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Accurate interpolation of the dependency of modal properties on the rotation speed for the transient response analysis of bladed disks
During fast gas-turbine engine acceleration and deceleration the transient vibration effects in bladed disk vibration become significant and the transient response has to be calculated. In this paper an effective method is developed for efficient calculations of the transient vibration response for mistuned bladed disks under varying rotation speeds. The method uses the large-scale finite element modelling of the bladed disks allowing the accurate description of the dynamic properties of the mistuned bladed disks. The effects of the varying rotation speed on the natural frequencies and mode shapes of a mistuned bladed disk and its effects on the amplitude and the spectral composition of the loading are considered. The dependency of the modal characteristics on the rotation speed are based on the evaluation of these characteristics at reference points followed by the interpolation to obtain values at any rotation speed from the operating range. A new method has been developed for the interpolation of mode shapes while preserving the orthogonality and mass-normalization of the mode shapes. The method of mode shape interpolation is elaborated for tuned and mistuned bladed disks. The accuracy and efficiency of the method is demonstrated on test examples and on analysis of transient forced response of realistic bladed discs
Densities and Viscosities of Aqueous Amino Acid Ionic Liquids [C<sub><i>n</i></sub>mim][Ala](<i>n</i> = 3, 4, 5)
Amino
acid ionic liquids [C<sub><i>n</i></sub>mim]Â[Ala]
(<i>n</i> = 3, 4, 5) (1-alkyl-3-methylimidazolium alanine
salt) were prepared by the neutralization method. The density and
viscosity for aqueous solutions of the ionic liquids (ILs) with various
molalities were measured at <i>T</i> = (288.15 to 328.15)
K with an interval of 5 K. In terms of the Jones–Dole equation,
the viscosity <i>B</i>-coefficients with large positive
values and d<i>B</i>/d<i>T</i> < 0 were obtained,
and these facts implied that the ionic liquids are water-structure-making.
According to Feakins, the contribution of the solute per mole to the
free energy of activation for viscous flow of the solution, Δμ<sub>2</sub><sup>⧧0</sup>, or called as the standard molar activation
free energy, was obtained at different temperatures. Under the constant
molality of solution, Δ<i>H</i><sub>2</sub><sup>⧧0</sup> (the activation enthalpy of the activation for viscous flow of aqueous
[C<sub><i>n</i></sub>mim]Â[Ala] (<i>n</i> = 3,
4, 5)) is a temperature-independent constant. This implies that the
activation process of the solute for viscous flow of aqueous [C<sub><i>n</i></sub>mim]Â[Ala] (<i>n</i> = 3, 4, 5)
is an isoCoulombic reaction. A semiempirical method to estimate the
viscosity of aqueous [C<sub><i>n</i></sub>mim]Â[Ala] (<i>n</i> = 3, 4, 5) was put forward based on Eyring’s theory,
and the estimated viscosity values of the aqueous ILs are in good
agreement with the corresponding experimental ones
Theoretical Study on Polynuclear Superalkali Cations with Various Functional Groups as the Central Core
A new series of polynuclear superalkali cations YLi<sub>3</sub><sup>+</sup> (Y = CO<sub>3</sub>, SO<sub>3</sub>, SO<sub>4</sub>,
O<sub>4</sub>, and O<sub>5</sub>) has been created when the central
group is surrounded by alkali atoms. The structural characteristics
and stabilities of these systems are provided on the basis of ab initio
methods. In the lowest-energy structure of the CO<sub>3</sub>Li<sub>3</sub><sup>+</sup>, SO<sub>3</sub>Li<sub>3</sub><sup>+</sup>, and
