scholarly journals A Novel Small-Specimen Planar Biaxial Testing System With Full In-Plane Deformation Control

2018 ◽  
Vol 140 (5) ◽  
Author(s):  
Samuel Potter ◽  
Jordan Graves ◽  
Borys Drach ◽  
Thomas Leahy ◽  
Chris Hammel ◽  
...  

Simulations of soft tissues require accurate and robust constitutive models, whose form is derived from carefully designed experimental studies. For such investigations of membranes or thin specimens, planar biaxial systems have been used extensively. Yet, all such systems remain limited in their ability to: (1) fully prescribe in-plane deformation gradient tensor F2D, (2) ensure homogeneity of the applied deformation, and (3) be able to accommodate sufficiently small specimens to ensure a reasonable degree of material homogeneity. To address these issues, we have developed a novel planar biaxial testing device that overcomes these difficulties and is capable of full control of the in-plane deformation gradient tensor F2D and of testing specimens as small as ∼4 mm × ∼4 mm. Individual actuation of the specimen attachment points, combined with a robust real-time feedback control, enabled the device to enforce any arbitrary F2D with a high degree of accuracy and homogeneity. Results from extensive device validation trials and example tissues illustrated the ability of the device to perform as designed and gather data needed for developing and validating constitutive models. Examples included the murine aortic tissues, allowing for investigators to take advantage of the genetic manipulation of murine disease models. These capabilities highlight the potential of the device to serve as a platform for informing and verifying the results of inverse models and for conducting robust, controlled investigation into the biomechanics of very local behaviors of soft tissues and membrane biomaterials.

Author(s):  
Yuzhen Chen ◽  
Tianzhen Liu ◽  
Lihua Jin

Supplementary Text 1: Material modeling and characterization We used the following incompressible neo-Hookean material model to define the instantaneous constitutive behavior of the shells, = tr − 3, (S1) where W is the strain energy density function, µ is the shear modulus, F is the deformation gradient tensor. To describe the viscoelastic behavior of the shells, Prony series were used and the shear modulus µ can be expressed as = 1 − ∑ 1 − ⁄ , (S2) where µ0 is the instantaneous shear modulus, n is the number of the series terms, is the dimensionless relaxation modulus, t is the time, and τi is the relaxation time constant. Here we characterize the viscoelastic properties of the silicone rubber (Dragon SkinTM30) and urethane rubber (VytaFlexTM 20). We modeled their viscou


2013 ◽  
Vol 20 (6) ◽  
pp. 987-991 ◽  
Author(s):  
V. Pérez-Muñuzuri ◽  
F. Huhn

Abstract. Spatial maps of the finite-time Lyapunov exponent (FTLE) have been used extensively to study LCS in two-dimensional dynamical systems, in particular with application to transport in unsteady fluid flows. We use the time-periodic double-gyre model to compare spatial fields of FTLE and the path-integrated Eulerian Okubo–Weiss parameter (OW). Both fields correlate strongly, and by solving the dynamics of the deformation gradient tensor, a theoretical relationship between both magnitudes has been obtained. While for long integration times more and more FTLE ridges appear that do not seem to coincide with the stable manifold, ridges in the field of path-integrated OW represent fewer additional structures.


Author(s):  
Lallit Anand ◽  
Sanjay Govindjee

This chapter develops the necessary mathematics for describing general deformations that a solid body may undergo, a topic known as kinematics. Definitions of motion, displacement, velocity, and acceleration which are vectors, and the deformation gradient and displacement gradient which are tensors are given. The mapping of material vectors by the deformation gradient tensor as a basic concept in describing the large deformation kinematics of a deformable body is presented. The powerful polar decomposition theorem is discussed and applied to the deformation gradient tensor to show that it can be decomposed into a stretch followed by a rotation, or a rotation followed by a stretch. Non-linear measures of strain are defined in terms of the stretch tensors. The important case of small deformations, which results in linear measures of strain, is discussed. For small strains the important decomposition of the state of strain that separates a volumetric strain from a non-volumetric or deviatoric strain is presented.


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