Connor J Stubbs1, Joshua C Worch1, Hannah Prydderch1, Zilu Wang2, Robert T Mathers3, Andrey V Dobrynin2, Matthew L Becker4, Andrew P Dove1. 1. School of Chemistry, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, U.K. 2. Department of Chemistry, University of North Carolina-Chapel Hill, Chapel Hill, North Carolina 27599, United States. 3. Department of Chemistry, Pennsylvania State University, New Kensington, Pennsylvania 15068, United States. 4. Department of Chemistry, Mechanical Engineering and Materials Science, Biomedical Engineering and Orthopedic Surgery, Duke University, Durham, North Carolina 20899, United States.
Abstract
Stereochemistry in polymers can be used as an effective tool to control the mechanical and physical properties of the resulting materials. Typically, though, in synthetic polymers, differences among polymer stereoisomers leads to incremental property variation, i.e., no changes to the baseline plastic or elastic behavior. Here we show that stereochemical differences in sugar-based monomers yield a family of nonsegmented, alternating polyurethanes that can be either strong amorphous thermoplastic elastomers with properties that exceed most cross-linked rubbers or robust, semicrystalline thermoplastics with properties comparable to commercial plastics. The stereochemical differences in the monomers direct distinct intra- and interchain supramolecular hydrogen-bonding interactions in the bulk materials to define their behavior. The chemical similarity among these isohexide-based polymers enables both statistical copolymerization and blending, which each afford independent control over degradability and mechanical properties. The modular molecular design of the polymers provides an opportunity to create a family of materials with divergent properties that possess inherently built degradability and outstanding mechanical performance.
Stereochemistry in polymers can be used as an effective tool to control the mechanical and physical properties of the resulting materials. Typically, though, in synthetic polymers, differences among polymer stereoisomers leads to incremental property variation, i.e., no changes to the baseline plastic or elastic behavior. Here we show that stereochemical differences in sugar-based monomers yield a family of nonsegmented, alternating polyurethanes that can be either strong amorphous thermoplastic elastomers with properties that exceed most cross-linked rubbers or robust, semicrystalline thermoplastics with properties comparable to commercial plastics. The stereochemical differences in the monomers direct distinct intra- and interchain supramolecular hydrogen-bonding interactions in the bulk materials to define their behavior. The chemical similarity among these isohexide-based polymers enables both statistical copolymerization and blending, which each afford independent control over degradability and mechanical properties. The modular molecular design of the polymers provides an opportunity to create a family of materials with divergent properties that possess inherently built degradability and outstanding mechanical performance.
The stereochemistry
within synthetic polymer backbones is known
to be critical to the performance of the resultant bulk polymeric
materials. Polypropylene (PP), for example, possesses a methyl group
at each repeat unit, and the stereochemical relationship of neighboring
substituents (tacticity) significantly impacts chain-packing behavior.
