Takanori Shimizu1,2, Nghia P Truong1, Richard Whitfield1, Athina Anastasaki1. 1. Laboratory of Polymeric Materials, Department of Materials, ETH Zurich, Vladimir-Prelog-Weg 5, 8093 Zurich, Switzerland. 2. Science & Innovation Center, Mitsubishi Chemical Corporation, 1000 Kamoshida-cho, Aoba-ku, Yokohama-shi, Kanagawa 227-8502, Japan.
Abstract
Cu(0)-reversible deactivation radical polymerization (RDRP) is a versatile polymerization tool, providing rapid access to well-defined polymers while utilizing mild reaction conditions and low catalyst loadings. However, thus far, this method has not been applied to tailor dispersity, a key parameter that determines the physical properties and applications of polymeric materials. Here, we report a simple to perform method, whereby Cu(0)-RDRP can systematically control polymer dispersity (Đ = 1.07-1.72), while maintaining monomodal molecular weight distributions. By varying the ligand concentration, we could effectively regulate the rates of initiation and deactivation, resulting in polymers of various dispersities. Importantly, both low and high dispersity PMA possess high end-group fidelity, as evidenced by MALDI-ToF-MS, allowing for a range of block copolymers to be prepared with different dispersity configurations. The scope of our method can also be extended to include inexpensive ligands (i.e., PMDETA), which also facilitated the polymerization of lower propagation rate constant monomers (i.e., styrene) and the in situ synthesis of block copolymers. This work significantly expands the toolbox of RDRP methods for tailoring dispersity in polymeric materials.
Cu(0)-reversible deactivation radical polymerization (RDRP) is a versatile polymerization tool, providing rapid access to well-defined polymers while utilizing mild reaction conditions and low catalyst loadings. However, thus far, this method has not been applied to tailor dispersity, a key parameter that determines the physical properties and applications of polymeric materials. Here, we report a simple to perform method, whereby Cu(0)-RDRP can systematically control polymer dispersity (Đ = 1.07-1.72), while maintaining monomodal molecular weight distributions. By varying the ligand concentration, we could effectively regulate the rates of initiation and deactivation, resulting in polymers of various dispersities. Importantly, both low and high dispersity PMA possess high end-group fidelity, as evidenced by MALDI-ToF-MS, allowing for a range of block copolymers to be prepared with different dispersity configurations. The scope of our method can also be extended to include inexpensive ligands (i.e., PMDETA), which also facilitated the polymerization of lower propagation rate constant monomers (i.e., styrene) and the in situ synthesis of block copolymers. This work significantly expands the toolbox of RDRP methods for tailoring dispersity in polymeric materials.
Low and high molecular
weight (MW) polymers display complementary
properties critical for various applications. For example, higher
MW materials typically possess greater mechanical strength and toughness
and higher glass transition and thermal degradation temperatures.[1−4] On the other hand, thanks to low chain entanglement and viscosity,
low MW polymers can be easily processed by extrusion and injection
molding technologies.[4] As such, preparing
polymers that contain a mixture of both high and low MW chains, more
commonly referred to as a broad molecular weight distribution or a
high dispersity, allows access to desirable materials combining the
advantageous properties of both low and high molecular weight segments.[5−7] In fact, increasing dispersity has been shown to significantly affect
mechanical, thermal, and rheological properties and also how polymers
self-assemble into nanostructured materials.[7−17]To date, high dispersity polymers have commonly been obtained
via
free radical polymerization (FRP), a method where radicals uncontrollably
react with monomers until irreversible termination occurs.[18] Although FRP generates polymers with high dispersities
(Đ = 1.5–2.0) that are suitable for
various industrial applications, this approach has poor control over
macromolecular structure, including the degree of polymerization,
dispersity range, end-group functionality, chain architecture, and
composition. Importantly, all chains are “dead”, which
makes any subsequent polymerization or modification steps impossible,
thus preventing access to block copolymers and other advanced materials.[19,20] On the other hand, controlled radical polymerization (CRP) methodologies
have been demonstrated to effectively regulate polymeric structures
and produce block copolymers with high end-group fidelity. However,
