13 research outputs found
Changes in the Electronic Transitions of Polyethylene Glycol upon the Formation of a Coordinate Bond with Li<sup>+</sup>, Studied by ATR Far-Ultraviolet Spectroscopy
This study investigates the electronic transitions of
complexes
of lithium with polyethylene glycol (PEG) by the absorption bands
of solvent molecules via attenuated total reflectance spectroscopy
in the far-UV region (ATR–FUV). Alkali-metal complexes are
interesting materials because of their functional characteristics
such as good ionic conductivity. These complexes are used as polymer
electrolytes for Li batteries and as one of the new types of room-temperature
ionic liquids, termed solvation ionic liquids. Considering these applications,
alkali-metal complexes have been studied mainly for their electrochemical
characteristics; there is no fundamental study providing a clear understanding
of electronic states in terms of electronic structures for the ground
and excitation states near the highest occupied molecular orbital–lowest
occupied molecular orbital transitions. This study explores the electronic
transitions of ligand molecules in alkali-metal complexes. In the
ATR–FUV spectra of the Li–PEG complex, a decrease in
intensity and a large blue shift (over 4 nm) were observed to result
from an increase in the concentration of Li salts. This observation
suggests the formation of a complex, with coordinate bonding between
Li+ and the O atoms in PEG. Comparison of the experimental
spectrum with a simulated spectrum of the Li–PEG complex calculated
by time-dependent density functional theory indicated that changes
in the intensities and peak positions of bands at approximately 155
and 177 nm (pure PEG shows bands at 155, 163, and 177 nm) are due
to the formation of coordinate bonding between Li+ and
the O atoms in the ether molecule. The intensity of the 177 nm band
depends on the number of residual free O atoms in the ether, and the
peak wavelength at approximately 177 nm changes with the expansion
of the electron clouds of PEG. We assign a band in the 145–155
nm region to the alkali-metal complex because we observed a new band
at approximately 150 nm in the ATR–FUV spectra of very highly
concentrated binary mixtures
Infrared Spectroscopy and X-ray Diffraction Studies of Thermal Behavior and Lamella Structures of Poly(3-hydroxybutyrate-<i>co</i>-3-hydroxyvalerate) (P(HB-<i>co</i>-HV)) with PHB-Type Crystal Structure and PHV-Type Crystal Structure
Thermal behavior and lamella structures of poly(3-hydroxybutyrate-co-3-hydroxyvalerate), hereafter P(HB-co-HV) (HV = 9, 15, 21, 28.8, 58.4, 73.9, and 88.6 mol %), were investigated using infrared (IR) spectroscopy, wide-angle X-ray diffraction (WAXD), and differential scanning calorimetry (DSC). Temperature-dependent IR and WAXD measurements revealed that P(HB-co-HV) with low HV content (HV = 9, 15, and 21 mol %) has a PHB-type crystal structure with CH3···OC hydrogen bonds, whereas P(HB-co-HV) with high HV content (HV = 73.9 and 88.6 mol %) has a PHV-type crystal structure with CH2···OC hydrogen bonds. The results of IR measurements showed that the strength of the CH3···OC hydrogen bonds in the P(HB-co-HV) (HV = 9, 15, and 21 mol %) copolymers is almost the same as that in PHB, whereas in the P(HB-co-HV) (HV = 28.8 mol %) copolymer, the hydrogen bonds become weaker. In the case of P(HB-co-HV) with higher HV content (HV = 73.9 and 88.6 mol %), the effect of lamella packing on CH2···OC hydrogen bonding in the PHV crystal is not considerable because the side chain of the HB unit is shorter than that of the HV unit. Additionally, it seems that in the crystal structure of P(HB-co-HV) (HV = 58.4 mol %) there are only very weak intermolecular interactions between a CO group and either a CH2 group or a CH3 group because the region of transition of the crystal structure of P(HB-co-HV) from the PHB type to the PHV type occurs at around 50 mol % HV content. Therefore, it is very much possible that with increasing temperature the crystal structure of P(HB-co-HV) (HV = 58.4 mol %) is more likely to collapse than other P(HB-co-HV) copolymers
Effects of Hydrogen Bond Intermolecular Interactions on the Crystal Spherulite of Poly(3-hydroxybutyrate) and Cellulose Acetate Butyrate Blends: Studied by FT-IR and FT-NIR Imaging Spectroscopy
The crystal melting behaviors of poly(3-hydroxybutyrate)
(PHB) and cellulose acetate butyrate (CAB) blends were studied using
infrared (IR) and near-infrared (NIR) imaging, which provided information
about spherulite growth in dynamic blend systems. By analyzing the
changes in the IR and NIR imaging spectra in the regions of the first
and second overtones of the CO stretching vibrations of PHB
and CAB, the evolution of heterogeneous spherulite during the time-resolved
isothermal crystallization process was explored. Time-resolved IR
and NIR imaging and polarized microscopic studies detected the PHB
domains are able to separate from the PHB/CAB blends early in the
process. Principal component analysis (PCA) was used to classify the
distribution of the different morphologies of spherulite. The first
principal component suggests that the discrimination of the imaging
spectra relies largely upon the crystallinity, while the second principal