SO<sub>4</sub>Li<sub>3</sub><sup>+</sup> cations, the central Y (Y
= CO<sub>3</sub>, SO<sub>3</sub>, and SO<sub>4</sub>) group features
a slight distortion. The global minima of O<sub>4</sub>Li<sub>3</sub><sup>+</sup> and O<sub>5</sub>Li<sub>3</sub><sup>+</sup> are of the
forms O<sub>2</sub><sup>–</sup>(Li<sup>+</sup>)<sub>3</sub>O<sub>2</sub><sup>–</sup> and O<sub>2</sub><sup>–</sup>(Li<sup>+</sup>)<sub>3</sub>O<sub>3</sub><sup>–</sup>, respectively,
both of which contain two monovalent ion units. The structural integrity
of the central Y group and the arrangement of the lithium ligands
are two influencing factors on the vertical electron affinities (EA<sub>vert</sub>) for the YLi<sub>3</sub><sup>+</sup> species. The YLi<sub>3</sub><sup>+</sup> cation, with its lithium ligands being distributed
evenly or far from each other, tends to exhibit a low EA<sub>vert</sub> value, whereas a greater extent of cleavage of the central Y group
leads to a higher EA<sub>vert</sub> value and even makes some species
lose their superalkali nature
Efficient Flexible Counter Electrode Based on Modified Graphite Paper and in Situ Grown Copper Sulfide for Quantum Dot Sensitized Solar Cells
Flexible counter
electrode (CE) plays an important role in portable quantum dot sensitized
solar cells (QDSCs). However, the present power conversion efficiency
(PCE) of bendable QDSC is rather limited partly due to the unsatisfactory
conductivity, flexibility, catalytic activity, and fabrication technique
of CE. In this work, flexible CEs composed of Cu<sub><i>x</i></sub>S and graphite paper (GP) are built and fabricated through
a facile successive ionic layer adsorption reaction (SILAR) method.
Through designing and optimizing of the surface property of GP, coverage,
and thickness of catalyst, excellently performed CEs are achieved
with the maximal PCE of 8.70% under one full sun illumination for
Zn–Cu–In–Se QDSCs. Further, fully flexible QDSCs
assembled with the as-prepared CEs and plastic photoanodes show a
high PCE of 2.45% under the same illumination
Surface Properties of Aqueous Solutions of Amino Acid Ionic Liquids: [C<sub>3</sub>mim][Gly] and [C<sub>4</sub>mim][Gly]
Glycine ionic liquids [C<sub>3</sub>mim]Â[Gly] (1-propyl-3-methylimidazolium
glycine) and [C<sub>4</sub>mim]Â[Gly] (1-butyl-3-methylimidazolium
glycine) have been prepared by the neutralization method and characterized
by <sup>1</sup>H NMR spectroscopy and DSC trace. The values of density
and surface tension of aqueous [C<sub>3</sub>mim]Â[Gly] and [C<sub>4</sub>mim]Â[Gly] with various molality were determined in the temperature
range of (288.15 to 328.15 ± 0.05) K, and the experimental values
of parachor for these solutions were calculated. Using the empirical
equation of parachor, the surface tension of these aqueous solutions
was estimated, and the estimated values are in good agreement with
experimental values within error
Table 1
<p>(*: KANR was used as a positive control spike).</p><p>doi:10.1371/journal.pone.0082030.t001</p><p>Human Reference Plex Gene Information.</p
Physico-chemical Properties of 1‑Alkyl-3-methylimidazolium Propionate Ionic Liquids {[C<sub><i>n</i></sub>mim][Pro](<i>n</i> = 3, 4, 5, 6)} from 288.15 K to 328.15 K
Four propionic acid ionic liquids
(PrAILs) [C<sub><i>n</i></sub>mim]Â[Pro] (<i>n</i> = 3, 4, 5, 6) (1-alkyl-3-methylimidazolium
propionate) were prepared by the neutralization method and characterized
by <sup>1</sup>H NMR spectroscopy and differential scanning calorimetry.
The values of their density, surface tension, and refractive index
were measured in the temperature range of 288.15–328.15 K.
