14 research outputs found
Termination Mechanism in the Radical Polymerization of Methyl Methacrylate and Styrene Determined by the Reaction of Structurally Well-Defined Polymer End Radicals
A novel
method to determine the termination mechanism of radical
polymerization, i.e., the selectivity between disproportionation (Disp)
and combination (Comb), is developed. The method relies on product
analyses of the reaction of polymer-end radicals, which are generated
from structurally well-controlled living polymers, and the analyses
of molecular weight and end-group structure of the product polymers
by GPC, mass spectroscopy, and <sup>1</sup>H NMR unambiguously determined
the contribution of two competing pathways. The termination mechanism
in the polymerization of methyl methacrylate (MMA) and styrene was
investigated as a proof of principle of the method by using the corresponding
polymers prepared by organotellurium-mediated radical polymerization.
The ratios of Disp and Comb (<i>D</i>/<i>C</i>) of poly(methyl methacrylate) (PMMA) or polystyrene (PSt) end radicals
at 25 °C were 73/27 or 15/85, respectively, and the results agreed
well with the previous reports. The contribution of the Comb increased
at higher temperature in both cases, though the temperature dependence
was less pronounced in PSt radicals (<i>D</i>/<i>C</i> = 67/37 and 13/87 at 100 °C for PMMA and PSt, respectively).
Thermodynamic parameters were determined as ΔΔ<i>G</i><sup>‡</sup><sub>d/c</sub> = (−6.9 ±
0.3) – <i>T</i> × (−14.4 ± 1.0)
× 10<sup>–3</sup> (kJ mol<sup>–1</sup>) for PMMA
and ΔΔ<i>G</i><sup>‡</sup><sub>d/c</sub> = (−2.0 ± 0.5) – <i>T</i> × (−20.8
± 1.5) × 10<sup>–3</sup> (kJ mol<sup>–1</sup>) for PSt, in which ΔΔ<i>G</i><sup>‡</sup><sub>d/c</sub> and <i>T</i> are difference in Gibbs energy
undergoing Disp and Comb, and temperature in Kelvin, respectively,
by carrying out the same experiments between −20 to +100 °C.
The parameters reveal that Comb is enthalpically less favored but
entropically more favored than Disp in both cases. The effects of
molecular weight (chain length) were also investigated, and the <i>D</i>/<i>C</i> ratio became constant when the molecular
weight of polymers was more than about 3000
Controlled Copolymerization of 1‑Octene and (Meth)acrylates via Organotellurium-Mediated Living Radical Polymerization (TERP)
Copolymerization of 1-octene and (meth)acrylates, such
as methyl
acrylate, trifluoroethyl acrylate (TFEA), methyl methacrylate, and
trifluoroethyl methacrylate, under organotellurium-mediated living
radical polymerization (TERP) conditions was investigated. Polymerization
under thermal conditions gave copolymers with considerably broad molecular
distributions (polydispersity index [PDI] > 1.45), whereas that
under
photoirradiation greatly increased the PDI control. Structurally well-controlled
copolymers with number-average molecular weights (<i>M</i><sub>n</sub>) of 3000–18 000 and low PDIs (1.22–1.45)
were obtained. Addition of Brønsted acids, such as 1,3-C<sub>6</sub>H<sub>4</sub>[C(CF<sub>3</sub>)<sub>2</sub>OH]<sub>2</sub> and hexafluoroisopropanol, increased the insertion of 1-octene into
the copolymer. The molar fraction of 1-octene (MF<sub>oct</sub>) reached
∼0.5 in the copolymerization using TFEA as an acrylate monomer
and excess amount of 1-octene in the presence of the acid. The copolymer
was used as a macro-chain-transfer agent for the synthesis of block
copolymers. This is the first example of the use of this type of copolymer
as a macro-chain-transfer agent in the controlled synthesis of block
copolymers
Modular Synthesis of Mid-Chain-Functionalized Polymers by Photoinduced Diene- and Styrene-Assisted Radical Coupling Reaction of Polymer-End Radicals
Photoirradiation of structurally
well-defined “living”
polymers prepared by organotellurium-mediated living radical polymerization
in the presence of dienes or styrenes induced selective polymer-end
coupling reaction with the concomitant insertion of the dienes or
styrenes with >90% coupling efficiency. The number of inserted
dienes
or styrenes could be highly controlled to two molecules when acrylic
polymers were used. Therefore, various mid-chain-functionalized polymers
with well-controlled molecular and macromolecular structure in terms
of their molecular weight, molecular weight distribution, functionality,
and position were successfully synthesized by employing functionalized
dienes or styrenes. The method was applied to the facile synthesis
