Cancan Xu1,2, Wenhan Lee3, Guohao Dai3, Yi Hong1,2. 1. Department of Bioengineering , University of Texas at Arlington , Arlington , Texas 76019 , United States. 2. Joint Biomedical Engineering Program , University of Texas Southwestern Medical Center , Dallas , Texas 75390 , United States. 3. Department of Bioengineering , Northeastern University , Boston , Massachusetts 02115 , United States.
Abstract
Cell printing is becoming a common technique to fabricate cellularized printed scaffold for biomedical application. There are still significant challenges in soft tissue bioprinting using hydrogels, which requires live cells inside the hydrogels. Moreover, the resilient mechanical properties from hydrogels are also required to mechanically mimic the native soft tissues. Herein, we developed a visible-light cross-linked, single-network, biodegradable hydrogel with high elasticity and flexibility for cell printing, which is different from previous highly elastic hydrogel with double-network and two components. The single-network hydrogel using only one stimulus (visible light) to trigger gelation can greatly simplify the cell printing process. The obtained hydrogels possessed high elasticity, and their mechanical properties can be tuned to match various native soft tissues. The hydrogels had good cell compatibility to support fibroblast growth in vitro. Various human cells were bioprinted with the hydrogels to form cell-gel constructs, in which the cells exhibited high viability after 7 days of culture. Complex patterns were printed by the hydrogels, suggesting the hydrogel feasibility for cell printing. We believe that this highly elastic, single-network hydrogel can be simply printed with different cell types, and it may provide a new material platform and a new way of thinking for hydrogel-based bioprinting research.
Cell printing is becoming a common technique to fabricate cellularized printed scaffold for biomedical application. There are still significant challenges in soft tissue bioprinting using hydrogels, which requires live cells inside the hydrogels. Moreover, the resilient mechanical properties from hydrogels are also required to mechanically mimic the native soft tissues. Herein, we developed a visible-light cross-linked, single-network, biodegradable hydrogel with high elasticity and flexibility for cell printing, which is different from previous highly elastic hydrogel with double-network and two components. The single-network hydrogel using only one stimulus (visible light) to trigger gelation can greatly simplify the cell printing process. The obtained hydrogels possessed high elasticity, and their mechanical properties can be tuned to match various native soft tissues. The hydrogels had good cell compatibility to support fibroblast growth in vitro. Various human cells were bioprinted with the hydrogels to form cell-gel constructs, in which the cells exhibited high viability after 7 days of culture. Complex patterns were printed by the hydrogels, suggesting the hydrogel feasibility for cell printing. We believe that this highly elastic, single-network hydrogel can be simply printed with different cell types, and it may provide a new material platform and a new way of thinking for hydrogel-based bioprinting research.
Entities:
Keywords:
biodegradable hydrogel; cell printing; elasticity; single network; tissue regeneration
Cell printing has gained a surge of interest
in biomedical engineering field because it combines biocompatible
materials, cells, and supportive components into printed constructs.[1] Today, nonbiological printing is very successful
to fabricate stiff biomaterial scaffold (without cells), such as osteoinductive
materials to match patients’ anatomy for bone repair.[2−5] However, in soft tissue bioprinting, which requires live cells inside
the scaffolds, there are still significant challenges. Current cell
printing of soft tissue uses biodegradable hydrogel materials, which
are naturally derived polymers, such as fibrin,[6] gelatin,[7] hyaluronic acid,[8,9] alginate,[10] and agarose;[11] synthetic polymers, such as poly(ethylene glycol) (PEG)[12,13] and methacrylated gelatin (GelMA);[14−16] or natural–synthetic
composites.[17−19] However, these hydrogels are brittle and unstretchable
due to lack of flexibility and elasticity, which cannot mimic the
mechanical behavior of softness, stretchability, and elasticity of
human soft tissues, such as skin, skeletal muscle, blood vessels,
and heart muscles. To make stretchable hydrogels, some groups have
developed dual cross-linking-network hydrogel system to achieve high
elasticity and mechanical strength,[20−22] but such dual-network
system using two cross-linking mechanisms significantly increases
the difficulty and complexity in cell printing control and handling.
To overcome these challenges, we pursue a simple system using single
cross-linking mechanism to achieve a highly elastic and robust, biodegradable,
and biocompatible hydrogel for cell printing, which is our work reported
in this paper. We found that a triblock biodegradable polymer of polycaprolactone–poly(ethylene
glycol)–polycaprolactone (PCL–PEG–PCL) with two
end groups of acrylates and visible-light water-soluble initiator
can form a hydrogel with high elasticity and flexibility, which is
also feasible for cell printing. Both PCL and PEG components are widely
used in Food and Drug Administration (FDA)-approved devices and implants;
thus our approach will facilitate quick translation of this material
into preclinical and clinical trials in the future.Our single-network
elastic hydrogel system is simple and thus can be easily controlled
during bioprinting process. In contrast, other methods are still quite
complex and difficult to implement for cell printing. For example,
a dual-network hydrogel consisted of PEG and sodium alginate was bioprinted
into complex, cellularized structures with high stretchability and
toughness.[20] However, the use of two cross-linking
mechanisms for cell printing encounters some challenges and limitations.