component indicates the variations in the amorphous portion of PHB,
the CAB contents, and the intermolecular hydrogen bonding of PHB and
CAB. The PC1–PC2 scores of different parts of the spherulite
suggest that the areas of low crystallinity in the blend spherulite
contain both PHB and CAB
sj-pdf-1-asp-10.1177_00037028221086913 – Supplemental Material for A Study of C=O…HO and OH…OH (Dimer, Trimer, and Oligomer) Hydrogen Bonding in a Poly(4-vinylphenol) 30%/Poly(methyl methacrylate) 70% Blend and its Thermal Behavior Using Near-Infrared Spectroscopy and Infrared Spectroscopy
Supplemental Material, sj-pdf-1-asp-10.1177_00037028221086913 for A Study of C=O…HO and OH…OH (Dimer, Trimer, and Oligomer) Hydrogen Bonding in a Poly(4-vinylphenol) 30%/Poly(methyl methacrylate) 70% Blend and its Thermal Behavior Using Near-Infrared Spectroscopy and Infrared Spectroscopy by Harumi Sato, Yusuke Morisawa, Satoshi Takaya and Yukihiro Ozaki in Applied Spectroscopy</p
Thermally Induced Exchanges of Hydrogen Bonding Interactions and Their Effects on Phase Structures of Poly(3-hydroxybutyrate) and Poly(4-vinylphenol) Blends
Effects of various hydrogen bondings (HBs) and thermally induced exchanges of them on cold crystallization and melting of poly(3-hydroxybutyrate) (PHB) and poly(4-vinylphenol) (PVPh) blends were explored as a function of the PVPh weight fraction (wPVPh) by using Fourier transform infrared spectroscopy. The HBs investigated in this work include intramolecular HBs within PHB crystals (intra PHB) as observed in the CO and CH stretching band regions, intramolecular HBs within PVPh (intra PVPh) as observed in the OH stretching band region, and intermolecular HBs (inter) between the CO groups of PHB in amorphous phase and the OH groups of PVPh. The results elucidated the following pieces of evidence. (i) Inter and intra PVPh suppress the rate of the crystallization and hence the crystallinity of PHB crystals in the blend via formation of physical cross-links in PHB and PVPh chains in the amorphous phase or melt. The crystallization and melting occur in two steps: (ii) the crystallization involves the dissociation of inter and intra PVPh, followed by the association of intra PHB and the reassociation of intra PVPh; (iii) the melting involves the dissociation of intra PHB, followed by the association of inter. (iv) Among CO groups of PHB in the melt blends existing in either free CO or inter, the fraction of inter linearly increases with wPVPh, which in turn suppresses the PHB crystallinity under given crystallization conditions to a greater extent due to an increased number of physical cross-links and hence due to the suppressed crystallization rate
Quantum Mechanical Interpretation of Intermolecular Vibrational Modes of Crystalline Poly‑(<i>R</i>)‑3-Hydroxybutyrate Observed in Low-Frequency Raman and Terahertz Spectra
Low-frequency vibrational bands observed in the Raman
and terahertz
(THz) spectra in the region of 50–150 cm–1 of crystalline powder poly-(R)-3-hydroxybutyrate
(PHB) were assigned based on comparisons of the Raman and THz spectra,
polarization directions of THz absorption spectra, and their congruities
to quantum mechanically (QM) calculated spectra. This combination,
Raman and THz spectroscopies and the QM simulations, has been rarely
adopted in spite of its potential of reliable assignments of the vibrational
bands. The QM simulation of a spectrum has already been popular in
vibrational spectroscopies, but for low-frequency bands of polymers
it is still a difficult task due to its large scales of systems and
a fact that interactions among polymer chains should be considered
in the calculation. In this study, the spectral calculations with
the aid of the Cartesian-coordinate tensor transfer (CCT) method were
applied successfully to the crystalline PHB, which include the explicit
consideration of an intermolecular interaction among helical polymer
chains. The agreements between the calculations and the experiments
are good in both the Raman and THz spectra in terms of spectral shapes,
frequencies, and intensities. A Raman active band at 79 cm–1 was assigned to the intermolecular vibrational mode of the out-of-plane
CO + CH3 vibration. A polarization state of the
corresponding far-infrared absorption band at ∼82 cm–1, perpendicular to the helix-elongation direction of PHB, was reproduced
only under the explicit correction, which indicates that this polarized
band originates from the interaction among the polymer chains. The
calculation explored that the polarization direction of this band
was along the a axis, which is consistent with the
direction in which weak intermolecular hydrogen bonds are suggested
between the CO and CH3 groups of two parallel polymer
chains. The results obtained here have confirmed sensitivity of the
low-frequency vibrational bands to the weak hydrogen bonds among the
polymer chains
Low-Frequency Vibrational Modes of Poly(glycolic acid) and Thermal Expansion of Crystal Lattice Assigned On the Basis of DFT-Spectral Simulation Aided with a Fragment Method
Low-frequency
vibrational modes of lamellar crystalline poly(glycolic
acid) (PGA) were measured on Raman and far-infrared (FIR) spectra.