By increasing the stereoregularity of these neighboring units along
the backbone (such as for isotactic polypropylene), polymer chains
can pack more efficiently, increasing material crystallinity, which
in turn results in dramatic improvements of the materials’
strength and toughness.[1] Leading bioplastics,
such as polylactic acid (PLA), have also begun utilizing stereochemistry
to enhance thermomechanical properties.[2−4] However, unlike the fundamental
difference in mechanical behavior observed in natural rubber (cis-1,4-polyisoprene), which is elastic, and gutta percha
(trans-1,4-polyisoprene), which is plastic, both
polypropylene and PLA retain plastic deformation under load irrespective
of their stereochemistry or tacticity.The unique structure
and stereoisomerism found in natural compounds
provide researchers with a strategic advantage in their endeavor toward
creating mechanically robust materials in which stereochemistry can
define the behavior.[5,6] Rigid-ring bicyclic ethers obtained
from the dehydrative cyclization of sugar hexitols have garnered substantial
attention as monomers because of their unique structural features,
imparting geometric isomerism (Scheme ).[7−22] While the most prevalent of the biosourced cyclic units is the glucose-derived
isosorbide, which is exemplified by its ubiquitous presence throughout
polymer chemistry,[7,15] the accompanying stereoisomers,
isomannide and isoidide, have received less attention. Some historic
and recent studies have reported the synthesis of isomannide- and
isoidide-containing polymers, but most lack detailed thermal and/or
mechanical characterization to fully elucidate the influence of the
stereochemistry. The isohexides all possess a bowl-shaped structure
that results from the two fused tetrahydrofuranyl rings with the hydroxyl
ring substituents in differing conformations. Beyond a few exceptions
using ring-opening polymerization[23] or
by polymerizing unsymmetrical isosorbide-based A–B monomers,[24] polymerization of isosorbide-based monomers
leads to regioirregular polymers. We hypothesized, however, that the endo–endo conformation in isomannide
and the exo–exo conformation
in isoidide would provide an opportunity to investigate if the geometric
isomerism of the isohexide could be leveraged to control the bulk
thermomechanical properties of the materials, eliminating the effects
of regiochemistry that are associated with the isosorbide derivative.
Scheme 1
Preparation of Isohexide-Containing Polyurethanes from Step-Growth
Polymerization
(a) 2-Isocyanatoethyl acrylate
(2.4 equiv), dibutyltin dilaurate (5 mol %) in THF at 22 °C,
16 h; (b) 1,8-octanedithiol (1 equiv), dimethylphenylphosphine (1
mol %) in CHCl3, −10 to 22 °C, 3 h.
Preparation of Isohexide-Containing Polyurethanes from Step-Growth
Polymerization
(a) 2-Isocyanatoethyl acrylate
(2.4 equiv), dibutyltin dilaurate (5 mol %) in THF at 22 °C,
16 h; (b) 1,8-octanedithiol (1 equiv), dimethylphenylphosphine (1
mol %) in CHCl3, −10 to 22 °C, 3 h.Herein, we report the synthesis and characterization
of isoidide-
and isomannide-based linear polymers (IIPU and IMPU, respectively)
by embracing a chemical design that allows the influence of the isohexide
stereochemistry on the properties of the resulting polymers to be
probed. In contrast to synthetic polymers such as polypropylene and
polylactide, but analogous to the unique behavior of the naturally
derived natural rubber and gutta percha,[25] an unexpectedly sharp contrast in mechanical properties was observed
between the plastic behavior of IIPU and the elastomeric behavior
of IMPU. Computational investigations suggested the stereochemistry
of the isohexide unit defines the supramolecular hydrogen-bonding
interactions within the material, which in turn define the mechanical
properties. We further exploit these differences by copolymerizing
stereoisomers and physically blending stereoisomeric homopolymers
to tune hydrolytic degradability and thermomechanical properties independently
of one another.