polymers prepared by CRPs typically have very low dispersities (Đ = 1.05–1.20), limiting their potential applications.[21] This limitation has therefore resulted in the
development of a whole raft of strategies whereby CRP and other polymerization
strategies can be used to prepare polymers with any desired intermediate
or high dispersity.[5−7]One of the elegant approaches for tuning dispersity
is the temporal
regulation of initiation method developed by Fors and co-workers,
where the initiator is fed in throughout a polymerization, so polymer
chains start growing at different times.[8,11,22−24] In addition, the groups of Boyer,
Junkers, Frey, Leibfarth, Guironnet, and others have independently
introduced a range of flow approaches, where dispersity can be carefully
controlled by adjusting reaction parameters.[25−34] These methods are often associated with excellent mathematical modeling
and the ability to be automated, allowing desired molecular weight
distributions to be obtained.[25,28−30,35,36] Furthermore, several batch methods have been recently developed
to tune polymer dispersity.[37−43] These include reducing the catalyst concentration in atom transfer
radical concentration (ATRP),[17,39,44−46] mixing high and low activity chain transfer agents
in reversible addition–fragmentation chain transfer (RAFT)
polymerization,[38,47] adjusting the solvent polarity
and concentration of azide in reversible complexation-mediated polymerization,[40] and using photochromic initiators to control
dispersity in cationic polymerization.[37] Other reported methods involve the modification of CRPs by either
addition of a comonomer or a termination agent[34,48,49] or blending prepurified polymers of either
different molecular weight or dispersity.[50,51] Despite these excellent recent breakthroughs, there are only limited
techniques that can give access to well-defined polymers with controlled
dispersity, hindering the widespread use of these materials.One of the most versatile polymerization methods for preparing
advanced polymeric materials is Cu(0)-reversible deactivation radical
polymerization (RDRP),[52−58] but this method has yet to be exploited to control polymer dispersity.
This is a major limitation, given that Cu(0)-RDRP utilizes very low
catalyst concentrations, typically has high polymerization rates,
and furnishes polymers with very high end-group fidelity.[59,60] This CRP method is also commonly associated with mild reaction conditions
and simple removal of the catalyst postpolymerization.[61−63] As such, access to polymers with tunable dispersity by Cu(0)-RDRP
is highly desirable. To this end, we sought a new strategy to effectively
tune dispersity. We present a system whereby, on variation of ligand
concentration, a wide range of dispersity polymers can be obtained,
with high end-group fidelity observed in all cases. Furthermore, in
situ chain extensions could be achieved, even from high dispersity
polymers, and the scope of the system could be expanded to incorporate
a lower activity complex, which allows for dispersity control in both
polyacrylates and polystyrene.
Experimental Section
Materials
and Instrumentation
All chemicals were purchased
from Sigma-Aldrich (Merck) and used as received unless otherwise stated.
Tris(2-(dimethylamino)ethyl)amine (Me6TREN) was synthesized
according to previously reported literature and distilled prior to
use.[64] Copper wire (gauge 0.25 mm) was
purchased from Sigma-Aldrich.1H NMR spectra were
recorded on a Bruker-300 Ultrashield at 25 °C using deuterated
chloroform as the solvent. Chemical shifts are given in parts per
million and are referenced to residual solvent proton signals. Size-exclusion
chromatography (SEC) was performed using an Agilent 390-LC MDS instrument,
equipped with differential refractive index (DRI) and dual wavelength
UV detectors. The system was equipped with 2× PLgel mixed C columns
(300 × 7.5 mm) and a PLgel 5 μm guard column. The eluent
was N,N-dimethylacetamide (HPLC
grade, with 0.03% w/v LiBr) run with a 1 mL/min flow rate at 40 °C.
A molecular weight calibration curve was produced using commercial
narrow molecular weight distribution poly(methyl methacrylate) standards
with molecular weights ranging from 5000 to 1.5 × 106. Samples were passed through a column of basic alumina to remove
Cu species and subsequently filtered through 0.45 μm filters
prior to injection. Experimental molar mass (Mn(SEC) and dispersity (Đ) values of
synthesized polymers were determined by conventional calibration using
Agilent SEC software. UV–vis absorbance spectra were recorded
on a JASCO V-730 spectrophotometer equipped with STR-773 water thermostated
cell holder and stirrer. Spectra were typically recorded from 400
to 1000 nm at a rate of 400 nm min–1 at 25 °C.
