Biomedical Engineering Reference
In-Depth Information
Fig. 9 Normalized strength
and normalized molecular
weight evolution for different
degradation time of
PLA-PCL fibers of 400 µm
under PBS
on the initial material mechanical properties. However, the lack of design tools to
predict long term behavior has limited the application of biodegradable materials.
A constitutive model for a mechanical analysis is a relationship between the re-
sponse of a body (for example, strain state) and the stress state due to the forces
acting on the body, which can include the environmental effects. A wide vari-
ety of material behaviors are described with a few different classes of constitutive
equations. Mechanical properties of biodegradable plastics are commonly assessed
within the scope of linearized elasticity, despite the clear evidence that they can un-
dergo large strains before breaking. Due to the nonlinear nature of the stress vs ,
strain plot, the classical linear elastic model is clearly not valid for large strains
simulation. Other plasticity or hyperelastic models are required to model those situ-
ations. Hence, given the nature of biodegradable polymers, classical models such as
the Neo-Hookean and Mooney-Rivlin models, for incompressible hyperelastic ma-
terials, may be used to predict mechanical behavior until rupture of non-degraded
PLA [ 13 , 26 ]. A single-order, isotropic Ogden material hyperelastic model was also
used [ 23 ] to simulate the mechanical behavior evolution during degradation of a
polyester-urethane scaffold.
These models are useful to model the toughness of materials with this type of
mechanical behavior. For these materials, the work assumption implies the existence
of a scalar field, the stored energy function W , which is a function of the deformation
gradient F . The stored energy function, W , can also be represented as a function of
the right Cauchy-Green deformation tensor invariants. In general, the strain energy
Ta b l e 1 Degradation rate of PLA-PCL under PBS, determined by measuring strength and molec-
ular weight evolution for different degradation time
Ln (σ/σ o )
=−
u s t
R
Ln (M n /M o )
=−
u m t
R
u
0.103
0.996
0.0841
0.989
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