Results and Discussion
Incorporation
of the isoidide and isomannide stereoisomers into
high molar mass polymers was achieved by step-growth polymerization
of an isohexide-containing diacrylate (Figures S8–S11) with 1,8-octanedithiol using previously reported
phosphine-catalyzed thiol-Michael polyaddition chemistry (Scheme ).[26] While isomannide is a commercially available derivative,
isoidide was synthesized through inversion of the isomannide stereochemistry
using a facile protection and deprotection technique (Figure S1).[27] This
overall approach is also analogous to recent protocols that employ
a Mitsunobu reaction to invert the stereochemistry of isomannide.[28,29] The resultant alternating non-cross-linked homopolymers of IIPU
and IMPU were well-defined, nonsegmented, regioregular polymers (Figures S12–S15). The polymers were isolated
by direct precipitation from the reaction mixture at a high molecular
weight with broad molar mass distribution, ĐM (IIPU – Mw = 117
kDa, ĐM = 8.12; IMPU – Mw = 95 kDa, ĐM = 9.69), which was expected as a result of irreversible formation
of cyclic oligomers in the step-growth polymerization (Figure S25).[30] The
non-cross-linked architecture is supported by analysis of the materials
using size-exclusion chromatography coupled with viscometry detection
(Figure S26). The results revealed α
values ranging from 0.51 to 0.58, which is indicative of a linear,
unbranched, or non-cross-linked material in a theta/good solvent.[31]Key to our monomer design was the internal
urethane units, which
we reasoned would enhance thermomechanical properties by promoting
a strong hydrogen-bonding network[32] and
complementing the rigidity of the bicyclic isohexide geometry. IIPU
and IMPU both possess high thermal stabilities that enabled facile
processing (heated compression molding) into a flexible, free-standing
film suitable for mechanical analysis (Figure S28). We observed that thermally processed IIPU became less
transparent (indicative of crystallization) within hours of processing,
so both IIPU and IMPU films were annealed for 3 days at ambient temperature
(22 °C) before testing to ensure a thermal equilibrium had been
reached (see Supporting Information for
details). The mechanical properties of the annealed isohexide polymers
were assessed using uniaxial tensile testing until failure (Figure a, Figure S29). Both IIPU and IMPU possessed a significant strain
hardening feature leading to high ultimate tensile strength (UTS)
and tensile toughness (Table S3). IIPU
exhibited a moderate Young’s modulus (320 ± 66 MPa) and
a distinct yield point as the material entered the plastic deformation
region, the latter of which is a feature common to thermoplastic materials.
The stiffness and ductility of IIPU were comparable to commodity polyolefins,
such as high-density polyethylene (HDPE) (Figure S30). However, the strain hardening phenomenon exhibited in
IIPU (onset near ∼100% strain) resulted in a high UTS that
was more comparable to Nylon-6 (Table S3). The tough plastic behavior of IIPU was starkly contrasted against
the softer elastomeric nature of IMPU, illustrated by their nearly
2 order of magnitude difference in the Young’s moduli (IIPU E = 320 MPa, IMPU E = 4 MPa) (Figure a, Figure S29, Table S3). In addition, IMPU displayed excellent
recovery after deformation (Figure S31),
which corroborates the absence of a yield point in the tensile analysis.
To investigate the possibility that the robust mechanical properties
of both IIPU and IMPU were influenced by their large molar mass distributions
(ĐM > 8), both polymers were
prepared
with a lower dispersity (ĐM <
3) and assessed using tensile analysis. Consistent general tensile
behavior was observed between each respective polymer; that is, IMPU
was a strong elastomer and IIPU was a tough plastic regardless of
dispersity values (Figure S32, Table S3). The IMPU samples were nearly indistinguishable in their mechanical
metrics. However, for IIPU, the tensile strength and strain at break
were decreased somewhat in the sample with lower dispersity, but this
can be explained by the comparatively lower molar mass of that polymer
(Mw = 37 kDa).
Figure 1
Thermomechanical analysis
of IIPU and IMPU. (a) Representative
stress vs strain curves obtained at 10 mm·min–1, 22 °C for annealed IIPU and IMPU with Young’s modulus
(E) displayed (inset: photographs of pressed films
of IIPU and IMPU). (b) DSC thermograms of the first heating and cooling
cycle for the annealed (3 days, 22 °C) IIPU and IMPU (solid line
= heating scan and dashed line = cooling scan). (c) Time–temperature
superposition of rheological frequency sweeps of IIPU and IMPU overlaid
at 130 °C. Chain entanglement molecular weight (Me) of IIPU and IMPU is displayed.