Matrix-assisted laser desorption ionization time-of-flight mass spectrometry
(MALDI-ToF-MS) data were recorded on an Autoflex speed time-of-flight
mass spectrometer (Bruker Daltonics, Bremen, Germany) equipped with
a Bruker smartbeamTM-II laser (355 nm wavelength) in reflection mode;
∼1000 spectra added up for processing, accumulated at a scan
rate of 2 kHz in the mass range of 600–7000 m/z; mass calibration to <5 ppm accuracy with
commercial poly(ethylene glycol) (PEG) calibrant. Solutions in THF
(HPLC grade) with dithranol as the matrix (20 mg/mL), sodium trifluoroacetate
as the cationization agent (1.0 mg/mL), and sample (20 mg/mL) were
prepared. Ten microliters of matrix solution was mixed with 2 μL
of cationization agent solution and 10 μL of sample solution,
and 1.0 μL of the mixture was applied to the target plate prior
to measurement.
General Procedure 1: Cu(0)-RDRP of MA with
Various Concentrations
of Me6TREN
In a 5 mL vial, 1 mL of DMSO, 1 mL
of MA (11.2 mmol, 100 equiv), and Me6TREN were added. EBiB
(16.4 μL, 0.112 mmol, 1 equiv) was transferred into the reaction
vessel via a microliter syringe. Concurrently, in a separate vial,
a stirrer bar wrapped with 5 cm of copper wire was immersed in 37%
HCl, stirred for 15 min, washed sequentially with water and acetone,
and dried. The stirrer bar was then placed into the reaction vessel
before it was sealed with a rubber septum and deoxygenated by bubbling
with nitrogen for 15 min. The reaction mixture was stirred at 200
rpm, and the reaction proceeded at 25 °C. Samples were taken
and analyzed via 1H NMR and SEC. A stock solution of 17.9
μL of Me6TREN was prepared in 1 mL of DMSO and used
for all reactions. For example, reactions were performed with 0.02
equiv of ligand (33 μL of stock solution, 2.2 μmol), 0.005
equiv of ligand (8.3 μL of stock solution, 0.56 μmol),
0.0025 equiv of ligand (4.2 μL of stock solution, 0.28 μmol),
and 0.00125 equiv of ligand (2.1 μL of stock solution, 0.14
μmol) to prepare PMA with dispersities of 1.07, 1.16, 1.31,
and 1.58.
General Procedure 2: Chain Extension of Poly(methyl
acrylate)
(PMA) Macroinitiator
The PMA macroinitiator was prepared
in a 5 mL vial, using 2 mL of DMSO, 2 mL of MA (22.4 mmol, 100 equiv),
and 2.6 μL of Me6TREN stock solution (0.00075 equiv,
0.17 μmol). EBiB (32.6 μL, 0.224 mmol, 1 equiv) was transferred
into the reaction vessel via a microliter syringe. Concurrently, in
a separate vial, a stirrer bar wrapped with 5 cm of copper wire was
immersed in 37% HCl, stirred for 15 min, washed sequentially with
water and acetone, and dried. The stirrer bar was then placed into
the reaction vessel, before it was sealed with a rubber septum, and
deoxygenated by bubbling with nitrogen for 15 min. The reaction mixture
was stirred at 200 rpm, and the reaction proceeded at 25 °C.
Once the reaction was complete, the PMA was then purified first by
dilution in ethyl acetate and extraction three times with sodium bromide
aqueous solution, thus removing copper salts. Magnesium sulfate was
then added to the remaining reaction mixture to remove water and the
mixture filtered. The organic phase was subsequently diluted with
acetone and then concentrated by blowing with air. This process was
repeated a total of three times, thus removing any unreacted monomer,
and the final polymer was isolated by drying in a vacuum oven at 25
°C overnight. Subsequently, a chain extension reaction was performed.