First, the preparation of two or more precursors before cell printing
is tedious and time consuming. Second, in many cases, there are more
than one external stimulus involving in gelation process, such as
temperature, light, ion concentration, and enzyme (thrombin), which
will increase the difficulty of cell printing. For example, to load
cells into a polycaprolactone (PCL)/poly(lactide-co-caprolactone) (PLCL)/fibrin hydrogel during the cell printing process,
a cooling system was required to maintain the bioprinter chamber at
18 °C to avoid the cells contacting the high-temperature PCL
and PLCL.[17] Hence, single-component-based
hydrogel system, which only need one external stimulus for gelation
and can be simply prepared and bioprinted, is considered a better
choice for cell printing. In addition, to mimic the resilient native
soft tissues,[23] biodegradable hydrogels
with good mechanical strength and elasticity are desirable. Herein,
a bioprintable, biodegradable hydrogel based on single component,
possessing good mechanical strength and elasticity was designed in
this study (Figure ), which has been rarely reported.
Figure 1
Preparation and characterization of highly
elastic, visible-light cross-linked, single-network, biodegradable
hydrogel for cell printing. An acrylated PCL–PEG–PCL
triblock polymer was synthesized and then cross-linked using visible
light to form a highly elastic single-network biodegradable hydrogel.
The hydrogel has attractive mechanical properties, and it is stretchable,
compressible, and twistable. The hydrogel can also be bioprinted with
various human cells and form complex patterns upon visible-light exposure.
Preparation and characterization of highly
elastic, visible-light cross-linked, single-network, biodegradable
hydrogel for cell printing. An acrylated PCL–PEG–PCL
triblock polymer was synthesized and then cross-linked using visible
light to form a highly elastic single-network biodegradable hydrogel.
The hydrogel has attractive mechanical properties, and it is stretchable,
compressible, and twistable. The hydrogel can also be bioprinted with
various human cells and form complex patterns upon visible-light exposure.In this study, we designed a triblock
copolymer, PCL–PEG–PCL diacrylate (DA) as the single-component
precursor to form a cross-linked hydrogel network (Figure S1). Specifically, a PCL–PEG–PCL triblock
copolymer diol containing hydrophilic PEG segments and hydrophobic
PCL segments was first synthesized via ring-opening reaction. The
acryloyl groups were then introduced to the two ends of the PCL–PEG–PCL
diols to obtain the PEG–PCL-DA polymers, which formed hydrogel
under visible-light exposure. The chemical structure, water absorption,
mechanical properties, and elasticity of the PEG–PCL-DA hydrogels
were characterized. The in vitro cytocompatibility of the PEG–PCL-DA
hydrogels was evaluated by mouse 3T3 fibroblasts. Various human cells
were bioprinted with the hydrogels, and the cell viabilities were
studied after 7 days of culture. Basic geometric shapes were printed
to prove the printability of the PEG–PCL-DA hydrogels.
Materials and Methods
Materials
Poly(ethylene
glycol) (PEG, MW = 20 000, Sigma) and ε-caprolactone
(CL, Sigma) were dried in a vacuum oven at 60 °C to remove residual
water before use. Stannous octoate (Sn(Oct)2, Sigma), triethylamine
(TEA, Sigma), acryloyl chloride (Sigma), dichloromethane (Sigma),
dimethyl phenylphosphonite (Acros Organics), 2,4,6-trimethylbenzoyl
chloride (Sigma), lithium bromide (Sigma), and 2-butanone (Sigma)
were used as received.
Synthesis of PCL–PEG–PCL Copolymer
Diols
The PCL–PEG–PCL diols were synthesized
using PEG to initiate a ring-opening polymerization of CL at 120 °C
for 24 h under N2 atmosphere (Figure S1).[24] Sn(Oct)2 was used
as a catalyst. Products were dissolved in dichloromethane, precipitated
in cold diethyl ether, and then dried in a vacuum oven at 60 °C
for 3 days.
Acrylation of PCL–PEG–PCL Copolymer
Diols
Acrylation of the PCL–PEG–PCL copolymer
diols was executed through acryloyl chloride (Figure S1). The copolymer diols were dissolved in 15 mL of
dichloromethane in a three-neck flask under N2 protection,
to which TEA was added dropwise under stirring for 30 min in an ice
bath.[25] Acryloyl chloride in 15 mL of dichloromethane
was then added to the mixture dropwise. The molar ratio of the hydroxyl
groups (−OH) in PCL–PEG–PCL diols/TEA/acryloyl
chloride was set at 1:2:2. The reaction was first performed in an
ice bath for 30 min and then heated to 40 °C for 24 h under N2 atmosphere. The reaction mixture was cooled to room temperature
and then precipitated in cold diethyl ether. The precipitates were
filtered, dried in a desiccator for 2 days, redissolved in deionized
water, and dialyzed over 2 days. The synthesized PEG–PCL-DA
was collected after lyophilization. The PEG–PCL-DA polymers
were set as PEG–PCL(X)-DA, with X referring to the block length of the PCL–PEG–PCL diols.
PEG-DA without PCL segments was set as the control group, which was
synthesized from PEG (MW = 20 000) and acryloyl chloride via
the same reaction process as described above.
Proton Nuclear Magnetic
Resonance (1H NMR) Spectroscopy
The chemical structures
of the PEG–PCL-DA and PEG-DA polymers were characterized by 1H NMR (JEOL ECX Instrument, 300 MHz) with D2O as
solvent. The block length of the PCL–PEG–PCL copolymer
diols and the degree of substitution (DS) of the acryloyl group on
both ends of the PCL–PEG–PCL diols were both calculated
from the 1H NMR spectra.