of mid-chain-functionalized telechelic polymers and a 4-miktoarm star
polymer with a well-controlled structure
Synthesis and Characterization of [<i>n</i>]CPP (<i>n</i> = 5, 6, 8, 10, and 12) Radical Cation and Dications: Size-Dependent Absorption, Spin, and Charge Delocalization
Radical
cations and dications of [<i>n</i>]cyclo-<i>p</i>-phenylenes ([<i>n</i>]CPPs, <i>n</i> = 5, 6,
10, and 12), which are the models of those of linear oligo-<i>p</i>-phenylenes without a terminus, were synthesized as hexafluoroantimonate
salts by the one- and two-electron chemical oxidation of CPP by NOSbF<sub>6</sub> or SbF<sub>5</sub>. The radical cations, [<i>n</i>]CPP<sup>•+</sup>, and dications, [<i>n</i>]CPP<sup>2+</sup>, exhibited remarkable bathochromic shifts in their
UV–vis–NIR absorption bands, suggesting that [<i>n</i>]CPP<sup>•+</sup> and larger [<i>n</i>]CPP<sup>2+</sup> exhibit longer polyene character than the shorter
analogues. The larger bathochromic shift was consistent with
the narrower HOMO–SOMO and HOMO–LUMO gaps in larger
[<i>n</i>]CPP<sup>•+</sup> and [<i>n</i>]CPP<sup>2+</sup>, respectively. In [<i>n</i>]CPP<sup>•+</sup>, the spins and charges were equally and fully delocalized over the <i>p</i>-phenylene rings of the CPPs, as noted by ESR. <sup>1</sup>H NMR revealed that the hydrogen of [<i>n</i>]CPP<sup>2+</sup> shifted to a high magnetic field from the neutral compounds due
to the diamagnetic ring current derived from the in-plane aromaticity
of [<i>n</i>]CPP<sup>2+</sup>. The single resonances observed
in all [<i>n</i>]CPP<sup>2+</sup> strongly suggest the complete
delocalization of the charges over the CPPs. Furthermore, the contribution
of biradical character was clarified for [10]- and [12]CPP by VT-NMR
experiment and theoretical calculation
Selective Synthesis and Crystal Structure of [10]Cycloparaphenylene
[10]Cycloparaphenylene ([10]CPP) was selectively synthesized in four steps in 13% overall yield from commercially available 4,4′-diiodobiphenyl by using mono-I–Sn exchange, Sn–Pt transmetalation, I–Pd exchange, and subsequent oxidative coupling reactions. The single-crystal X-ray structure of [10]CPP is described
Tetracyclo(2,7-carbazole)s: Diatropicity and Paratropicity of Inner Regions of Nanohoops
Three
N-substituted tetracyclo(2,7-carbazole)s were synthesized to investigate
the inner regions of nanohoops. One compound has a 5,5-dimethylnonane
bridge between two neighboring <i>anti</i>-carbazoles, which
can be used as covalently bonded “methane probes”. These
probes near the ring center are strongly shielded by local ring currents
and exhibit a singlet at δ = −2.70 ppm in <sup>1</sup>H NMR. To visualize local and macrocyclic ring currents separately,
we drew nucleus-independent chemical shift contour maps of tetracyclo(9-methyl-2,7-carbazole)
and [<i>n</i>]cycloparaphenylenes (CPPs). Local ring currents
make the interior diatropic, and paratropic regions exist only outside
the ring. Macrocyclic ring currents in [5]CPP to [7]CPP generate deshielding
cones, which are typical of antiaromatic [4<i>n</i>]annulenes
Tetracyclo(2,7-carbazole)s: Diatropicity and Paratropicity of Inner Regions of Nanohoops
Three
N-substituted tetracyclo(2,7-carbazole)s were synthesized to investigate
the inner regions of nanohoops. One compound has a 5,5-dimethylnonane
bridge between two neighboring <i>anti</i>-carbazoles, which
can be used as covalently bonded “methane probes”. These
probes near the ring center are strongly shielded by local ring currents
and exhibit a singlet at δ = −2.70 ppm in <sup>1</sup>H NMR. To visualize local and macrocyclic ring currents separately,
we drew nucleus-independent chemical shift contour maps of tetracyclo(9-methyl-2,7-carbazole)
and [<i>n</i>]cycloparaphenylenes (CPPs). Local ring currents
make the interior diatropic, and paratropic regions exist only outside
the ring. Macrocyclic ring currents in [5]CPP to [7]CPP generate deshielding
cones, which are typical of antiaromatic [4<i>n</i>]annulenes
In-Plane Aromaticity in Cycloparaphenylene Dications: A Magnetic Circular Dichroism and Theoretical Study
The electronic structures of [8]cycloparaphenylene
dication ([8]CPP<sup>2+</sup>) and radical cation ([8]CPP<sup>•+</sup>) have been investigated by magnetic circular dichroism (MCD) spectroscopy,
which enabled unambiguous discrimination between previously conflicting
assignments of the UV–vis–NIR absorption spectral bands.