Thermomechanical analysis
of IIPU and IMPU. (a) Representative
stress vs strain curves obtained at 10 mm·min–1, 22 °C for annealed IIPU and IMPU with Young’s modulus
(E) displayed (inset: photographs of pressed films
of IIPU and IMPU). (b) DSC thermograms of the first heating and cooling
cycle for the annealed (3 days, 22 °C) IIPU and IMPU (solid line
= heating scan and dashed line = cooling scan). (c) Time–temperature
superposition of rheological frequency sweeps of IIPU and IMPU overlaid
at 130 °C. Chain entanglement molecular weight (Me) of IIPU and IMPU is displayed.Typically, creating materials with mechanical properties that are
as divergent as IIPU and IMPU requires significant microstructure
changes to the polymer architecture (such as altering composition,
topology, and/or cross-linking); that is, one must “redesign”
the polymer system. Here, the profound difference in thermomechanical
properties appears to be solely attributed to the stereochemical differences
between the isohexide moieties. The significance of the isohexide
moiety to the polymer architecture and ultimate performance can be
further evidenced by comparison to an analogous study of alkene-containing
polyurethanes.[26] In that study, the cis/trans stereoisomerism indeed influenced
the mechanical properties of the materials, but the effect was modest
and all unsaturated polymers displayed plastic-like behavior irrespective
of the stereoisomer. This behavior has also been observed in polymers
that contain double bonds, synthesized by nucleophilic thiol-yne addition,
in which the materials retain a yield point and hence display plastic
deformation, even despite significant differences in mechanical behavior.[33−36] To our knowledge, the only exceptions from this behavior are natural
rubber and gutta percha (poly(cis-isoprene) and poly(trans-isoprene), respectively) and a recent report of a
cross-linked photoset material in which constraints imposed by the
network formation prevent association of the oligomeric chains when
low molar mass oligomers are used.[37]Encouraged by the divergent mechanical behavior of the isomeric
polymers, we then examined the influence of stereochemistry on the
thermal properties. Annealed thin films of IIPU and IMPU were compared
using differential scanning calorimetry (Figure b, Figure S33).
Both IIPU and IMPU were found to possess single glass transitions
around the same temperature (Tg ≈
15 °C), which suggests that the alternating structure of the
polymer prevents bulk phase separation. However, the DSC thermograms
indicated a distinct difference between the materials at higher temperatures.
The prominent endothermic peak (from 111 to 158 °C) observed
in the first IIPU heating cycle is characteristic of a first-order
phase transition (Tm). Subsequent heating
cycles display an exothermic cold crystallization peak (Tcc) before again melting, due to an inability to crystallize
in the cooling cycle time frame. These features are notably absent
for the IMPU sample, which indicates that the IIPU is semicrystalline,
while the IMPU sample appears to be amorphous. Annealing IIPU at a
higher temperature resulted in no significant changes to the crystallinity
or overall thermal profile of the polymer (Figure S34).To further understand how the isohexide structure
influenced the
polymer chain interactions, rheological frequency sweeps were performed
on IIPU and IMPU at various temperatures (Figure c). From this measurement, the molecular
weight between polymer entanglements (Me) can be calculated from fitting the rheology data with a reptation
model (Figure S38).[38] IIPU was calculated to have a larger Me (Me = 10.5 kDa, Ge = 1.8 MPa) than IMPU (Me = 5.7 kDa, Ge = 5.3 MPa), which
indicates that the isoidide stereochemistry leads to polymer chains
that are more linear, or less entangled, in comparison to isomannide.We performed detailed molecular dynamics simulations to highlight
the origin of the opposing mechanical properties of the IIPU and IMPU
polymers (Figures S39 and S40). Evolution
of the macromolecular conformations of two intertwined IIPU macromolecules
upon deformation (snapshots shown in Figure a) revealed that the IIPU macromolecules
have a large number of both inter- and intramolecular H-bonds in the
undeformed state (Figure b). In fact, an almost equal number of intra- and intermolecular
H-bonds is indicated by the observed ratio close to unity. A similar
analysis of the effect of the macromolecular elongation on intermolecular
interactions demonstrates striking differences between structural
transformations in IIPU and IMPU (Figure b). Under increasing deformation, the number
of intramolecular H-bonds decreases for both systems, while the number
of intermolecular bonds remains constant for IIPU yet increases for
IMPU. We postulated that this preference for formation of the intermolecular
associations in IIPU chains could be the reason that this polymer
crystallizes. To further understand the origin of crystallinity in
the IIPU polymer materials, we performed molecular dynamics simulations
of the bulk systems consisting of 75 IIPU repeat units with a degree
of polymerization, DP, of 16, at a polymer density of 0.95 g·cm–3, temperature T = 300 K, and pressure P = 1.0 atm and compared them to an equivalent system with
IMPU chains (Figure S40). These simulations
show that IIPU forms approximately 50% more H-bonds than IMPU and
is a direct consequence of the differences in the local molecular
conformations (Figure S40). Furthermore,
unlike IMPU, IIPU is capable of forming strong H-bonded associations,
which could be viewed as precursors of IIPU chain crystallization.