Elastic Hydrogel Formation
The PEG–PCL-DA hydrogel was formed by photopolymerization
using lithium phenyl(2,4,6-trimethylbenzoyl)phosphinate (LAP) as the
water-soluble, visible-light initiator which was synthesized according
to the previous studies (Figure S1).[26,27] The PEG–PCL-DA polymers were dissolved in deionized water
and mixed with the LAP water solution to reach various final concentrations
(10, 20, and 40% w/v). The mixed solution was then poured into a cylinder
or strip mold, followed by exposure under an light-emitting diode
(LED) splash lighter (395–405 nm, 5 W) for 2 min to irradiate
the mixed solution. Then, the PEG–PCL-DA hydrogels were formed.
Unless otherwise noted, the hydrogels used for all measurements were
at a concentration of 40%.
Hydrogel Water Absorption
To determine
the swelling ratio of the PEG–PCL-DA hydrogels, the cylinder
samples (4 mm height; 9 mm diameter; n = 3) were
immersed in phosphate-buffered saline (PBS) at 37 °C for 24 h.[28] The hydrogels were then taken out, and the surface
water of the hydrogels was removed gently with a filter paper; the
hydrogels were weighed (Ws). The swollen
hydrogels were rinsed by deionized water and lyophilized. The weight
of dry hydrogel after freeze-drying was recorded as Wd. The swelling ratio was calculated as (Ws – Wd)/Wd × 100%.
Mechanical Property Measurement
The hydrogels used for all mechanical measurements were in wet state
(immersion in PBS for 24 h) before testing. The compression testing
of cylinder hydrogels (4 mm height; 9 mm diameter; n = 4) was performed on MTS Insight Testing System with a 500 N load
cell and a cross-head rate of 1 mm/min.[29] For uniaxial tensile testing, the strips of PEG–PCL-DA hydrogels
with 50 mm length, 5 mm width, and 3 mm height (n = 3) were prepared and tested on MTS Insight Testing System with
a 500 N load cell and a cross-head rate of 10 mm/min according to
ASTM D638-03.[30] The instant strain recovery
of PEG–PCL-DA hydrogel strips (n = 4) were
carried out and measured under the same conditions as described above.[31] The hydrogel strip was stretched to 10% strain,
held for 1 min, and then released. The stretching cycle was repeated
three times. The original length (L0)
and the length after stretching (L1) were
measured by a caliper. The instant strain recovery was calculated
as (1 – (L1 – L0)/L0) × 100%. For cyclic
stretch, the PEG–PCL-DA hydrogel specimens (50 mm length, 5
mm width; 3 mm height; n = 3) were stretched to the
maximum strain of 30% and released back to 0% strain for 10 cycles
at a constant rate of 10 mm/min.[32]
Cell Viability
in Hydrogels
PEG–PCL-DA polymers (1.2 g) and LAP (0.015
g) were sterilized under UV radiation for 1 h and dissolved in 1 mL
of sterilized PBS to obtain 120% (w/v) PEG–PCL-DA/PBS solution
and 1.5% (w/v) LAP/PBS solution, respectively. Mouse 3T3 fibroblasts
(ATCC, Manassas, VA) in 1 mL cell culture medium (Dulbecco’s
modified Eagle’s medium supplemented with 10% fetal bovine
serum, 100 U/mL penicillin, and 100 μg/mL streptomycin) at a
density of 1.5 × 107 cells/mL was first mixed with
the PEG–PCL-DA/PBS solution and then subsequently blended with
the LAP/PBS solution. The final PEG–PCL-DA hydrogel concentration
was 40% (w/v), the final initiator concentration was 0.5% (w/v), and
the final cell density in the obtained cell/hydrogel precursor was
5 × 106 cells/mL. The cell/hydrogel precursor was
injected into a mold by a 1 mL syringe and exposed to the LED splash
lighter to form cell/hydrogel construct as described above. Standard
biopsy punches (6 mm, Miltex) were used to punch the cell/hydrogel
construct to obtain cell/hydrogel disks (6 mm diameter), which were
transferred to 24-well cell culture plates and incubated at 37 °C
in a 5% CO2 environment. The cell culture medium was exchanged
every 2 days. The cell viabilities after 1 and 3 days of incubation
in PEG–PCL-DA hydrogels (n = 5) were detected
by a mitochondrial activity assay (3-(4,5-dimethylthiazol-2-yl)-2,5-diphenyltetrazolium
bromide (MTT), Sigma) at 1 and 3 days. The MTT results were verified
using a live and dead staining (live, SYTO 10 green fluorescent nucleic
acid stain; dead, ethidium homodimer-1 nucleic acid stain, Life Technologies,
Inc.) kit to visualize the 3T3 fibroblasts in the hydrogels. The images
of live/dead stained 3T3 fibroblasts were taken on a fluorescence
microscope.
Viscosity of PEG–PCL-DA Solution
PEG–PCL-DA polymers were dissolved in PBS to create solutions
ranging from 10 to 40% (w/v). The viscosity of the polymer solutions
was measured using a falling ball viscometer (size 3, Gilmont) under
manufacturer’s instructions. A glass ball was used to measure
the viscosity of polymer solutions that were less than 10% (w/v),
and a stainless steel ball was used for the other concentrations.
