9 research outputs found
Density and Viscosity Study of Interactions of Some Amino Acids in Aqueous Solutions of Sodium Benzoate
The density (Ï)
and viscosity (η) of three amino acids,
glycine, l-alanine, and l-valine, have been determined
as a function of amino acid concentration in aqueous solutions of
0.1011, 0.3088, and 0.5245 mol·kg<sup>â1</sup> sodium
benzoate at temperatures 303.15, 308.15, and 313.15 K. Apparent molar
volumes (<i>V</i><sub>Ï</sub>), limiting values of
apparent molar volumes (<i>V</i><sup>0</sup><sub>Ï</sub>), and transfer volumes (Î<sub>t</sub><i>V</i><sup>0</sup><sub>Ï</sub>) have been calculated from the density
data. The viscosity data could be fit to the JonesâDole equation,
and <i>B</i> coefficients and variation of <i>B</i> with temperature d<i>B</i>/d<i>T</i> were obtained
at different concentrations and temperatures. Free energies of activation
of the solvent (ÎÎŒ<sub>1</sub><sup>0â </sup>) and
solute (ÎÎŒ<sub>2</sub><sup>0â </sup>) were also
calculated by application of the Eyring transition-state theory. The
obtained thermophysical data have been interpreted in terms of the
structure of the amino acids and their interactions with the sodium
benzoate solution
Transport Properties of the 1âHexyl-3-methylimidazolium Bis(trifluoromethylsulfonyl)amideâTrichloromethane Binary System: Indication of Trichloromethane Segregation
Self-diffusion coefficients
and electrical conductivity were studied
for the binary system 1-hexyl-3-methylimidazolium bisÂ(trifluoromethylsulfonyl)Âamideâtrichloromethane
([C<sub>6</sub>mim]Â[NTf<sub>2</sub>]âCHCl<sub>3</sub>) as a
function of composition and temperature. Self-diffusion coefficients
of cation and anion are identical for ionic liquid mole fractions <i>x</i><sub>IL</sub> < 0.95. The self-diffusion coefficient
of CHCl<sub>3</sub> is consistently larger than that of the ions by
a factor of 4. A double logarithmic plot for the ratio of self-diffusion
coefficient and temperature versus viscosity is linear for ionic liquid
mole fractions 0.1 < <i>x</i><sub>IL</sub> < 0.9 indicating
(a) a fractional StokesâEinstein applies where self-diffusion
is inverse proportional to some power <i>b</i> of viscosity
(<i>D</i> ⌠η<sup>â<i>b</i></sup>) and (b) single average length scales are associated with
the mass transport of [C<sub>6</sub>mim]Â[NTf<sub>2</sub>] and CHCl<sub>3</sub>. However, the obtained length scale for CHCl<sub>3</sub> is
unreasonably small, which is indicative of CHCl<sub>3</sub> segregation.
The molar conductivity displays a maximum near <i>x</i><sub>IL</sub> = 0.2. Evaluation of the ionicity from molar conductivity
and self-diffusion coefficients indicates a gradual speciation change
from charged species to neutral species for <i>x</i><sub>IL</sub> < 0.5. The temperature dependencies of self-diffusion
and molar conductivity follow Arrhenius behavior. The obtained <i>x</i><sub>IL</sub>-dependent activation energies are found to
be linear for molar conductivity and largest for the cation and anion
self-diffusion coefficients. The activation energies for the self-diffusion
of CHCl<sub>3</sub> appear to be identical with those obtained from
fluidity data
Comparing Composition- and Temperature-Dependent Excess Molar Volumes of Binary Systems Involving Ionic Liquids
A total
of 167 data sets of composition- and temperature-dependent
excess molar volumes, <i>V</i><sup>E</sup>, which are derived
from density measurements, for ionic liquidâmolecular solvent
binary systems are inspected concerning their temperature dependence
at fixed compositions. It is found that the <i>V</i><sup>E</sup> temperature dependence is generally linear regardless of
the sign and shape of the <i>V</i><sup>E</sup> composition
dependence. Plotting the slopes and intercepts of the linear <i>V</i><sup>E</sup> temperature dependence as a function of composition
allows for convenient comparisons of existing data sets. In doing
so, <i>V</i><sup>E</sup> data sets are critically examined
with respect to data quality as well as obtaining insight into structureâproperty