The observed divergence in properties between isoidide- and isomannide-based
materials highlights the power of controlling supramolecular interactions
via stereochemistry (especially ring-induced geometric isomerism)
in renewable monomer feedstocks. This is in line with a recent study
of chemically analogous, carbohydrate-derived isosorbide- and glucarodilactone-based
thermosets that demonstrated significant mechanical differences as
a consequence of divergent chain interactions; however the samples
both displayed elastomeric behavior.[39]
Figure 2
Molecular
dynamic simulations of hydrogen bonding in IIPU and IMPU
under deformation. (a) Snapshots illustrating the conformational changes
of IIPU macromolecules under deformation and highlighting the observed
intramolecular hydrogen bonding. (b) Dependence of the ratio of the
intermolecular (Ninter) hydrogen bonds
to intramolecular (Nintra) hydrogen bonds
on deformation for IIPU (left) and IMPU (right) systems. Data were
averaged over 20 different simulation runs from undeformed state.
Molecular
dynamic simulations of hydrogen bonding in IIPU and IMPU
under deformation. (a) Snapshots illustrating the conformational changes
of IIPU macromolecules under deformation and highlighting the observed
intramolecular hydrogen bonding. (b) Dependence of the ratio of the
intermolecular (Ninter) hydrogen bonds
to intramolecular (Nintra) hydrogen bonds
on deformation for IIPU (left) and IMPU (right) systems. Data were
averaged over 20 different simulation runs from undeformed state.The disparity of mechanical properties juxtaposed
against the chemical
similarity between IIPU and IMPU presented the opportunity to finely
manipulate material mechanical properties by combining the stereoisomers
either in physical blends or by copolymerization. Statistical copolymers
(co-IIIM) with controlled stereochemical composition were
obtained by varying the relative quantity of isoidide and isomannide
monomer in the feed and copolymerizing with 1,8-octanedithiol to afford
polymers. 1H NMR spectroscopy confirmed the feed ratios
of isomannide and isoidide were retained in the final polymer (Figure S41). The copolymer with 75% isoidide
content (co-II75IM25) was semicrystalline,
albeit with a significant reduction in overall crystallinity as evidenced
by a decrease of 9 J·g–1 in the total enthalpy
of melting (ΔHm) compared to IIPU
(Figure S35a, Table S3). A significant
decrease in the polymer melting range was also observed (ΔTm ≈ 60 °C, Table S3). The semicrystalline co-II75IM25 behaved like a plastic, albeit with a reduction in
overall material toughness and modulus as compared to IIPU (Figures S42a and S43). Below 75% isoidide content,
copolymer thermal properties were more influenced by isomannide than
isoidide and resulted in a series of amorphous thermoplastic elastomers
(Figure S35b,c). Both co-II50IM50 and co-II25IM75 presented with a similar tensile profile (J-shaped
curve) to the elastomeric IMPU sample and a statistically significant
(P < 0.05) increase in both strength and toughness
compared to IMPU (Figures S42b,c and S43, Table S3). Together these observations suggest that the presence
of small amounts of isoidide enhanced the mechanical performance of co-II50IM50 and co-II25IM75 without imparting crystallinity to
the samples, in contrast to the stereopure IIPU or 75% II formulations.