In a 5 mL vial, the PMA macroinitiator (153 mg, degree of polymerization
(DP) = 51, 0.034 mmol, 1 equiv) was dissolved in 0.5 mL of DMSO. Me6TREN (various amounts depending on target dispersity) and
MA (0.3 mL, 3.4 mmol, 100 equiv) were added. Concurrently, in a separate
vial, a stirrer bar wrapped with 5 cm of copper wire was immersed
in 37% HCl, stirred for 15 min, washed sequentially with water and
acetone, and dried. The stirrer bar was then placed into the reaction
vessel, before it was sealed with a rubber septum, and deoxygenated
by bubbling with nitrogen for 15 min. The reaction mixture was stirred
at 200 rpm, and the reaction proceeded at 25 °C. Samples were
taken and analyzed via 1H NMR and SEC.
General Procedure
3: In Situ Chain Extension of PMA Macroinitiator
A stock
solution of 4.7 μL of PMDETA was prepared in 1 mL
of DMSO. In a 5 mL vial, 12.5 μL of the stock solution (0.275
μmol, 0.0025 equiv), 0.99 mL of DMSO, and MA (1 mL, 11.2 mmol,
100 equiv) were added. EBiB (16.4 μL, 0.112 mmol, 1 equiv) was
transferred into the reaction vessel via a microliter syringe. Concurrently,
in a separate vial, a stirrer bar wrapped with 5 cm of copper wire
was immersed in 37% HCl, stirred for 15 min, washed sequentially with
water and acetone, and dried. The stirrer bar was then placed into
the reaction vessel, sealed with a rubber septum, and deoxygenated
by bubbling with nitrogen for 15 min. The reaction mixture was stirred
at 200 rpm to proceed at 25 °C. Samples were taken and analyzed
via 1H NMR and SEC. Once a near quantitative conversion
had been reached, 1.5 mL of DMSO, 1.5 mL of MA, and 0.13 mL of PMDETA
stock solution (1.22 μL) were mixed in a separate vial. The
vial was sealed with a rubber septum and deoxygenated by bubbling
with nitrogen for 15 min. Two milliliters of the mixture was transferred
into the vial in which polymerization was conducted via a gastight
syringe. Consequently, the components of the reaction mixture were
as follows: 2 mL of DMSO, PMA macroinitiator (0.112 mmol, 1 equiv),
MA (1 mL, 11.2 mmol, 100 equiv), and PMDETA (0.47 μL, 2.2 μmol,
0.02 equiv). The reaction was allowed to proceed at 25 °C, with
a stirring rate of 200 rpm.
Results and Discussion
We first explored the possibility of increasing polymer dispersity
by reducing the concentration of ligand used in Cu(0)-RDRP. Initial
experiments were performed with methyl acrylate as the monomer, ethyl-α-bromoisobutyrate
(EBiB) as the initiator, dimethyl sulfoxide (DMSO) as the solvent,
Cu(0) wire as the copper source, and Me6TREN as the ligand
(Scheme S1). Model reaction conditions
were selected with a target DP of 100, 5 cm of Cu(0) wire, and a ligand
concentration 18% that of the initiator ([MA]:[EBiB]:[Me6TREN] = 100:1:0.18).[65,66] As expected, after 3 h of polymerization,
well-defined PMA was obtained with a very low dispersity (96% conversion, Đ = 1.06, Figure S1 and Table S1, entry 1). Kinetic analysis revealed typical features of
a well-controlled polymerization with rapid initiator consumption,
more than 70% conversion achieved in just 20 min and low dispersity
values throughout the synthesis (Figures S2 and S3 and Table S2). We next reduced the amount of Me6TREN from 18 to 6% ([MA]:[EBiB]:[Me6TREN] = 100:1:0.06),
but a similarly low dispersity was obtained (Đ = 1.05, Figure S4 and Table S1, entry
2). Even on lowering the Me6TREN concentration to 2% ([MA]:[EBiB]:[Me6TREN] = 100:1:0.02), polymerization yielded PMA with a dispersity
of 1.07 (Figure a, Figures S5 and S6 and Table S1, entry 3). Although,
under the aforementioned conditions, polymer dispersity could not
be increased, it is important to highlight that low dispersity polymers
can be obtained with much lower amounts of ligand than previously
reported.[53] This finding is particularly
useful for large-scale synthesis or industrial applications as Me6TREN is a relatively expensive ligand ($167 per mL).