relationships. This study also includes new density measurements for
the binary systems 1-hexyl-3-methylimidazolium bisÂ(trifluoroÂmethylÂsulfonyl)Âamideâchloroform
and 1-butyl-3-methylimidazolium methylsulfonateâwater, measured
in the respective temperature ranges of (288.15 and 318.15) K and
(298.15 and 358.15) K
Combining Freezing Point Depression and Self-Diffusion Data for Characterizing Aggregation
The
colligative property freezing point depression is evaluated
as a means for estimating the extent of aggregation for solutions
of polyÂ(ethylene oxide) alcohol (C<sub>10</sub>E<sub>6</sub>) nonionic
surfactant in cyclohexane. Combined with additional measurements of
self-diffusion coefficients, it is shown that both unaggregated C<sub>10</sub>E<sub>6</sub> as well as reverse micelles are significantly
present for the entire range of measured C<sub>10</sub>E<sub>6</sub> concentration (0.048â2.35 mol kg<sup>â1</sup>). A
change in speciation near 0.2 mol kg<sup>â1</sup> is indicated
by the results from both freezing point depression and self-diffusion
coefficient measurements. It is shown that average reverse micelle
radii and aggregation numbers obtained from the ratio of solvent and
C<sub>10</sub>E<sub>6</sub> self-diffusion coefficients are consistent
with prior reported results. However, unreasonably small radii for
the reverse micelles as well as for the cyclohexane were obtained
from analysis of the results by the StokesâEinstein equation
using additional measured solution viscosities. The concentration
of reverse micelles and unaggregated C<sub>10</sub>E<sub>6</sub> was
calculated from the freezing point depression results using the aggregation
numbers obtained from ratio of self-diffusion coefficients. These
concentrations indicate that the reverse micelles become smaller in
average size and increase in number with increasing temperature without
an increase in unaggregated C<sub>10</sub>E<sub>6</sub>
Comparative Study of the Magnetic Field Dependent Signal Enhancement in Solid-State Dynamic Nuclear Polarization Experiments
A detailed
study of the magnetic field dependent signal enhancement
in solid-state dynamic nuclear polarization (DNP) experiments is presented
for a specific sample consisting of AMUPol dissolved in the nonionic
surfactant C<sub>10</sub>E<sub>6</sub>. C<sub>10</sub>E<sub>6</sub> displays a superposition of âdirectâ and âindirect
channelâ resonances in <sup>13</sup>C MAS DNP NMR spectra.
The shapes of the DNP enhancement profiles are essentially identical
for the <sup>1</sup>H MAS, <sup>1</sup>H â <sup>13</sup>C CP
MAS, and <sup>13</sup>C MAS indirect channel signals, which confirms
that the same polarization transfer process from electron to proton
is responsible for the obtained enhancements of these experiments.
The shape of the DNP enhancement profiles of <sup>1</sup>H and of <sup>13</sup>C direct channel resonances reveals that the cross effect
is the dominant polarization transfer mechanism for the studied sample.
The magnitudes of the <sup>13</sup>C MAS DNP enhancement profiles
for <sup>1</sup>H â <sup>13</sup>C CP MAS, direct and indirect
channel signals were found to be not uniform. For <sup>1</sup>H â <sup>13</sup>C CP MAS and the indirect channel signals, this observation
is related to relaxation effects of the methyl group carbon. For the <sup>13</sup>C MAS direct channel resonances, differences in magnitudes
are discussed in terms of preferential structural orientation of the
polar ethylene oxide headgroup of C<sub>10</sub>E<sub>6</sub> toward
the AMUPol radical
Comparing Composition- and Temperature-Dependent Viscosities of Binary Systems Involving Ionic Liquids
More than 200 composition- and temperature-dependent
viscosity
datasets for binary systems involving ionic liquids are analyzed with
the Arrhenius model to inspect the composition dependence of the Arrhenius
fit parameters activation energy, <i>E</i><sub>a</sub>,
and <i>y</i>-intercept, ln <i>A</i>. The
analysis also includes a new viscosity dataset for the binary system
1-hexyl-3-methylimidazolium bisÂ(trifluoromethylsulfonyl)Âamideâtrichloromethane.