This feature also adds to the capacity of isoidide as an attractive
sustainable comonomer to improve toughness in existing thermoplastic
elastomer designs.Physical blending of polymers provides a
rapid and convenient method
to access a range of properties between two or more distinctly different
polymers; however it can be practically challenging to achieve desirable
physical properties in the resultant material. In many cases, immiscibility
between polymers dominates, even where the structures are very similar
(i.e., polypropylene and polyethylene), unless specific
compatibilization efforts are applied. The inherent incompatibility
often leads to macroscopic phase separation, or defects, in the blended
sample, which contributes to poor mechanical performance.[40] Moreover, miscibility limitations can be even
more exaggerated in binary blends derived from a semicrystalline/amorphous
polymer mixture,[41] but could offer advantages
in mechanical recycling of these materials. Despite IIPU and IMPU
possessing distinctly different thermomechanical properties (IIPU,
semicrystalline, plastic; IMPU, amorphous elastomer), blending of
these two polymers was accomplished without any complex compatibilization
requirements and yielded macroscopically homogeneous films (Figure a), presumably as
a result of the isomeric nature of the polymers. Polymer blends with
varying quantities of IMPU and IIPU (Figures S22–S24 and S27, Table S3) were made by a simple dissolution–precipitation
method and then melt processed into uniform films after drying. In
contrast to the copolymer samples, all physical blends were semicrystalline,
but they exhibited more complex melting behaviors compared to IIPU
(Figure d). Specifically,
the physical blends exhibited multifeatured DSC profiles, possibly
due to multiple crystalline domains within the samples, with melting
ranges between that of the IIPU homopolymer (Figure S36, Table S3). Surprisingly, the ΔHm for the blended films is greater than expected when
normalized to the molar content of isoidide in the sample (Table S3). The presence of IMPU homopolymer appeared
to enhance the crystallization efficiency of IIPU, which is a similar
phenomenon previously reported in cis- or trans-rich polyisoprene blends.[42] The semicrystalline nature of the blended samples also imbued them
with tough plastic behavior, analogous to IIPU (Figure c, Figures S44 and S45). Many polymerization methods prevent the copolymerization of monomers
that produce materials with dramatically different mechanical properties,
and, commonly, blending of polymers results in bulk phase separation
to produce plastics that have inferior properties to their respective
homopolymers.[43−49] Here, however, the postblending compatibility enabled materials
with practical mechanical properties (Figure f). This offers further opportunity to retain
the excellent material properties of IIPU and has potential application
for mechanical recycling of mixed polymer feeds.
Figure 3
(a) Image of heat-compressed
IIPU, IMPU, co-II50IM50, and bl-II50IM50 to illustrate crystallinity
differences. (b) Bulk system
simulations of co-II50IM50 and bl-II50IM50 illustrating the separation
of isoidide (white) and isomannide (red) regions. (c) DSC thermograms
of the first heating cycle of annealed IIPU, IMPU, co-II50IM50, and bl-II50IM50 at 10 K·min–1. Total enthalpy
of melting (ΔHm) calculated from
integration of all melting transitions. (d) Representative stress
vs strain tensile curves of annealed IIPU, IMPU, and both statistical
copolymers and a physical blend at 50/50 II/IM (n > 3). Mechanical testing was performed at 10 mm·min–1. (e) Normalized weight loss of IIPU, IMPU, co-II50IM50, and bl-II50IM50 discs in 1 M NaOH(aq) over
45 days at 25 °C. n = 3. (f) Table summarizing
thermomechanical properties
of blend and copolymer in comparison to IIPU and IMPU homopolymers: aYoung’s modulus; bultimate tensile strength
(UTS); cstrain at break.