Figure 1
Dispersity
control of PMA synthesized with various concentrations
of ligand (2, 0.5, 0.25, and 0.1% with regard to initiator) by Cu(0)-RDRP.
In (a), size-exclusion chromatography illustrates monomodal SEC traces
with dispersities ranging from 1.07 to 1.59. In (b), the linear inverse
relationship between the ligand concentration and the dispersity is
presented, along with an equation to predict the concentration of
ligand required to obtain intermediate dispersities. [L]0 is the equivalent of ligand with respect to initiator at time zero.
Dispersity
control of PMA synthesized with various concentrations
of ligand (2, 0.5, 0.25, and 0.1% with regard to initiator) by Cu(0)-RDRP.
In (a), size-exclusion chromatography illustrates monomodal SEC traces
with dispersities ranging from 1.07 to 1.59. In (b), the linear inverse
relationship between the ligand concentration and the dispersity is
presented, along with an equation to predict the concentration of
ligand required to obtain intermediate dispersities. [L]0 is the equivalent of ligand with respect to initiator at time zero.Importantly, when we further decreased the ligand
concentration
by a factor of 4 (from 2 to 0.5%, [MA]/[EBiB]/[Me6TREN]
= 100:1:0.005), a slightly broader molecular weight distribution was
obtained (Đ = 1.16, Figure a and Table S1, entry 4). This encouraged us to continue decreasing the concentration
of ligand to 0.25% ([MA]:[EBiB]:[Me6TREN] = 100:1:0.0025)
and then to 0.125% ([MA]:[EBiB]:[Me6TREN] = 100:1:0.00125),
which resulted in final values of 1.31 and 1.59, respectively (Figure a and Figure S7 and Table S1, entries 5–7).
A further decrease in the ligand concentration, for example, to ([MA]:[EBiB]:[Me6TREN] = 100:1:0.000625), did yield an even higher dispersity
PMA (Đ = 1.76), although this was accompanied
by a pronounced deviation between theoretical and experimental molecular
weights (Figure S7 and Table S1, entry
8). These results clearly illustrate that dispersity can be effectively
tuned by simply changing the ligand concentration within a suitable
range. In all cases, the molecular weight distributions obtained were
monomodal with minimal tailing observed. Interestingly, we discovered
a fairly linear inverse relationship between the ligand concentration
and the resulting dispersity value with the equation Đ = 0.0007/[L]0 + 1.03 (for ligand equivalents between
0.02 and 0.00125 with regard to initiator, Figure b). This equation could be a useful tool
to predict the required concentration of ligand when a specific intermediate
dispersity value is targeted.To gain an insight into why a
low concentration of Me6TREN (0.125% with regard to initiator)
resulted in a high dispersity
polymer (Đ = 1.59), we performed detailed kinetics
analysis of the polymerization (Figure and Figure S8 and Table S3). The living nature of the polymerization was evidenced by a linear
dependence of ln([M]0/[M]t) with time, but a
significant contrast was observed in comparison to when higher ligand
concentrations were employed (Figure c). The Mn and Đ values remained high throughout the polymerization,
with slow initiation occurring as evidenced by 1H nuclear
magnetic resonance spectroscopy. In particular, full initiator consumption
had not occurred until more than 40% conversion had been reached (Figure b and Table S4). During this period, a gradual decrease
in Mn was observed (Mn,2h = 6800, Mn,4h = 5800, Mn,6h = 5500, Mn,8h = 5200), which was attributed to the continuous formation of new
polymer chains as a result of slow initiator consumption. Once all
initiator had been consumed, existing chains then started to propagate,
and hence, there was subsequently an increase in the Mn (Mn,12h = 5600 and Mn,24h = 7100, Figure d,e). It is noted that full initiator consumption
should be achieved in order to obtain comparable DPs and similar dispersity
values regardless of the targeted conversions. Together, these results
suggest that the ligand concentration plays an important role in determining
the rate of initiator consumption at the beginning of the polymerization.