Three measurements were taken for each concentration. Shear stress
within the nozzle during bioprinting is estimated using the Hagen–Poiseuille
equation: , where μ is the viscosity, Q is the mean volumetric flow rate, and d is the diameter of the needle.
Cell Printing of PEG–PCL-DA
All cell printing experiments were performed using a modified printing
platform reported in previous studies.[8] The printer consists of a dispenser mounted onto a Cartesian robotic
stage that moves in the x–y direction. Another motor-controlled stage that moves in the z direction acts as the printing substrate. The extrusion-based
dispenser is driven by a syringe pump (Harvard Apparatus); the speed
of extrusion can be controlled by programming the pump. In addition,
printing resolution can be controlled by adjusting the speed of extruder
movement, extrusion speed, and nozzle size. Syringe barrels containing
the bioink and tubing attached to the dispenser were covered in aluminum
foil to prevent premature cross-linking during the printing process.
The printing apparatus was housed in a sterile laminar flow hood to
prevent contamination. Basic geometric shapes were printed by extruding
a 20% (w/v) PEG–PCL-DA solution through an 18G needle and a
21G needle.
Cell Viability under Printing Conditions
Sterilized PEG–PCL-DA polymers of varying weight (0.1–0.3
g) were dissolved in 500 μL of media to obtain polymer/medium
solutions. Three types of media were used: fibroblast growth medium
(FGM-2, Lonza) for neonatal human lung fibroblasts, endothelial growth
medium (EGM-2, Lonza) for human umbilical vein endothelial cells,
and smooth muscle growth medium (SmGM-2, Lonza) for human aortic smooth
muscle cells. The cells were suspended in their respective media at
a concentration of 2.5 × 106 cells/mL. The cell suspension
(400 μL) was mixed with the polymer solution and then subsequently
mixed with 100 μL of LAP/PBS solution to obtain a PEG–PCL-DA
bioink with a final concentration of 10–30% (w/v), a final
initiator concentration of 0.5% (w/v), and a final cell density of
1.0 × 106 cells/mL. The resulting bioink was wrapped
in aluminum foil and kept on ice prior to printing. The bioink was
loaded into sterile 10 mL Luer Lock syringes (Becton Dickinson) and
mounted onto our printing apparatus. The bioink was extruded through
nozzles of four different gauges (18G, 21G, 23G, and 25G) at a constant
flow rate of 0.15 mL/min and photo-cross-linked for 30 s to create
cylindrical cell/hydrogel constructs. Live/dead staining (live, calcein
AM; dead, ethidium homodimer-1, Thermo Fisher Scientific) was used
to determine cell viability of cells immediately after printing (n = 3). The constructs were immersed in media and incubated
under 37 °C in a 5% CO2 environment. Media was changed
every 2 days, and live/dead staining was performed again 7 days after
printing.
Statistical Analysis
All results
are presented as mean ± standard deviation. All data were analyzed
by one-way analysis of variance, followed by a post hoc Tukey–Kramer
test. Differences were considered statistically significant when p < 0.05.
Results and Discussion
PEG–PCL-DA Polymer
Synthesis and Hydrogel Formation
The chemical structures
of synthesized PEG-DA (Figure A) and PEG–PCL-DA (Figure B) were confirmed by 1H NMR spectra.
The specific peaks of the ethylene oxide protons of the PEG segments
in PEG-DA and PEG–PCL-DA polymers were located at 3.55 and
4.20 ppm, and 3.56 and 4.09 ppm, respectively (Figure ). The methyl protons of the PCL blocks in
the PEG–PCL-DA polymer were assigned to chemical shifts between
1.22 and 3.99 ppm (Figure B). The specific peaks of the acryloyl protons in the PEG–PCL-DA
were located from 5.81 to 6.30 ppm (Figure ). The block length of the PCL–PEG–PCL
was calculated from the 1H NMR spectra and distributed
as 1863–20 000–1863 for PEG–PCL(24k) and
1151–20000–1151 for PEG–PCL(22k) (Table ). The degrees of substitution
(DS) of the acryloyl group calculated from the 1H NMR spectra
were 55, 59, and 60% for PEG-DA, PEG–PCL(22k)-DA, and PEG–PCL(24k)-DA,
respectively. The DS of the acryloyl group for PEG-DA is comparable
to the previous study,[33] which verified
the success of the acrylation.
Figure 2
1H NMR spectra of (A) PEG-DA
and (B) PEG–PCL(24k)-DA.