Molecular orbital and nucleus-independent chemical shift (NICS) analysis
revealed that [8]CPP<sup>2+</sup> shows in-plane aromaticity with
a (4<i>n</i> + 2) π-electron system (<i>n</i> = 7). This aromaticity appears to be the origin of the unusual stability
of the dication. Theoretical calculations further suggested that not
only [8]CPP<sup>2+</sup> but also all [<i>n</i>]CPP (<i>n</i> = 5–10) dications and dianions exhibit in-plane
aromaticity
Near-Infrared Fluorescence from In-Plane-Aromatic Cycloparaphenylene Dications
Cycloparaphenylenes
(CPPs) are hoop-shaped conjugated hydrocarbons
corresponding to partial structures of fullerenes or armchair carbon
nanotubes. Here, we examined the fluorescence properties of a series
of [<i>n</i>]cycloparaphenylene dications ([<i>n</i>]CPP<sup>2+</sup>, <i>n</i> = 5–9), which have unique
in-plane aromaticity. The fluorescence peak positions of the [<i>n</i>]CPP<sup>2+</sup>s shifted to the longer-wavelength region
with increasing ring size, reaching the near-infrared region for those
with <i>n</i> > 5. The fluorescence quantum yield of
[6]CPP<sup>2+</sup> was the highest among the [<i>n</i>]CPP<sup>2+</sup>s examined in this study, and the value was on the same order
as
that of carbon nanotubes. The Stokes shifts of [<i>n</i>]CPP<sup>2+</sup>s were smaller than those of neutral [<i>n</i>]CPPs, which do not have in-plane aromaticity. Theoretical calculations
indicate that [<i>n</i>]CPP<sup>2+</sup>s undergo smaller
structural changes upon S<sub>0</sub>–S<sub>1</sub> transition
than [<i>n</i>]CPPs do, and this is responsible for the
difference of the Stokes shift. Furthermore, molecular orbital analysis
reveals that the S<sub>0</sub>–S<sub>1</sub> transition of
smaller [<i>n</i>]CPP<sup>2+</sup>s has an electric-dipole-forbidden
character due to HOMO → LUMO/HOMO → LUMO+1 mixing. The
relatively high fluorescence quantum yield of [6]CPP<sup>2+</sup> is
considered to arise from the balance between relatively allowed character
and the dominant effect of energy gap
Radical Ions of Cycloparaphenylenes: Size Dependence Contrary to the Neutral Molecules
Cycloparaphenylenes (CPPs) have attracted wide attention because of their interesting properties owing to distorted and strained aromatic systems and radially oriented p orbitals. For application of CPPs, information on their charged states (radical cation and radical anion) is essential. Here, we measured absorption spectra of the radical cations and the radical anions of CPPs with various ring sizes over a wide spectral region by means of radiation chemical methods. The peak position of the near-IR bands for both the radical cation and the radical anion shifted to lower energies with an increase in the ring size. This trend is contrary to what is observed for transitions between the HOMO and LUMO of the neutral CPP. The observed spectra of the CPP radical ions were reasonably assigned based on time-dependent density functional theory. These results indicate that the next HOMO and the next LUMO levels are important in the electronic transitions of radical ions