High-rate bulk and shear responses of bovine brain tissue

Abstract This experimental study systematically investigates the dynamic response of bovine brain tissue under uniaxial strain and pure shear loading conditions. The combination of such stress states and strain rates are representative in the brain under blast loading in which both bulk and shear deformation may be involved. The dynamic uniaxial strain experiments (bulk response) were conducted on a modified Kolsky compression bar with an aluminum confinement collar. Bovine brain samples were sealed in the collar and loaded by the Kolsky bars so that the specimen only deformed in the axial direction. The resultant stress-strain curves reflected the pressure–volume relations from which the bulk modulus were obtained. The dynamic shear response was determined by using a recently developed Kolsky torsion bar technique for tissue materials characterization. Quasi-static torsion experiments were also conducted on an MTS system to construct a full set of shear stress-strain curves over a wide range of shear strain rates (0.01–700 s−1). The experimental results show that the dynamic bulk modulus of brain is in the range of 1.68–2.33 GPa which is close to the low rate values reported in the literature, while the shear responses show significant rate sensitivity over the tested strain rate range.

[1]  B. Song,et al.  SPLIT HOPKINSON PRESSURE BAR TECHNIQUES FOR CHARACTERIZING SOFT MATERIALS , 2005 .

[2]  G W M Peters,et al.  Towards a reliable characterisation of the mechanical behaviour of brain tissue: The effects of post-mortem time and sample preparation. , 2007, Biorheology.

[3]  A I King,et al.  Dynamic response of the human head to impact by three-dimensional finite element analysis. , 1994, Journal of biomechanical engineering.

[4]  B. Donnelly,et al.  Shear properties of human brain tissue. , 1997, Journal of biomechanical engineering.

[5]  L. Shuck,et al.  Rheological Response of Human Brain Tissue in Shear , 1972 .

[6]  Svein Kleiven,et al.  Finite Element Modeling of the Human Head , 2000 .

[7]  Roger C Haut,et al.  The effect of impact angle on knee tolerance to rigid impacts. , 2003, Stapp car crash journal.

[8]  Weinong Chen,et al.  Dynamic Tensile Testing of Soft Materials , 2009 .

[9]  John W. Melvin,et al.  Dynamic characteristics of the tissues of the head , 1973 .

[10]  B. Bhushan,et al.  Measurement of dynamic material behavior under nearly uniaxial strain conditions , 1978 .

[11]  A. Mackay,et al.  In vivo measurement of T2 distributions and water contents in normal human brain , 1997, Magnetic resonance in medicine.

[12]  K. Chinzei,et al.  Mechanical properties of brain tissue in tension. , 2002, Journal of biomechanics.

[13]  Tusit Weerasooriya,et al.  Radial Inertia Effects in Kolsky Bar Testing of Extra-soft Specimens , 2007 .

[14]  F. Huang,et al.  Inertia-induced radial confinement in an elastic tubular specimen subjected to axial strain acceleration , 2010 .

[15]  A. J. Maisano,et al.  Verification and implementation of a modified split Hopkinson pressure bar technique for characterizing biological tissue and soft biosimulant materials under dynamic shear loading. , 2011, Journal of the mechanical behavior of biomedical materials.

[16]  K. T. Ramesh The short-time compressibility of elastohydrodynamic lubricants , 1991 .

[17]  J. van Dommelen,et al.  The mechanical behaviour of brain tissue: large strain response and constitutive modelling. , 2006, Biorheology.

[18]  Philip V Bayly,et al.  Measurement of the dynamic shear modulus of mouse brain tissue in vivo by magnetic resonance elastography. , 2008, Journal of biomechanical engineering.

[19]  K. T. Ramesh,et al.  On the Compressibility of Elastohydrodynamic Lubricants , 1993 .

[20]  F. Pervin,et al.  Effect of inter-species, gender, and breeding on the mechanical behavior of brain tissue , 2011, NeuroImage.

[21]  T. L. Warren,et al.  Comments on the Effect of Radial Inertia in the Kolsky Bar Test for an Incompressible Material , 2010 .

[22]  K. T. Ramesh,et al.  Measurement of the Dynamic Bulk and Shear Response of Soft Human Tissues , 2007 .

[23]  James H. McElhaney,et al.  Handbook of human tolerance , 1976 .

[24]  W.-Y. Lu,et al.  A Long Split Hopkinson Pressure Bar (LSHPB) for Intermediate-rate Characterization of Soft Materials , 2008 .

[25]  Rolf H Eppinger,et al.  On the Development of the SIMon Finite Element Head Model. , 2003, Stapp car crash journal.

[26]  Takeo Matsumoto,et al.  Mechanical Characterization of Brain Tissue in High-Rate Compression , 2007 .

[27]  R. Willinger,et al.  Shear Properties of Brain Tissue over a Frequency Range Relevant for Automotive Impact Situations: New Experimental Results. , 2004, Stapp car crash journal.

[28]  Weinong W Chen,et al.  Dynamic mechanical response of bovine gray matter and white matter brain tissues under compression. , 2009, Journal of biomechanics.

[29]  Glenn R. Paskoff,et al.  Effects of tissue preservation temperature on high strain-rate material properties of brain. , 2011, Journal of biomechanics.

[30]  J C Gardiner,et al.  Simple shear testing of parallel-fibered planar soft tissues. , 2001, Journal of biomechanical engineering.

[31]  J. M. Caruthers,et al.  A Kolsky Torsion Bar Technique for Characterization of Dynamic Shear Response of Soft Materials , 2011 .