Table 1
Block Lengths of PCL–PEG–PCL Copolymer
Diols
copolymer diols
theoretical block length of PCL–PEG–PCL
calculated block length of PCL–PEG–PCL
PEG–PCL(24k)
2000–20 000–2000
1863–20 000–1863
PEG–PCL(22k)
1000–20 000–1000
1151–20 000–1151
1H NMR spectra of (A) PEG-DA
and (B) PEG–PCL(24k)-DA.The hydrogel was formed by
covalent cross-linking though visible-light initiation. The formed
hydrogel was transparent. The triblock PCL–PEG system was previously
designed for thermosensitive biodegradable hydrogel, which depended
on the hydrophobicity/hydrophilicity balance by changing the feeding
ratio of PEG–PCL and total macromolecular weight. The thermosensitive
PEG–PCL hydrogel was opaque and not elastic.[34−36] In contrast,
the acrylated PEG–PCL polymer in this work can form transparent
and elastic hydrogel via photopolymerization under exposure to visible
light. The selected photoinitiator, LAP, can maintain high cell viability
during direct cellular encapsulation because it has very good cell
compatibility in vitro and in vivo,[26,37] and can trigger
the photopolymerization under visible light (395–405 nm) exposure.[26] The visible light for cross-linking is much
safer than the common UV cross-linking (365 nm), and it would allow
a longer duration and safer cell printing. In addition, light cross-linking
technique is highly compatible with the current three-dimensional
printing technique.Water
absorption of PEG–PCL-DA hydrogel is summarized in Table . A decrease in water
absorption was observed with an increase in the concentration of PEG–PCL-DA
precursor solution. The water absorption of PEG–PCL(24k)-DA-10%
was 1930 ± 140%; however, it decreased to 766 ± 18% when
the concentration of PEG–PCL(24k)-DA precursor solution increased
to 40% (Table ). It
was primarily because more polymer chains involved in cross-linking
process would result in denser hydrogel mesh, which lead to lower
water absorption rate.[38]
Table 2
PEG–PCL-DA Hydrogel Characterization*,#
polymers
concentrations (%)
compressive modulus (kPa)
compressive
stress at 80% strain (kPa)
water absorption (%)
PEG–PCL(24k)-DA
40
26.7 ± 4.5a
356.8 ± 18.7a
766 ± 18a
20
14.9 ± 3.1b
162.5 ± 14.5b
1184 ± 43b
10
10.7 ± 2.5b
78.6 ± 4.5c
1930 ± 140c
PEG–PCL(22k)-DA
40
19.4 ± 1.5a
-##
971 ± 48a
20
8.9 ± 1.7b
122.4 ± 2.3a
1593 ± 51b
10
4.9 ± 0.4c
45.0 ± 5.2b
2504 ± 337c
PEG-DA
40
9.2 ± 1.8a
-##
1692 ± 296a
20
4.7 ± 0.5b
24.1 ± 2.7a
2819 ± 292b
10
1.1 ± 0.2c
8.8 ± 1.8b
3798 ± 276c
a,
b, c represent significantly different groups for each characteristic. #The compression testing of hydrogels was carried out after
immersion in PBS for 24 h. ##The PEG-DA and PEG–PCL(22k)-DA
hydrogels at 40% concentration were broken at 80% strain during the
compressive test.
a,
b, c represent significantly different groups for each characteristic. #The compression testing of hydrogels was carried out after
immersion in PBS for 24 h. ##The PEG-DA and PEG–PCL(22k)-DA
hydrogels at 40% concentration were broken at 80% strain during the
compressive test.Furthermore,
the incorporation of hydrophobic PCL segments into the network resulted
in a decrease in water absorption rate. The PEG-DA without PCL segments
had the highest water absorption rate at 1692 ± 296%. The PEG–PCL(24k)-DA
with the highest PCL content had the lowest water absorption rate
at 766 ± 18%. Additionally, there is a balance between the water
absorption from the hydrophilic PEG moiety and the enhanced mechanical
properties and elasticity majorly attributed to the hydrophobic PCL
moiety.The water absorption is important to be characterized
to predict the swollen shape and size for a bioprinted construct,[39] and it is also required to be optimal for cell
culture. However, water adsorption range appropriate for both printing
and cell survival has not been well defined yet. Some publications
have reported that materials with water absorption from 78% (PEG-alginate
hydrogel) to 1183% (GelMA/collagen hydrogel) were acceptable for printing.[20,40−42] However, the optimal hydrogel water absorption rates
for printing and cell growth are often opposing.[43,44] No strong evidence exists to show that such water absorption ranges
were good for cell culture. In our study, the water absorption rates
of PEG–PCL(24k)-DA hydrogel (766–1930%) were comparable
to the reported acceptably printable range (78–1183%). In addition,
introducing low-molecular-weight cross-linker or polymers with low
water absorption can assist in reducing the water absorption rate
of the PEG–PCL-DA hydrogel.[42,45,46]
Mechanical Properties of the PEG–PCL-DA
Hydrogel
It is a desired property that the hydrogel maintains
its elasticity under the media culture condition (wet state). We therefore
examine their mechanical properties after submerging the hydrogel
in media overnight. As shown in Figure and Video S1, the PEG–PCL(24k)-DA
hydrogel exhibited high flexibility and elasticity by withstanding
large deformations of stretching (Figure B), compression (Figure D), and twisting (Figure F) without any obvious breakage. Particularly,
after removal of the applied force, the PEG–PCL(24k)-DA hydrogel
could recover quickly from deformation. In contrast, the swollen PEG-DA
hydrogel became broken after slightly stretching (Figure A), large deformation of compression
(Figure C), and twisting
(Figure E, Video S2). The brittle nature of the PEG-DA hydrogel
is consistent with a previous study, which also showed the swollen
PEG-DA hydrogel (Mn = 20 000 g/mol)
broken upon high deformation of compression or slight stretching.[33] As determined by the compressive testing (Figures A, S2A, and Table in the Supporting Information), the initial modulus and compressive
strength at 80% strain of the PEG–PCL-DA hydrogels increased
with increasing PCL segments when the polymer concentration was fixed
(p < 0.05). The PEG–PCL(24k)-DA hydrogel
achieved a compressive stress of 356.8 ± 18.7 kPa and a compressive
modulus of 26.7 ± 4.5 kPa at 80% strain, which was around 3 times
higher than the compressive modulus of PEG-DA hydrogel (9.2 ±
1.8 kPa). The compressive stress at 80% strain of PEG-DA was not able
to be collected due to the hydrogel collapsing at 80% deformation.