Although with our method all of the initiator is added prepolymerization,
a phenomenon is observed that is similar to that in previous methods
where the initiator is slowly fed in throughout the polymerization.[24] Thus, polymer chains form and start to grow
at different times, resulting in various chain lengths and a broad
molecular weight distribution. The higher dispersity values were attributed
to a lower rate of deactivation which would, in theory, result in
a longer lifetime of radicals before they are capped, thus the potential
for chains to grow to a wider range of lengths during each activation/deactivation
cycle.[67,68]
Figure 2
Kinetics for the synthesis of high dispersity
PMA using a low concentration
of ligand in Cu(0)-RDRP. (a) Scheme of the polymerization reaction.
(b) Cascade of 1H NMR spectra for the different kinetic
time points. (c) Conversion vs time plot. (d) Mn and dispersity vs conversion plot. (e) Illustrates SEC data
for this polymerization.
Kinetics for the synthesis of high dispersity
PMA using a low concentration
of ligand in Cu(0)-RDRP. (a) Scheme of the polymerization reaction.
(b) Cascade of 1H NMR spectra for the different kinetic
time points. (c) Conversion vs time plot. (d) Mn and dispersity vs conversion plot. (e) Illustrates SEC data
for this polymerization.To confirm whether slow
deactivation was playing a role in increasing
the dispersity, we performed UV–vis experiments to measure
the concentration of the effective deactivator complex (CuBr2/Me6TREN) generated in our reactions. In these experiments,
we employed Cu(0) wire, EBiB, DMSO, and the various concentrations
of Me6TREN that we had previously used to tune the dispersity
(i.e., 2, 0.5, 0.25, and 0.125% with regard to initiator or 1.11,
0.278, 0.139, and 0.0695 mM, respectively). It is noted that no external
CuBr2 was added in these experiments, in agreement with
the protocol we used for the actual polymerizations. UV–vis
measurements showed that the intensity of the CuBr2/Me6TREN absorbance decreased with decreasing amounts of ligand
(Figure S9). Therefore, in line with our
initial hypothesis, lower ligand concentrations led to lower deactivation
rates and, as a result, an increased polymer dispersity.A key
parameter associated with controlled radical polymerization
is the ability to maintain high end-group fidelity, as this allows
for efficient block formation, access to advanced polymeric architectures,
as well as quantitative end-group modification. To assess this, low
(Đ = 1.08) and high dispersity PMA (Đ = 1.53) were synthesized, with the aforementioned
conditions (Figure S10 and Table S5). We
then MALDI-ToF-MS of our two dispersity extremes (Figure a,b). In both cases, a single
polymer distribution could be observed, with excellent correlation
between the observed molecular weight and the expected values for
PMA oligomers initiated by the expected ATRP initiator fragment and
terminated with an active bromine, with each peak separated by the
mass of one monomer unit. Of particular note are the isotopic splitting
patterns of the respective molecular ions observed for both the low
and the high dispersity polymer, which further support the high chain-end
fidelity obtained through our approach (Figure S11). Thus, regardless of the targeted dispersity, excellent
preservation of the active bromine could be maintained. In addition,
the increase in dispersity for the second polymer could also be evidenced
by the extended mass range of the distribution and an increase in
the number of polymeric species (Figure b).
Figure 3
MALDI-ToF-MS spectra of (a) low dispersity (Đ = 1.08) PMA prepared with 0.02 equiv of ligand and
(b) high dispersity
(Đ = 1.53) PMA prepared with 0.00075 equiv
of ligand.