The majority of the binary systems show linear dependence of <i>E</i><sub>a</sub> and ln <i>A</i> with mole fraction,
either over the entire range of composition or over a wide range of
compositions, typically between 0.2 < <i>x</i><sub>IL</sub> < 1.0. These findings are useful for estimating unknown viscosities
for binary systems involving ILs. As a side-outcome from the Arrhenius
analysis and careful comparisons between datasets, a number of datasets
are identified that are suspect of experimental inaccuracies
Composition Dependent Physicochemical Property Data for the Binary System Water and the Ionic Liquid 1âButyl-3-methylimidazolium Methanesulfonate ([C<sub>4</sub>mim][MeSO<sub>3</sub>])
A number of composition dependent physicochemical properties
were
measured for the waterâ[C<sub>4</sub>mim]Â[MeSO<sub>3</sub>]
binary system at 85 °C. Specifically, we provide data for density,
heat capacity, heats of dissolution, conductivity, viscosity, as well
as the self-diffusion coefficients of the cation, anion, and water.
Ionic liquids based on the MeSO<sub>3</sub> anion constitute a suitable
medium for various chemistries. This study addresses the need to provide
physicochemical data on [C<sub>4</sub>mim]Â[MeSO<sub>3</sub>] and the
waterâ[C<sub>4</sub>mim]Â[MeSO<sub>3</sub>] binary systems that
are currently unavailable. Additional analysis of the combined data
is also presented to provide further insight into the molecular level
behavior of the waterâ[C<sub>4</sub>mim]Â[MeSO<sub>3</sub>]
binary system
Directly vs Indirectly Enhanced <sup>13</sup>C in Dynamic Nuclear Polarization Magic Angle Spinning NMR Experiments of Nonionic Surfactant Systems
A study
of dynamic nuclear polarization (DNP) in polyethylene glycol
and related nonionic surfactants is presented. In these experiments,
we found the surprising result that DNP enhanced <sup>13</sup>C magic
angle spinning (MAS) spectra display two sets of resonances, one with
broad and one with sharp spectral features that are 180° opposite
in phase. These two sets indicate the presence of a direct polarization
transfer channel as expected for <sup>13</sup>C MAS experiments, and
a second unexpected indirect polarization transfer channel. Plots
of DNP enhancements as a function of applied magnetic field for the
two resonances show a superposition of two DNP enhancement profiles
for AMUpol in the nonionic surfactant C<sub>10</sub>E<sub>6</sub>.
The indirect polarization channel can be suppressed by application
of a string of <sup>1</sup>H 180° pulses during <sup>13</sup>C DNP buildup. The presence of direct and indirect polarization channels
is observed in a total of four different nonionic surfactants and
with three different radicals, showing that these concurring polarization
mechanisms are of general nature. Therefore, the presented findings,
including the demonstration of how the indirect polarization channel
can be suppressed, are of high importance for all future applications
of direct <sup>13</sup>C MAS DNP
Influence of APTES-Decorated Mesoporous Silica on the Dynamics of Ethylene Glycol MoleculesInsights from Variable Temperature <sup>2</sup>H Solid-State NMR
The physicochemical effects of decorating pore walls
of high surface
area materials with functional groups are not sufficiently understood,
despite the use of these materials in a multitude of applications
such as catalysis, separations, or drug delivery. In this study, the
influence of 3-amino-propyl triethoxysilane (APTES)-modified SBA-15
on the dynamics of deuterated ethylene glycol (EG-d4) is inspected by comparing three systems: EG-d4 in the bulk phase (sample 1),
EG-d4 confined in SBA-15 (sample 2), and EG-d4 confined in SBA-15
modified with APTES (sample 3). The phase behavior (i.e.,
melting, crystallization, glass formation, etc.) of EG-d4 in these three systems is studied by differential scanning
calorimetry. Through line shape analysis of the 2H solid-state
NMR (2H ssNMR) spectra of the three systems recorded at
different temperatures, two signal patterns, (i) a Lorentzian (liquid-like)
and (ii) a Pake pattern (solid-like), are identified from which the
distribution of activation energies for the dynamic processes is calculated
employing a two-phase model