(a) Image of heat-compressed
IIPU, IMPU, co-II50IM50, and bl-II50IM50 to illustrate crystallinity
differences. (b) Bulk system
simulations of co-II50IM50 and bl-II50IM50 illustrating the separation
of isoidide (white) and isomannide (red) regions. (c) DSC thermograms
of the first heating cycle of annealed IIPU, IMPU, co-II50IM50, and bl-II50IM50 at 10 K·min–1. Total enthalpy
of melting (ΔHm) calculated from
integration of all melting transitions. (d) Representative stress
vs strain tensile curves of annealed IIPU, IMPU, and both statistical
copolymers and a physical blend at 50/50 II/IM (n > 3). Mechanical testing was performed at 10 mm·min–1. (e) Normalized weight loss of IIPU, IMPU, co-II50IM50, and bl-II50IM50 discs in 1 M NaOH(aq) over
45 days at 25 °C. n = 3. (f) Table summarizing
thermomechanical properties
of blend and copolymer in comparison to IIPU and IMPU homopolymers: aYoung’s modulus; bultimate tensile strength
(UTS); cstrain at break.To understand the differences between copolymers and blends, we
undertook molecular dynamics simulations of each bulk system. In both
samples, there was a distinct regional separation between the isoidide
and isomannide domains (Figure b). The copolymer simulations showed the formation of a greater
number of smaller domains, which indicates that this microstructure
facilitates better separation between II- and IM-rich regions than
is possible in the physical blends. This was further quantified by
calculating the interfacial surface area per unit volume between the
II and IM domains (Figure b and Figure S47) with a lower
surface area being calculated in each case for physical blends (i.e., bl-II50IM50 =
0.9297 Å–1) in comparison to the copolymers
(i.e., co-II50IM50 = 1.4399 Å–1) at the same II/IM molar
ratio. We postulate that the larger IIPU domains in the physical blends
facilitate crystallization of the IIPU regions and hence promotes
the plastic behavior. This was further investigated using AFM to study
the surface morphology of co-II50IM50 and bl-II50IM50.
Evidence for phase separation is shown within the physically blended
sample, while the copolymer sample exhibits a more homogeneous morphology
(Figures S47−48).Petroleum-derived
plastics are notorious for their environmental
persistence, even under extreme conditions, due to the hydrophobicity
and homogeneity imparted by their all carbon-based backbones.[50] Without useful chemical “trigger”
points (such as oxygen and nitrogen) in the backbone of polymers,[51] environmental degradation processes are limited
and slow, and hence we also sought to demonstrate that hydrolytic
degradation could provide a further advantage for our sustainable
thermoplastic materials over traditional petrochemical-derived plastics.
A straightforward accelerated degradation experiment was used to study
this process in a rapid manner. Thin discs (ca. 0.5 mm thickness)
of IIPU and IMPU were placed in 1 M NaOH(aq), to assess
the influence of stereochemistry and composition on the rate of hydrolytic
degradation (Figure e). Polymer crystallinity is known to inhibit hydrolytic degradation
by restricting water penetration into the bulk sample,[52] and hence we postulated that differences in
degradation between IIPU and IMPU would be largely regulated by crystallinity.
Although IIPU degraded at a slower rate than amorphous IMPU, the sample
still exhibited significant mass loss within the time frame of the
study (∼25% mass loss within 45 days), showing its potential
to degrade by hydrolysis, should it be released into the environment,
or for chemical depolymerization methods[53,54] such as those used for the chemical recycling of PET.Exploration
of the hydrolytic degradation of the copolymers and
physical blends revealed that the mechanical behavior (plastic vs
elastic) could be decoupled from the inherent hydrolytic degradation.