The tensile properties (Figures B, S2B, and Table ) of the PEG–PCL-DA hydrogels
demonstrate similar trends with their compressive properties. The
initial modulus and tensile stress of PEG–PCL(24k)-DA hydrogel
were 37.7 ± 1.7 and 34.5 ± 2.5 kPa, which were 6.3 times
and 8.2 times higher than the initial modulus (6.0 ± 1.2 kPa)
and tensile stress (4.2 ± 1.2 kPa) of PEG-DA, respectively. There
was no significant difference on the breaking strain between the PEG–PCL(24k)-DA
(150 ± 14%), PEG–PCL(22k)-DA (145 ± 17%), and PEG-DA
(187 ± 27%) (p > 0.05). The instant recovery
of both PEG–PCL(22k)-DA and PEG–PCL(24k)-DA hydrogel
was ≥99% for three cycles at 10% strain, which was larger than
that of PEG-DA hydrogel (97 ± 1%) (p < 0.05; Table ). The PEG–PCL(24k)-DA
hydrogel had the highest suture retention strength at 0.32 ±
0.06 N/mm2, whereas the PEG-DA had the lowest suture retention
strength at 0.15 ± 0.01 N/mm2 (p <
0.05; Table ). Cyclic
stretching was carried out to study the elasticity of the PEG–PCL-DA
hydrogels at a maximum strain of 100% (Figure C). All of the hydrogels exhibited a large
hysteresis loop in the first cycle and much smaller hysteresis loops
in the next nine cycles. The irreversible deformations decreased with
the increasing block length of the PCL segments in the PEG–PCL-DA
polymer chain from PEG-DA (∼45%) to PEG–PCL(24k)-DA
(∼20%). The PEG–PCL-DA hydrogel with increasing PCL
amounts had an increasing capacity to hold their own weight when suspended
on cantilever right after gelation, which can be proved by the increasing
angles from 8° (PEG-DA) to 39° (PEG–PCL(24k)-DA)
between the hydrogels and vertical lines (Figure S3). These results suggested that the incorporation of PCL
segments enhanced the strength, toughness, flexibility, and elasticity
of the single-component hydrogel network. These observations were
mainly attributed to the hydrophobic interactions between the PCL
moieties in the hydrogel network. The hydrophobic interactions may
form a second physical network along with the chemical cross-linking
network, which may dissipate the crack energy applied along the hydrogel
sample due to the reversible dissociation of the hydrophobic interactions.[47,48] The developed PEG–PCL-DA hydrogel with good mechanical strength
and elasticity is promising for soft tissue engineering. For example,
the initial moduli of PEG–PCL(24k)-DA-40% (37.7 ± 1.7
kPa), PEG–PCL(22k)-DA-40% (28.2 ± 2.4 kPa), PEG–PCL(24k)-DA-20%
(16.4 ± 4.8 kPa), and PEG–PCL(22k)-DA-20% (10.7 ±
1.7 kPa) fall in the range of that of human myocardium (Emyocardium = 10–500 kPa).[49] The initial moduli of PEG–PCL(24k)-DA-20% (16.4 ± 4.8
kPa), PEG–PCL(24k)-DA-10% (9.4 ± 1.9 kPa), and PEG–PCL(22k)-DA-20%
(10.7 ± 1.7 kPa) are comparable to those of human muscle (Emuscle = 8–17 kPa).[50]
Figure 3
Photographs demonstrating the attractive mechanical properties
of the PEG–PCL(24k)-DA hydrogel under stretching, compression,
and twisting. (A) PEG-DA hydrogel was broken under stretching. (B)
PEG–PCL(24k)-DA hydrogel could be stretched and recoiled back
to the original length. (C) PEG-DA hydrogel was broken into pieces
under compression at 80% strain. (D) PEG–PCL(24k)-DA hydrogel
deformed and recovered under compression. (E) PEG-DA hydrogel was
broken after twisting for four cycles. (F) PEG–PCL(24k)-DA
hydrogel could be twisted for four cycles and recovered after releasing.
Figure 4
Mechanical properties of the PEG–PCL(24k)-DA
hydrogel. (A) Compressive stress–strain curves of PEG–PCL-DA
hydrogels. (B) Tensile stress–strain curves of PEG–PCL-DA
hydrogels. (C) Cyclic stretching of PEG–PCL-DA hydrogels at
100% deformation for 10 cycles.
