Others are hard points <strong>and</strong> little care must be given to<br />

the determination of their stiffness as long as the resulting strength is considerably<br />

higher than that of the surrounding structural parts. An exception is the radiator<br />

model, which must crush under the impact of the engine block <strong>and</strong> somewhat<br />

damp its acceleration response. Equivalent models based on force-displacement<br />

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