Head kinematics during shaking associated with abusive head trauma
Introduction
Abusive head trauma (AHT) is a leading cause of traumatic brain injury in children (Duhaime et al., 1998, Parks et al., 2012a, Parks et al., 2012b) that is characterised by a triad of symptoms comprising of subdural and retinal haemorrhages and acute brain dysfunction (Harding et al., 2003). Shaking of infants by caregivers is believed to be a common feature of the abusive injury, but the mechanism of injury is unclear and there is debate about whether shaking alone is sufficient to elicit the injuries observed (Geddes et al., 2001, Geddes et al., 2003, Geddes et al., 2004, Punt et al., 2004, Squier, 2008).
To further the understanding of injury mechanisms, a number of animal experimental and computational models have been used. Early experiments were performed on primates to investigate injury thresholds during whiplash (Ommaya and Hirsch, 1971, Ommaya et al., 1968) and the injuries caused by translational and rotational head motion (Gennarelli et al., 1982, Ommaya and Gennarelli, 1974). These experiments were designed to investigate traumatic head injuries resulting from motor vehicle accidents in adults. Simple brain mass scaling was used to extrapolate insights from these adult primate data to children (Duhaime et al., 1987), but experimental work in piglets has shown that age-dependant material properties of brain tissue may have a large effect on biomechanical injury thresholds (Thibault and Margulies, 1998). A suitable animal model that exhibits all features of abusive head trauma in infants has not yet been described. Recently, repeated manual shaking experiments in lambs were shown to produce microscopic damage (Finnie et al., 2010, Finnie et al., 2012) but macroscopic bleeding, such as is reported in infants clinically, has not been observed.
Coupled rigid-body computational models of the paediatric head and neck have been developed to investigate car crash injuries (Dibb et al., 2014) and have been used to describe head kinematics during infant shaking (Wolfson et al., 2005). However, no in vivo shaking validation was performed by Wolfson et al. who instead relied upon mechanical surrogates (Cory and Jones, 2003, Duhaime et al., 1987). The unification of computational and experimental models is necessary to justify the use of a rigid-body modelling framework to describe the head kinematics of AHT and to assist in providing a mechanistic link between the input shaking motion and head injury.
The primary objective of this study was to develop a coupled rigid-body computational model of a lamb that is based upon in vivo head kinematics measurements. In reproducing the kinematics of lambs' heads during manual shaking, the results address the hypothesis that the modelling framework is an appropriate tool for investigating the kinematics of AHT in human infants.
Section snippets
In vivo lamb experiments
Four anaesthetised lambs were shaken manually in a manner that replicates the shaking believed to occur during abusive incidents in human infants. Anaesthesia was induced in the animals with an intravenous dose of propofol and maintained with inhaled isoflurane following intubation of the airway. All protocols were approved by the Animal Ethics Committee at the University of Auckland and were designed to cause minimal distress to the animals. The animals were aged between 5 days and 8 days old
Results
The results of this study demonstrated that in vivo head kinematics were able to be reproduced by the computational model using the experimentally identified model parameters (Fig. 2). Representative results are included in Fig. 2 with the remaining results included as supplementary material. The root-mean-squared error (RMSE), defined in Eq. 3, was used to compare the fitted results to the experimental measurements.
The RMSE accelerations for Lamb1 (Fig. A.1), Lamb2 (Fig. A.2), Lamb3 (
Discussion
This study has described a computational modelling framework that is capable of reproducing head kinematics during in vivo shaking of an animal model of AHT. Identification of model parameters allowed a model-based interpretation of the experimental results. The computational model was shown to be able to reproduce the head accelerations that occur during contact of the head with the torso and demonstrated that these were the dominant accelerations of the head during shaking. The ability to
Conflict of interest statement
The authors of this paper have no conflict of interest.
Acknowledgements
The authors would like to acknowledge the support of CureKids (grant number 9491), the Health Research Council of New Zealand Maori Health Doctoral Scholarship (T.O.L) (grant number 10/738), and medical imaging support provided by Ascot Radiology (http://www.ascotrad.co.nz/) and the Centre for Advanced MRI (http://www.mri.auckland.ac.nz/). Additional technical support was provided by Mr. Mark Finch from IMeasureU Ltd (http://imeasureu.com/).
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