Table 3
Tensile Testing of PEG–PCL-DA Hydrogel*,#
polymers
concentrations (%)
initial modulus (kPa)
tensile strength
(kPa)
breaking strain (%)
suture retention (N/mm2)
instant recovery (%)
PEG–PCL(24k)-DA
40
37.7 ± 1.7a
34.5 ± 2.5a
150 ± 14a
0.32 ± 0.06a
100 ± 1a
20
16.4 ± 4.8b
18.7 ± 4.3b
165 ± 25a,b
10
9.4 ± 1.9c
10.8 ± 2.6c
202 ± 27b
PEG–PCL(22k)-DA
40
28.2 ± 2.4a
25.3 ± 2.1a
145 ± 17
0.20 ± 0.02b
99 ± 1a
20
10.7 ± 1.3b
12.3 ± 1.1b
160 ± 12
10
5.5 ± 0.6c
8.6 ± 1.0c
176 ± 21
PEG-DA
40
6.0 ± 1.2a
4.2 ± 1.2a
187 ± 27a
0.15 ± 0.01c
97 ± 1b
20
1.4 ± 0.3b
1.2 ± 0.2b
102 ± 15b
10
-##
-##
-##
a,
b, c represent significantly different groups for each characteristic. #The tensile testing of hydrogels was carried out after immersion
in PBS for 24 h. The suture retention and instant recovery were measured
for hydrogels at a concentration of 40%. ##The PEG-DA-10%
hydrogel was too weak to be loaded on the MTS machine.
Photographs demonstrating the attractive mechanical properties
of the PEG–PCL(24k)-DA hydrogel under stretching, compression,
and twisting. (A) PEG-DA hydrogel was broken under stretching. (B)
PEG–PCL(24k)-DA hydrogel could be stretched and recoiled back
to the original length. (C) PEG-DA hydrogel was broken into pieces
under compression at 80% strain. (D) PEG–PCL(24k)-DA hydrogel
deformed and recovered under compression. (E) PEG-DA hydrogel was
broken after twisting for four cycles. (F) PEG–PCL(24k)-DA
hydrogel could be twisted for four cycles and recovered after releasing.Mechanical properties of the PEG–PCL(24k)-DA
hydrogel. (A) Compressive stress–strain curves of PEG–PCL-DA
hydrogels. (B) Tensile stress–strain curves of PEG–PCL-DA
hydrogels. (C) Cyclic stretching of PEG–PCL-DA hydrogels at
100% deformation for 10 cycles.a,
b, c represent significantly different groups for each characteristic. #The tensile testing of hydrogels was carried out after immersion
in PBS for 24 h. The suture retention and instant recovery were measured
for hydrogels at a concentration of 40%. ##The PEG-DA-10%
hydrogel was too weak to be loaded on the MTS machine.
In Vitro Cytocompatibility of the PEG–PCL-DA
Hydrogel
The two chemical components in the hydrogel, PEG
and PCL, are widely known as biocompatible materials, and have been
used in FDA-approved devices.[31] Hence,
we expected that the hydrogel consisting of the two moieties can possess
good cytocompatibility. The ability of the PEG–PCL-DA hydrogel
to support the encapsulated cell growth was evaluated using mouse
3T3 fibroblasts. Live/dead staining was used to determine the cell
viability in the hydrogel over 3 days of culture. In Figure A, the 3T3 fibroblasts maintained
a round morphology inside the PEG-DA hydrogel on day 1 and day 3.
However, a portion of the 3T3 fibroblasts exhibited elongated cell
morphology after 1 day culture inside the PEG–PCL(24k)-DA hydrogel,
which suggested the ability of the PEG–PCL(24k)-DA hydrogel
to support cell attachment. This might be attributed to the hydrophobic
PCL moiety, which can promote the protein adsorption to the hydrogel
and thus improve the cell–hydrogel interactions.[33,51] Cells encapsulated in PEG-based synthetic hydrogels are difficult
to spread out because the high hydrophilicity of the inert hydrogels
resists protein adhesion and cannot support interactions between cells
and the hydrogels.[52] Incorporating bioactive
components into the synthetic networks, such as proteins, peptides,
and polysaccharides, can significantly improve cell growth.[25,53,54] For example, cells with rounded
morphology were observed in PEG hydrogel; however, with the addition
of hyaluronic acid or fibrinogen, the cells exhibited spreading morphology
inside the hydrogels.[53,54] Furthermore, the cell survival
rates of the 3T3 fibroblasts inside the PEG–PCL(24k)-DA and
PEG-DA hydrogels were both over 90% from day 1 to day 3 (Figure B). There was no
significant difference in the cell viability between PEG–PCL(24k)-DA
and PEG-DA within 3 days of culture (p > 0.05)
(Figure C). The results
indicate that the PEG–PCL-DA hydrogel with good cell compatibility
can support the growth of the photoencapsulated 3T3 fibroblasts in
vitro.
Figure 5
In vitro cytocompatibility of elastic hydrogels. (A) Live and dead
stained 3T3 fibroblasts encapsulated in PEG-DA and PEG–PCL(24k)-DA
hydrogels after 1 day and 3 days of culture. (B) Cell viability calculated
as percentage of live cells (green) from the live and dead staining
images. (C) Metabolic index of 3T3 fibroblasts encapsulated in PEG-DA
and PEG–PCL(24k)-DA hydrogels.
In vitro cytocompatibility of elastic hydrogels. (A) Live and dead
stained 3T3 fibroblasts encapsulated in PEG-DA and PEG–PCL(24k)-DA
hydrogels after 1 day and 3 days of culture. (B) Cell viability calculated
as percentage of live cells (green) from the live and dead staining
images. (C) Metabolic index of 3T3 fibroblasts encapsulated in PEG-DA
and PEG–PCL(24k)-DA hydrogels.The viscosity of
the hydrogel precursors can be tuned for bioprinting. The viscosity
of the PEG–PCL-DA precursors increased exponentially with their
concentration (Figure A). In particular, precursors exceeding 30% (w/v) showed remarkable
increase in viscosity with respect to their concentration, whereas
0–20% precursor solution has very low viscosity. We envision
that different bioprinting techniques may be needed for hydrogel at
different viscosities. For example, inkjet-based printer can be used
for precursor solution below 20%. For high-concentration solutions,
extrusion-based printer will be used, which is suitable for printing
high viscous materials.