MALDI-ToF-MS spectra of (a) low dispersity (Đ = 1.08) PMA prepared with 0.02 equiv of ligand and
(b) high dispersity
(Đ = 1.53) PMA prepared with 0.00075 equiv
of ligand.Considering the high end-group
fidelity achieved, the next step
was the preparation of well-defined diblock copolymers. Low dispersity
diblocks are widely reported with Cu(0)-RDRP, but blocks incorporating
medium and higher dispersities are yet to be realized.[59,60,69,70] We therefore prepared a high dispersity PMA macroinitiator, by selecting
the lowest concentration of ligand ([MA]:[EBiB]:[CuBr2]:[Me6TREN] = 100:1:0:0.00075) and, as desired, obtained a final
dispersity of 1.55 (DP51 by 1H NMR, Figure S12 and Table S6, entry 1). A chain extension experiment
was then performed using a high concentration of ligand to target
a low dispersity diblock ([MA]:[PMA-Br]:[Me6TREN] = 100:1:0.18).
A clear shift in the molecular weight distribution to higher molecular
weight and a low final dispersity were observed (ĐDB = 1.16, Figure a and Table S6, entry 2). By decreasing
the concentration of ligand, excellent control over diblock dispersity
could also be achieved, with ratios of [MA]:[PMA-Br]:[Me6TREN] equal to 100:1:0.005 and 100:1:0.0025, yielding diblocks with
final dispersities of 1.31 and 1.47, respectively (Figure b,c and Table S6, entries 3 and 4). These results demonstrate that
the dispersity of both homopolymers and diblocks can be carefully
controlled by judicious selection of a suitable ligand concentration.
Figure 4
Chain
extensions of a high dispersity PMA macroinitiator. By varying
the concentration of ligand, a diblock of (a) low, (b) medium, and
(c) high dispersity can be obtained.
Chain
extensions of a high dispersity PMA macroinitiator. By varying
the concentration of ligand, a diblock of (a) low, (b) medium, and
(c) high dispersity can be obtained.We subsequently expanded the scope of the system to prepare diblocks,
where the second block was composed of either a hydrophobic or hydrophilic
monomer. Butyl acrylate (BA) and poly(ethylene glycol) methyl ether
acrylate (PEGA) were selected as the monomers and polymerizations
were conducted with high concentrations of ligand, using a high dispersity
PMA macroinitiator (Scheme S2). P(MA-b-BA) and P(MA-b-PEGA) diblock copolymers
were obtained with monomodal molecular weight distributions, large
shifts in the molecular weight distributions, and final dispersity
values of less than 1.20 (Figure and Figures S13 and S14 and Table S7). Overall, these data show that the high end-group fidelity
of this polymerization system can be successfully exploited to provide
diblock copolymers with both tunable dispersity and hydrophobicity.
Figure 5
Dispersity
controlled diblock copolymers of (a) P(MA-b-BA) and
(b) P(MA-b-PEGA) prepared by Cu(0)-RDRP.
Dispersity
controlled diblock copolymers of (a) P(MA-b-BA) and
(b) P(MA-b-PEGA) prepared by Cu(0)-RDRP.To further expand the potential of our method, we were interested
to investigate an alternative ligand. We selected PMDETA, as it is
an inexpensive, commercially available, and widely used ligand ($100
for 250 mL).[65,71] We kept all other reaction conditions
consistent with previous experiments and performed our first reaction
with a ratio of [MA]:[EBiB]:[PMDETA] of 100:1:0.02. Similarly to Me6TREN, we also obtained PMA homopolymer with a low final dispersity
of 1.18 when using this high concentration of PMDETA (Figure a and Table S8, entry 1). On subsequent reduction of the PMDETA concentration
to 0.5 and 0.25% with respect to initiator ([MA]:[EBiB]:[PMDETA] of
100:1:0.005 and 100:1:0.0025), the molecular weight distributions
could be efficiently tuned with final dispersity values of 1.40 and
1.72 (Figure a and Table S8, entries 2 and 3). In all cases, very
high monomer conversions were observed and the initiator was fully
consumed, thus resulting in good agreement between theoretical and
experimental molecular weights (Figure S15 and Table S8). We performed in situ chain extensions by adding
a second aliquot of monomer once high conversions had been reached
(>90%). High to low and medium to low dispersity diblocks were
successfully
obtained (Figure b,c
and Figures S15 and S16 and Table S9).