Studying the accelerated hydrolysis of the crystalline polymer blend
(bl-II50IM50) and the analogous
amorphous copolymer (co-II50IM50) under the same conditions revealed that bl-II50IM50 degraded far more rapidly than IIPU, even
though the thermomechanical properties were comparable (Figure c–e). On the contrary, co-II50IM50 degraded significantly
slower than the IMPU despite both materials being amorphous and possessing
similar Tgs. The wettability of each homopolymer
and corresponding 50:50 physical blend or copolymer formulation was
investigated using the contact angle of the water–polymer interface
(Figure S49). The semicrystalline bl-II50IM50 was observed to be less
hydrophilic than the amorphous co-II50IM50, which suggests that this property is not driving
its increased degradation rate compared to the copolymer sample (Table S1). However, the contrasting degradation
behaviors are consistent with the separation of II and IM domains
within copolymers and physical blends (Figure b, Figure S48),
such that the slower degradation of the copolymer is influenced by
the II-based domains, which are smaller and more evenly dispersed
throughout the bulk system; the greater separation of domains in the
blended system leads to a degradation rate that is more influenced
by the IMPU. Previous systems with degradability control based on
microstructure have required precision-made sequences;[55−58] however the simplicity of the approach herein lends to the opportunity
to tune mechanical properties independent of degradation.Finally,
to further explore the degradation behavior of IMPU and
IIPU and understand how they might degrade in the ocean, a combination
of experimental and calculated physical property data was used to
predict quantitative and qualitative degradation profiles.[59] Using a qualitative model, classification trees
converted physical property data to degradation categories (i.e.,
fast, medium, slow) and placed both IIPU and IMPU as “medium”,
alongside polymers that are well known to degrade in the environment
(i.e., polyhydroxybutyrate). To calculate a quantitative degradation
profile for biotic and abiotic conditions, we adopted an equation
based on seawater temperature (Twater), Tg, crystallinity, and logP(SA)−1 (as a measure of hydrophobicity) to calculate relative
rates (krel) of seawater degradation.
IIPU and IMPU offer a unique balance of physical properties that should
facilitate seawater degradation including Tg values < ocean temperature, low degrees of hydrophobicity [i.e.,
logP(SA)−1],[60−62] and minimal
crystallinity. To quantify the contribution of abiotic hydrolysis
to degradation, we screened physical property data, including relative
rates for degradation experiments in NaOH(aq), and gained insight
from a degradation database (which contains similar functional groups
to those found in IIPU and IMPU)[59] to propose
a simple model to predict krel values
(Figures S50−51, and Table S2).
As such, the predicted rate of degradation of IIPU in seawater is
comparable to poly(ϵ-caprolactone), PCL, and is faster by approximately
an order of magnitude when compared to PLA (Figure ). Furthermore, IMPU is predicted to degrade
approximately an order of magnitude faster than IIPU (i.e., 2 orders of magnitude faster than PLA).
Figure 4
Calculated krel values for predicted
seawater degradation of isohexide-based polymers and degradable commercial
polymers: PLA and PCL.
Calculated krel values for predicted
seawater degradation of isohexide-based polymers and degradable commercial
polymers: PLA and PCL.
Conclusion
The
complex structure and stereoisomerism found in natural compounds
provide a strategic advantage in the endeavor toward creating mechanically
robust sustainable materials. The difference in fundamental deformation
behavior between isoidide- and isomannide-based materials, as well
as their outstanding mechanical features in their own right, is testament
to the potential of leveraging stereochemistry to direct supramolecular
interactions in biosourced monomer feedstocks. However, the most outstanding
feature of this system is the distinct property difference arising
from stereochemically distinct hydrogen bonding in otherwise compositionally
and stoichiometrically identical materials. Here, we have shown the
ability to independently tune, or decouple, the hydrolytic degradation
rate from the thermomechanical properties while also controlling these
features through simple copolymerization or blending strategies. Simply
put, the exhibition of intricate property manipulation presented herein
is unparalleled in the state-of-the-art materials portfolio and affords
a path to materials with on-demand property tuning that is made possible
only by stereochemistry manipulation.
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