Among the observed bands, an FIR band at ∼70 cm–1 and a Raman band at 125 cm–1 showed a gradual
lower-frequency shift with increasing temperature from 20 °C
to the melting point at ∼230 °C. Their polarization direction
was perpendicular to the chain axis of PGA. Both spectra were quantum-mechanically
simulated with the aid of a fragment method, the Cartesian-coordinate
tensor transfer, which enabled an explicit consideration of molecular
interactions between two adjacent polymer chains. Good agreement was
achieved between the experiment and theory in both spectra. The temperature-sensitive
bands at ∼70 cm–1 in FIR and at 125 cm–1 in Raman comprise the out-of-plane CO bending
motion. The temperature-dependent shifts of the low-frequency bands
were successfully simulated by the DFT-spectral calculation, exploring
that the main origin of the shifts is the thermal expansion of the
crystal lattice. This result indicates that the thermally shifted
bands may be used as an indicator of the lattice expansion of PGA.
Possible changes in intermolecular interactions of PGA under temperature
rising were ascribed on the basis of natural bond orbital theory.
The steric repulsion between the carbonyl O atom in one chain and
the H–C bond in the adjacent chain will be a dominant interaction
in the lattice-expanding process, which would cause the observed thermal
shifts of the bending modes. Comparisons of the spectral assignment
for PGA obtained in this study and that for poly-(R)-3-hydroxybutyrate (PHB) reported by us suggest that crystalline
polyesters give vibrational modes composed of out-of-plane bending
motion of CO groups between ∼70 and ∼125 cm–1, the modes of which are sensitive to the thermal
expansion of crystal lattice and its concomitant changes in their
intermolecular interactions
Rydberg and π–π* Transitions in Film Surfaces of Various Kinds of Nylons Studied by Attenuated Total Reflection Far-Ultraviolet Spectroscopy and Quantum Chemical Calculations: Peak Shifts in the Spectra and Their Relation to Nylon Structure and Hydrogen Bondings
Attenuated total reflection far-ultraviolet
(ATR-FUV) spectra in
the 145–260 nm region were measured for surfaces (thickness
50–200 nm) of various kinds of nylons in cast films to explore
their electronic transitions in the FUV region. ATR-FUV spectra show
two major bands near 150 and 200 nm in the surface condensed phase
of nylons. Transmittance (Tr) spectra were also observed in particular
for the analysis of valence excitations. Time-dependent density functional
theory (TD-DFT/CAM-B3LYP) calculations were carried out using the
model systems to provide the definitive assignments of their absorption
spectra and to elucidate their peak shifts in several nylons, in particular,
focusing on their crystal alignment structures and intermolecular
hydrogen bondings. Two major bands of nylon films near 150 and 200
nm are characterized as σ-Rydberg 3p and π–π*
transitions of nylons, respectively. These assignments are also coherent
with those of liquid <i>n</i>-alkanes (<i>n</i> = 5–14) and liquid amides observed previously. The Rydberg
transitions are delocalized over the hydrocarbon chains, while the
π–π* transitions are relatively localized at the
amide group. Differences in the peak positions and intensity were
found in both ATR- and Tr-FUV spectra for different nylons. A red-shift
of the π–π* amide band in the FUV spectra of nylon-6
and nylon-6/6 models in α-form is attributed to the crystal
structure pattern and the intermolecular hydrogen bondings, which
result in the different delocalization character of the π–π*
transitions and transition dipole coupling
Combined X‑ray Reflectivity and Infrared Study of the Effect of Hydrogen Bonding of the OH Group on the Relaxation Behavior in Ultrathin Polyvinylphenol Films on SiO<sub>2</sub>
Utilizing X-ray reflectivity and infrared reflection
absorption
spectroscopy (IR-RAS), we have investigated the thermal expansion
and contraction of ultrathin polyvinylphenol (PVPh) films supported
on a silicon (100) substrate capped with an amorphous SiO2 layer. Despite being known to form strong interactions with the
SiO2 surface, the thin PVPh films showed a reduction in
the glass-transition point Tg, similar
to the behavior of polystyrene thin films deposited on SiO2. We explored the relationship between thermal expansivity and film
thickness using well-annealed films and found that it decreases with
film thickness in the range below twice the radius of gyration of
a polymer chain (2Rg) in the glassy state.
Thickness expansion in the glassy state and contraction in thickness
at temperatures higher than Tg bulk (melt state) showed the presence of two competing relaxation processes.
The reported negative thermal expansion in PVPh thin films, which
was discovered to be one of the inherent properties, may have been
caused by the fast relaxations that take place at the free polymer
surface. IR-RAS was utilized to investigate the effect of thickness
on hydrogen bonding in PVPh, and it was confirmed that with decreasing
thickness, hydrogen bonding becomes weak, and the number of free OH
groups increases. Therefore, thinner PVPh samples exhibit lower Tgs as an effect of easier molecular motions
