Viscoelastic Characterization
of Agarose Gel Scaffolds
Viscoelastic Characterization
of Agarose Gel Scaffolds
The Challenge:
To Determine Viscoelastic Behavior of
Low Concentration Agarose Type VII Gel
Background
Agarose hydrogels are rapidly becoming a popular option for
an implantable scaffold material due to their biocompatibility,
native tissue-like viscoelastic mechanical properties and ease
of casting into complex shapes and sizes. Hydrogel implants
have been used in applications where structural integrity is
necessary, such as cartilage and skin. With a key functional
role of cartilage being force dampening, any potential
substitute must be capable of sustaining high impact loading.
This series of experiments uses the ElectroForce
®
3200 test
instrument to characterize the dynamic mechanical properties
of agarose gels at high frequencies.
These mean amplitudes, as measured by stretch ratio,
ranged from 0.99 to 0.70, where the stretch ratio, λ, is
defined as λ=
l
/ L
0
, where
l
is the loaded height and L
0
is the unloaded height. The displacement amplitude was
±0.5% of the unloaded height.
Figure 1 - 1% Agarose Modulus at λ = 0.9
The contribution to the complex modulus at lower frequencies
is approximately equal, while the storage modulus dominates
at higher frequencies. This is an indication that less energy
is dissipated at higher frequencies.
While this figure provides insight into the material behavior
at λ = 0.9, there is a wide range of other loading scenarios
this material can experience. Figures 2 and 3 quantify the
material responses at different mean stretch ratios. Tan
delta, an indication of the phase shift between displacement
and load, is shown for the 1% agarose gel. There is a much
larger phase shift at lower frequencies. This effect can be
understood in Figure 1 as the loss modulus does not greatly
contribute to complex modulus at higher frequencies.
Dr. Murakami and Dr. Sawae, lead researchers at the
Kyushu Institute of Technology in Japan, were interested
in investigating the mechanical behavior (dynamic modulus
and tan delta) of low concentration agarose gels at high
frequencies.To accomplish this, the ElectroForce 3200 test
instrument, in combination with WinTest
®
software, was used
to perform DMA (Dynamic Mechanical Analysis) experiments
at frequencies that ranged from 0.1 Hz to 100 Hz at different
mean displacements.
Meeting the Challenge
1% and 2% (wt.) agarose gels were produced from agarose
type VII powder (Sigma-Aldrich) using a standard gelling
protocol supplied by Dr. Murakami. Test specimens, cut
from the bulk gels, were approximately 18 mm in diameter
and 2.5 mm in height. 50 mm
diameter solid platens were
used to secure the sample.
An ElectroForce 3200 test
instrument equipped with a
1000 g load cell was used in
these experiments. DMA was
set up as a frequency sweep
from 0.1 Hz to 100 Hz at a
range of mean displacements.
Materials and Methods
Results
The DMA software immediately produces usable results
at the end of the experiments. One example of this is the
complex modulus shown in Figure 1. As the frequency is
increased, complex modulus asymptotically increases. In
addition, the software generates the two components:
storage and loss modulus.
Bose Corporation – ElectroForce Systems Group
10250 Valley View Road, Suite 113, Eden Prairie, Minnesota 55344 USA
Email: electroforce@bose.com – Website: www.bose-electroforce.com
Phone: 952-278-3070 – Fax: 952-278-3071
©2010 Bose Corporation. Patent rights issued and/or pending in the United States and other countries.
Bose, the Bose logo, ElectroForce and WinTest are registered trademarks of Bose Corporation. 032410
Figure 2 - 1% Agarose, Tan Delta at Different Mean λ
Figure 3 - 1% Agarose, Modulus at Different Mean λ
Figure 4 - 2% Agarose, Tan Delta at Different Mean λ
Figure 5 - 2% Agarose, Modulus at a Different Mean λ
Figure 3, complex modulus at different λ, provides more
insight into the material behavior. It can also be seen that
as the mean stretch ratio is decreased (i.e., the material is
more compressed), the modulus of that material is significantly
increased. Analyzing this graph along with tan delta
information from Figure 2 shows that the material behaves
significantly differently depending upon pre-stretch. As
the stretch ratio is decreased, the contribution by the loss
modulus to the complex modulus is substantially reduced.
Therefore, as the material is initially more compressed, the
behavior resembles a more purely elastic material.
Similar results can be seen for the 2% agarose gel with
different magnitudes. Tan delta for the 2% agarose gel
is less than 1% gels at lower frequencies (Figure 4).
Additionally, the complex modulus of the 2% agarose gel,
shown in Figure 5, is greater than the modulus for the 1%
agarose gel.
Plotting this data in three dimensional space leads to further
understanding of experimental results, as shown in Figure 6.
This figure displays the complex modulus of a 1% agarose
gel as a function of both the frequency and mean stretch
ratio. A surface can be fit to this data using mathematical
models which would lead to predictive capabilities. Similar
graphs can be developed displaying tan delta as a function
of both mean stretch ratio and frequency.
Incorporating tan delta into the model would further
strengthen the predictive capabilities of the model. With
this knowledge of material behavior, scaffold design
parameters and clinical application of agarose gels can be
understood prior to development.
This series of experiments demonstrates that the
ElectroForce
®
3200 test instrument is capable of operating
at the desired high frequencies while measuring small
magnitude loads with accuracy and precision. With a
variety of options for load cells and platens, the
ElectroForce 3200 is well suited for use in testing weak
viscoelastic materials.
Figure 6 - 1% Agarose, Complex Modulus
Summary