The possibility to perform in situ chain extensions substantially
simplifies our method, as the need for macroinitiator purifications
can be avoided. It is noted that further decreasing the PMDETA concentration
results in even higher dispersity values. For example, with 0.125%
of PMDETA, a final dispersity of 2.04 can be obtained ([MA]:[EBiB]:[PMDETA]
of 100:1:0.00125), but there was a significant loss of initiator efficiency
and some shouldering in the molecular weight distribution (Figure S17 and Table S8, entry 4). As such, we
propose a minimum concentration of 0.125% for Me6TREN and
0.25% for PMDETA to ensure monomodal molecular weight distributions,
full initiator consumption, and high end-group fidelity.
Figure 6
PMDETA as a
ligand to tailor dispersity with Cu(0)-RDRP. SEC data
illustrate (a) monomodal traces with dispersities ranging from 1.18
to 1.72 for PMA synthesis, (b,c) in situ chain extension data from
medium and high dispersity PMA, and (d) monomodal traces with dispersities
ranging from 1.16 to 1.52 for PS synthesis.
PMDETA as a
ligand to tailor dispersity with Cu(0)-RDRP. SEC data
illustrate (a) monomodal traces with dispersities ranging from 1.18
to 1.72 for PMA synthesis, (b,c) in situ chain extension data from
medium and high dispersity PMA, and (d) monomodal traces with dispersities
ranging from 1.16 to 1.52 for PS synthesis.One of the great advantages of PMDETA’s compatibility with
our approach is that it may allow us to facilitate the polymerization
of low propagation rate constant (kp)
monomers and tailor the dispersity of the resulting polymers. We selected
styrene (S) as the monomer and performed polymerization with ethyl-2-bromopropionate
(EBP) as the initiator and a toluene/acetonitrile mixture (9:1) as
the solvent medium (Scheme S3).[72] The initial reaction was performed at 60 °C,
with a ratio of [S]:[EBP]:[PMDETA] of 100:1:0.36. With this high concentration
of ligand, a low dispersity PS was obtained (Đ = 1.16, Figure d
and Figure S18 and Table S10, entry 1).
On systematically lowering the concentration of ligand to 6, 3.5,
and 1% with respect to initiator, the dispersity of polystyrene could
be accurately tuned, yielding final dispersity values of 1.24, 1.32,
and 1.52 (Figure d
and Table S10, entries 2–4). These
preliminary data suggest that our developed strategy can also be applied
to different monomer classes (acrylates and styrene), thus expanding
the scope of the materials accessible by this approach. However, we
anticipate that controlling the dispersity of methacrylate monomers
would be more challenging, as lowering the ligand concentration would
potentially lead to cessation of the polymerization, and as such,
different reaction conditions would need to be optimized.
Conclusions
To summarize, we have successfully developed a simple Cu(0)-RDRP
method that can effectively tune polymer dispersity (Đ = 1.07–1.72). The key to our approach is to change the ligand
concentration, which allows the rates of initiation and deactivation
to be carefully regulated, thus controlling the dispersity of the
resulting polymer. High end-group fidelity is maintained during all
polymerizations, which can subsequently be exploited in the preparation
of a wide range of dispersity-controlled diblock copolymers. Importantly,
we illustrate that the lower activity copper complex formed with PMDETA
is advantageous in increasing polymerization conversions, thus allowing
for in situ diblock copolymers to be realized. Furthermore, the scope
of obtainable materials can be extended to incorporate block copolymers
of various hydrophobicities and polystyrene. Therefore, our method
significantly expands the toolbox of approaches to control dispersity,
allowing facile access to polymeric materials with not only high end-group
fidelity but also tailored dispersity.
Authors: Krzysztof Matyjaszewski; Wojciech Jakubowski; Ke Min; Wei Tang; Jinyu Huang; Wade A Braunecker; Nicolay V Tsarevsky Journal: Proc Natl Acad Sci U S A Date: 2006-10-10 Impact factor: 11.205
Authors: Théophile Pelras; Anton H Hofman; Lieke M H Germain; Anna M C Maan; Katja Loos; Marleen Kamperman Journal: Macromolecules Date: 2022-09-26 Impact factor: 6.057