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ENGINEERING ASPECTS OF HUMAN SKULL FRACTURE:EXPERIMENTAL STUDY AND THEORETICAL CONSIDERATION ON BRAIN DAMAGE Hideaki Masuzawa 1 1Dept. of Neurosurgery, University of Tokyo pp.547-561
Published Date 1972/5/1
DOI https://doi.org/10.11477/mf.1406203111
  • Abstract
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1) Four dry skulls were statically compressed in fronto-occipital direction. The forces to produce bone fracture ranged between 600 and 1000 kg weight. The load-deflection curves before fracture gave spring rates of 400 to 900 kg/mm, average 600 kg/mm.

2) Dynamic load tests after the method of Hirakawa et al. showed foamed stylene of 17 mm thickness, among other foamed plastics and rubbers, the best-fit as human scalp simulator.

3) Semi-free fall test on 25 dry human skulls were performed using a strain-gauge load cell and an accelerometer, a DC amplifier and a cathode-ray oscilloscope. Among them 20 received impact at the mid-frontal region. Various damping materials, including the scalp simulator mentioned above were used.

At fracture notching and abrupt lowering of the load curves and high frequency vibration of the acceleration curves were noted. The peak time or rise time at fracture becomes shorter compared to those when fracture does not occur. The dynamic force level for frontal bone fracture was between 400 and 1300 kg peak loads, and independent of acceleration, energy, damping materials, as well aspeak times. The variation in peak loads at the moment of fracture is closely related to the weights of skulls themselves. These results indicate that human skulls have the characteristics of brittle fracture both statically and dynamically.

4) Postulating a head falling brow-down on a hard surface, the loads in this experiment can be considered as the acceleration of the whole head multiplied by the head mass. Then, the threshold for fracture in terms of peak acceleration and peak time is very close to the Wayne State Human Tolerance Curve or H. T. C. Above this threshold, or when higher energy is applied,the head does not give rise to a higher acceleration, but fracture should occur at the same peak acceleration value and the possibly shorter peak time. This means transition to the safe zone of the H. T. C. but clinically severer brain damage is expected. The H. T. C. and the acceleration injury theory should not be applied to the brain damage when fracture occurs. Instead, skull deformation and possibly snap-back of the deformed skull should be considered as the mech-anism of brain damage associated with skull fracture.


Copyright © 1972, Igaku-Shoin Ltd. All rights reserved.

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電子版ISSN 2185-405X 印刷版ISSN 0006-8969 医学書院

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