Human head–neck computational model for assessing blast injury

Abstract A human head finite element model (HHFEM) was developed to study the effects of a blast to the head. To study both the kinetic and kinematic effects of a blast wave, the HHFEM was attached to a finite element model of a Hybrid III ATD neck. A physical human head surrogate model (HSHM) was d...

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Veröffentlicht in:Journal of biomechanics 2012-11, Vol.45 (16), p.2899-2906
Hauptverfasser: Roberts, J.C, Harrigan, T.P, Ward, E.E, Taylor, T.M, Annett, M.S, Merkle, A.C
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container_end_page 2906
container_issue 16
container_start_page 2899
container_title Journal of biomechanics
container_volume 45
creator Roberts, J.C
Harrigan, T.P
Ward, E.E
Taylor, T.M
Annett, M.S
Merkle, A.C
description Abstract A human head finite element model (HHFEM) was developed to study the effects of a blast to the head. To study both the kinetic and kinematic effects of a blast wave, the HHFEM was attached to a finite element model of a Hybrid III ATD neck. A physical human head surrogate model (HSHM) was developed from solid model files of the HHFEM, which was then attached to a physical Hybrid III ATD neck and exposed to shock tube overpressures. This allowed direct comparison between the HSHM and HHFEM. To develop the temporal and spatial pressures on the HHFEM that would simulate loading to the HSHM, a computational fluid dynamics (CFD) model of the HHFEM in front of a shock tube was generated. CFD simulations were made using loads equivalent to those seen in experimental studies of the HSHM for shock tube driver pressures of 517, 690 and 862 kPa. Using the selected brain material properties, the peak intracranial pressures, temporal and spatial histories of relative brain–skull displacements and the peak relative brain–skull displacements in the brain of the HHFEM compared favorably with results from the HSHM. The HSHM sensors measured the rotations of local areas of the brain as well as displacements, and the rotations of the sensors in the sagittal plane of the HSHM were, in general, correctly predicted from the HHFEM. Peak intracranial pressures were between 70 and 120 kPa, while the peak relative brain–skull displacements were between 0.5 and 3.0 mm.
doi_str_mv 10.1016/j.jbiomech.2012.07.027
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To study both the kinetic and kinematic effects of a blast wave, the HHFEM was attached to a finite element model of a Hybrid III ATD neck. A physical human head surrogate model (HSHM) was developed from solid model files of the HHFEM, which was then attached to a physical Hybrid III ATD neck and exposed to shock tube overpressures. This allowed direct comparison between the HSHM and HHFEM. To develop the temporal and spatial pressures on the HHFEM that would simulate loading to the HSHM, a computational fluid dynamics (CFD) model of the HHFEM in front of a shock tube was generated. CFD simulations were made using loads equivalent to those seen in experimental studies of the HSHM for shock tube driver pressures of 517, 690 and 862 kPa. Using the selected brain material properties, the peak intracranial pressures, temporal and spatial histories of relative brain–skull displacements and the peak relative brain–skull displacements in the brain of the HHFEM compared favorably with results from the HSHM. The HSHM sensors measured the rotations of local areas of the brain as well as displacements, and the rotations of the sensors in the sagittal plane of the HSHM were, in general, correctly predicted from the HHFEM. 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To study both the kinetic and kinematic effects of a blast wave, the HHFEM was attached to a finite element model of a Hybrid III ATD neck. A physical human head surrogate model (HSHM) was developed from solid model files of the HHFEM, which was then attached to a physical Hybrid III ATD neck and exposed to shock tube overpressures. This allowed direct comparison between the HSHM and HHFEM. To develop the temporal and spatial pressures on the HHFEM that would simulate loading to the HSHM, a computational fluid dynamics (CFD) model of the HHFEM in front of a shock tube was generated. CFD simulations were made using loads equivalent to those seen in experimental studies of the HSHM for shock tube driver pressures of 517, 690 and 862 kPa. Using the selected brain material properties, the peak intracranial pressures, temporal and spatial histories of relative brain–skull displacements and the peak relative brain–skull displacements in the brain of the HHFEM compared favorably with results from the HSHM. The HSHM sensors measured the rotations of local areas of the brain as well as displacements, and the rotations of the sensors in the sagittal plane of the HSHM were, in general, correctly predicted from the HHFEM. Peak intracranial pressures were between 70 and 120 kPa, while the peak relative brain–skull displacements were between 0.5 and 3.0 mm.</description><subject>Biological and medical sciences</subject><subject>Biomechanical Phenomena</subject><subject>Blast</subject><subject>Blast Injuries - physiopathology</subject><subject>Brain injury</subject><subject>Brain research</subject><subject>Computer Simulation</subject><subject>Computerized, statistical medical data processing and models in biomedicine</subject><subject>Elasticity</subject><subject>Finite Element Analysis</subject><subject>Finite element models (FEM)</subject><subject>Head - physiopathology</subject><subject>Human models</subject><subject>Humans</subject><subject>Hydrodynamics</subject><subject>Medical sciences</subject><subject>Miscellaneous</subject><subject>Models and simulation</subject><subject>Models, Biological</subject><subject>Neck - physiopathology</subject><subject>Physical Medicine and Rehabilitation</subject><subject>Pressure</subject><subject>Sensors</subject><subject>Studies</subject><subject>Surrogate models</subject><subject>Traumas. 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Using the selected brain material properties, the peak intracranial pressures, temporal and spatial histories of relative brain–skull displacements and the peak relative brain–skull displacements in the brain of the HHFEM compared favorably with results from the HSHM. The HSHM sensors measured the rotations of local areas of the brain as well as displacements, and the rotations of the sensors in the sagittal plane of the HSHM were, in general, correctly predicted from the HHFEM. Peak intracranial pressures were between 70 and 120 kPa, while the peak relative brain–skull displacements were between 0.5 and 3.0 mm.</abstract><cop>Kidlington</cop><pub>Elsevier Ltd</pub><pmid>23010219</pmid><doi>10.1016/j.jbiomech.2012.07.027</doi><tpages>8</tpages></addata></record>
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source MEDLINE; Access via ScienceDirect (Elsevier); ProQuest Central UK/Ireland
subjects Biological and medical sciences
Biomechanical Phenomena
Blast
Blast Injuries - physiopathology
Brain injury
Brain research
Computer Simulation
Computerized, statistical medical data processing and models in biomedicine
Elasticity
Finite Element Analysis
Finite element models (FEM)
Head - physiopathology
Human models
Humans
Hydrodynamics
Medical sciences
Miscellaneous
Models and simulation
Models, Biological
Neck - physiopathology
Physical Medicine and Rehabilitation
Pressure
Sensors
Studies
Surrogate models
Traumas. Diseases due to physical agents
Viscosity
title Human head–neck computational model for assessing blast injury
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