Jean-Lynce Gnanago1, Tony Gerges1, Laura Chastagnier2, Emma Petiot2, Vincent Semet1, Philippe Lombard1, Christophe Marquette2, Michel Cabrera1, and Simon Auguste Lambert1
1Université de Lyon, INSA Lyon, Université Claude Bernard Lyon 1, Ecole Centrale de Lyon, CNRS, Ampère UMR5005, Villeurbanne, France, 23d.FAB, Univ Lyon Université Lyon1 CNRS, INSA, CPE-Lyon ICBMS UMR 5246, Villeurbanne, France
Synopsis
Tissue
engineering for regenerative medicine have been developing for a few decades
now and the number of applications is increasing to tackle the shortage of
organ donors. To date, only few systems can allow both monitoring and 3D
characterization of tissue constructs during their growth. In this study, we decided
to focus on following the Apparent Diffusion Coefficient (ADC) known to be
a marker of cell density and built a MR-Bioreactor to probe the ADC of a
growing tissue. In this preliminary work, we were able to follow the cell
density of a tumor tissue model using our dedicated MR-bioreactor.
Introduction
Tissue
engineering for regenerative medicine have been developing for a few decades
now and the number of applications is increasing to tackle the shortage of
organ donors. From cartilage to skin, a wide range of tissues are currently
being studied with the goal of restoring or replacing damaged tissues 1. While massive progress has been
achieved to produce 3D printed constructs, only few systems can allow both
monitoring and 3D characterization of tissue constructs during their growth 2,3. Despite a lower spatial resolution
compared to optical modalities, Magnetic Resonance Imaging (MRI) allows non-destructive
3D characterizations of soft tissues based on multiscale parameters that are
key in assessing tissue development 4,5. In this study, we decided to focus
on characterizing the Apparent Diffusion Coefficient (ADC) known to be a marker
of cell density 6 and built a MR-bioreactor to probe
the ADC of a growing tissue 5,7. Performing MR characterization of
growing tissues is challenging because it requires to couple an imaging
apparatus and a bioreactor which are usually not MR-compatible. To our
knowledge, only one group tackled this issue by building a dedicated
MR-compatible bioreactor3 to be used with a commercial surface
MR coil. Generally, those coils are large (~1-10cm)
compared to engineered tissues (~0.1-5cm) and thus do not allow optimal MRI
conditions. In addition to that, using such a setup consisting in two devices
adds complexity to an already complex modality, especially for non-experts. The
resulting poor integration of the bioreactor and the MR coil can result in
non-reproductible measurements. Hence, we decided to pursue our previous work 2 and propose here an improved MR-bioreactor
for ADC assessment of a 3D printed tumor tissue model.Method
Based on our
previous work based on plastronic techniques
2,8, both the electrical and mechanical
aspects of our MR-bioreactor were improved.
The coil
geometry and the passive decoupling scheme remained unchanged but two
electrical connections needed to be modified. First, the connection between the
coil and the decoupling circuit integrated within the top cap has been made
using a pair of twisted vias in order to avoid parasitic loops leading to
imaging artifacts (figure 1a,1b). Second, the connection between the MR-bioreactor
and the scanner has been displaced to an external 3D printed cover to reduce
the mechanical load on the MR-bioreactor copper tracks (figure 1c). The connection
between this cover and the MR-bioreactor is made using shield fingers (figure 5a).
Mechanical
stability and hence measurement repeatability of the experiments were improved
with a bench support designed specifically for our imaging platform (figure 5b,5c).
The imaging
platform we used was equipped with a 7 T Bruker MRI Scanner running ParaVision
5.1 and a transmitting 72mm birdcage.
To illustrate the ability of our MR-bioreactor to obtain morphological
images of small samples we 3D printed the logo of our laboratory and filled the
MR-bioreactor with a 0.9% sodium chloride solution.
3D printed
tissue models were provided by 3d.FAB platform. At time t=0, 3 tissues samples
were printed and put inside a 37°C 5% CO2 dedicated incubator. The tissues
samples were 80% porous hydrogel scaffolds containing HT29 cells and
fibroblasts (CAF). Each week, one sample was placed in our MR-Bioreactor for
MRI characterization. After the MRI experiment, a calcein-am marking of living cells
was performed on the sample.
During the
experiments, tissues were immersed in a 0.9 % sodium chloride solution to
ensure tissue viability during the acquisition time. Fluid circulation was also
needed for removing air bubbles.
The samples
were imaged using three acquisition sequences:
- Two
morphological sequences. One axial and one coronal Turborare T2 (Repetition
time (TR)=3700ms, Echo time (TE)=20ms, 16 averages, Field-of-view(FOV)=1.92*1.92,
256² matrix, 400 microns slice thickness)
- One
quantitative EPI ADC diffusion sequence (TE=19.39ms, TR=5250ms, 8 segments, 8
averages, FOV=1.92*1.92, 128² matrix, b=0 100 200 300 500 750
1000 s/mm²) in order to quantify the ADC.
Regions of
interest (ROI) were positioned within the sample. The ADC was computed using the
ParaVision’s post-processing tool.
Results
Figures
1a,1b demonstrate the artefact suppression using our twisted vias. Moreover, figures
1b,1c shows how having an additional connection with a connected cover between
the MR-bioreactor and the terminal can be detrimental to the SNR.
A 40µm
in plane resolution image of the
logo of our laboratory can be seen figure 2.
A
decreasing tendency of the ADC over the three weeks can be seen figure 3. On figure
5, the calcein AM marking of the living cells illustrate an increasing number
of cells which is in agreement with the results shown by the ADC.Conclusion
In this
preliminary work, we were able to follow the cell density of our tissues. An
analytical model 9 along with a higher sampling rate would
allow to derive the proliferation and cell motility from our measurements. However,
that would necessitate to have a more precise positioning of the sample with no
displacement or deformation which is challenging due to samples’ mechanical
properties and fluid circulation. In any case, those results are the first steps
towards in vitro 3D tumor tissue model characterization.Acknowledgements
This work
was supported by a grant from the Agence National de la Recherche
(Estimate
Project N° ANR-18-CE19-0009-01). The financial support provided by
Ingénierie@Lyon,
member of the Carnot Institutes Network (Metafab 3D project) for the
postdoctoral scholarship of Dr T. Gerges is also acknowledged. Moreover,
the role of CERMEP - Imagerie du vivant and especially Radu Bolbos and is
acknowledged.References
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