Figure 6
Cytotoxicity and printability of elastic PEG–PCL(24k)-DA
hydrogel using an extrusion bioprinter. (A) Viscosity curve of elastic
PEG–PCL(24k)-DA precursor solution. (B, C) Cell viability of
different cell types in printed 10% elastic PEG–PCL(24k)-DA
hydrogel. Live/dead assay was performed immediately after gel polymerization
and after 7 days in culture (scale bars represent 500 μm). (D)
Effect of different needle sizes and precursor solution concentrations
on viability of neonatal human lung fibroblasts. (E) Effect of shear
stress on cell viability evaluated immediately after printing. (F,
G) Sample shapes printed using a printer with different needle sizes
(scale bars in (F) represent 2 mm and scale bars in (G) represent
5 mm).
Cytotoxicity and printability of elastic PEG–PCL(24k)-DA
hydrogel using an extrusion bioprinter. (A) Viscosity curve of elastic
PEG–PCL(24k)-DA precursor solution. (B, C) Cell viability of
different cell types in printed 10% elastic PEG–PCL(24k)-DA
hydrogel. Live/dead assay was performed immediately after gel polymerization
and after 7 days in culture (scale bars represent 500 μm). (D)
Effect of different needle sizes and precursor solution concentrations
on viability of neonatal human lung fibroblasts. (E) Effect of shear
stress on cell viability evaluated immediately after printing. (F,
G) Sample shapes printed using a printer with different needle sizes
(scale bars in (F) represent 2 mm and scale bars in (G) represent
5 mm).
Cellular Printing
We printed the hydrogel loaded with the cells to test whether this
material can be applied toward bioprinting of cell–gel construct.
As for the constructs that were printed with PEG–PCL(24k)-DA
at 10% of polymer concentration, cell viability of over 83% were observed
across three different human cell types: human umbilical vein endothelial
cells, neonatal human lung fibroblasts, and human aortic smooth muscle
cells. These results suggest that the PEG–PCL-DA could potentially
be used to print a wide range of different human soft tissues. The
cells within the constructs continued to exhibit high viability after
7 days in culture printing (Figure B,C). In addition, no significant difference in cell
viability was observed with decreasing nozzle diameter immediately
after printing (Figure D). Similarly, there was no significant difference in cell viability
with increasing shear stress (Figure E). However, there was a significant decrease in cell
viability after 7 days in culture (Figure D). This could be a result of a decrease
in the rate of nutrient diffusion from the increased polymer concentration
and/or cell damage experienced from the printing process.The
PEG–PCL-DA hydrogel can also be easily printed for various
patterns. Basic geometric shapes were printed using the PEG–PCL-DA
precursor, and their resolution can be adjusted by changing the nozzle
diameter (Figure F).
Complex patterns could also be achieved by modifying the printing
pattern on our cell printing platform; however, the polymer solution
spread as it contacted the substrate, limiting the minimum feature
size (Figure G). The
chemical composition of the polymer may need to be modified to create
smaller features. There are two major factors affecting the hydrogel
shape fidelity, viscosity and swelling behavior.[43] For hydrogel swelling behavior, high levels of cross-linking
extent and charge densities will result in low swelling ratio, which,
however, will impair cell growth and migration due to reduced pore
sizes.[55] In addition, hydrogel fidelity
can also be improved by increasing its viscosity and enhancing its
shear-thinning properties. For example, micro/nanoparticles could
be incorporated into the precursor to make it more suitable for bioprinting.[20,56]
Conclusions
In summary, we have developed a visible-light
cross-linked, single-component, elastic, and biodegradable hydrogel
system based on a triblock copolymer of PEG and PCL. It is biocompatible,
biodegradable, and has tunable mechanical properties. The possessed
elastic properties are much desired for soft tissue engineering based
on the premise that the elastic material, capable of transducing the
correct mechanical stimulation to cells, will improve tissue adaptation
to biomechanical environment. Various cells can be incorporated with
the hydrogel for bioprinting. The selected two components are FDA-approved,
which is helpful for quickly translating our research into the preclinical
and clinical trials. Ultimately, this elastic hydrogel may be fully
compatible with many other recently developed biomaterial approaches,
such as incorporating biomimetic peptides, proteins, growth factors,
or other bioactive molecules, and thus allow easy optimization for
further improvement for soft tissue engineering.
Authors: Tao Xu; Cassie A Gregory; Peter Molnar; Xiaofeng Cui; Sahil Jalota; Sarit B Bhaduri; Thomas Boland Journal: Biomaterials Date: 2006-03-03 Impact factor: 12.479
Authors: Shannon E Bakarich; Robert Gorkin; Marc in het Panhuis; Geoffrey M Spinks Journal: ACS Appl Mater Interfaces Date: 2014-09-08 Impact factor: 9.229
Authors: Kaivalya A Deo; Kanwar Abhay Singh; Charles W Peak; Daniel L Alge; Akhilesh K Gaharwar Journal: Tissue Eng Part A Date: 2020-03 Impact factor: 3.845