Since the PrAILs can strongly form hydrogen bonds with water, the
small amount of water is difficult to remove from the PrAILs by conventional
methods. To eliminate the effect of the water impurity, the standard
addition method (SAM) was applied to these measurements. The dependence
of volumetric properties, surface properties, and molar refraction
on temperature were discussed. In terms of Kabo’s method the
molar enthalpies of vaporization, Δ<i>H</i><sup>V</sup>, for the PrAILs were estimated. As a new idea, it was put forward
that Δ<i>H</i><sup>V</sup> can be assumed to consist
of two parts: one is the contribution from induced dipole, Δ<i>H</i><sup>V</sup><sub><i>n</i></sub>, and the other
is the contribution from the permanent dipole of ion pair in ILs,
Δ<i>H</i><sup>V</sup><sub>μ</sub>. The values
of Δ<i>H</i><sup>V</sup><sub><i>n</i></sub> can be estimated in terms of refractive index data so that the values
of Δ<i>H</i><sup>V</sup><sub>μ</sub> can be
obtained and Δ<i>H</i><sup>V</sup><sub>μ</sub> may be seen as the measure of polarity for ILs
Determination of the Enthalpy of Vaporization and Prediction of Surface Tension for Ionic Liquid 1‑Alkyl-3-methylimidazolium Propionate [C<sub><i>n</i></sub>mim][Pro](<i>n</i> = 4, 5, 6)
With
the use of isothermogravimetrical analysis, the enthalpies
of vaporization, Δ<sup>g</sup><sub>l</sub><i>H</i><sup>o</sup><sub>m</sub>(<i>T</i><sub>av</sub>), at the
average temperature, <i>T</i><sub>av</sub> = 445.65 K, for
the ionic liquids (ILs) 1-alkyl-3-methylimidazolium propionate [C<sub><i>n</i></sub>mim]Â[Pro]Â(<i>n</i> = 4, 5, 6) were
determined. Using Verevkin’s method, the difference of heat
capacities between the vapor phase and the liquid phase, Δ<sup>g</sup><sub>l</sub><i>C</i><sub>p</sub><sup>o</sup><sub>m</sub>, for [C<sub><i>n</i></sub>mim]Â[Pro]Â(<i>n</i> = 2, 3, 4, 5, 6), were calculated based on the statistical thermodynamics.
Therefore, with the use of Δ<sup>g</sup><sub>l</sub><i>C</i><sub>p</sub><sup>o</sup><sub>m</sub>, the values of Δ<sup>g</sup><sub>l</sub><i>H</i><sup>o</sup><sub>m</sub>(<i>T</i><sub>av</sub>) were transformed into Δ<sup>g</sup><sub>l</sub><i>H</i><sup>o</sup><sub>m</sub>(298), 126.8,
130.3, and 136.5 for [C<sub><i>n</i></sub>mim]Â[Pro]Â(<i>n</i> = 4, 5, 6), respectively. In terms of the new scale of
polarity for ILs, the order of the polarity of [C<sub><i>n</i></sub>mim]Â[Pro]Â(<i>n</i> = 2, 3, 4, 5, 6) was predicted,
that is, the polarity decreases with increasing methylene. A new model
of the relationship between the surface tension and the enthalpy of
vaporization for aprotic ILs was put forward and used to predict the
surface tension for [C<sub><i>n</i></sub>mim]Â[Pro]Â(<i>n</i> = 2, 3, 4, 5, 6) and others. The predicted surface tension
for the ILs is in good agreement with the experimental one
Superficial Chiral Etching on Achiral Metal–Organic Framework for Enantioselective Sorption
Chiral
recognition and separation is of general research interests
in natural product separation and the pharmacy industry. In this work,
we develop a novel strategy to modify achiral porous metal–organic
framework (MOF) surfaces via a <i>superficial chiral etching
process</i> (SCEP), in which reacting a presynthesized achiral
MOF with a chiral ligand produces an achiral@chiral MOF core–shell
hybrid composition. SCEP creates chiral species on an achiral porous
MOF surface but does not change the porosity and pore structure, enabling
core–shell composition enantioselective sorption. Reacting
(+)-camphoric acid, (+)-Cam, and 1,4-diazabicyclo[2.2.2]Âoctane (Dabco)
with [Cu<sub>3</sub>(Btc)<sub>2</sub>] microcrystals leads to a chiral
MOF of [Cu<sub>2</sub>((+)-Cam)<sub>2</sub>Dabco] crystallites attached
on the surface of [Cu<sub>3</sub>(Btc)<sub>2</sub>] (Btc = 1,3,5-benzenetricarboxylate).
The resulting [Cu<sub>3</sub>(Btc)<sub>2</sub>]@[Cu<sub>2</sub>((+)-Cam)<sub>2</sub>Dabco] core–shell composition displays preferred sorption
kinetics toward (<i>S</i>)-limonene against (<i>R</i>)-limonene, with a similar discrimination effect with pure chiral
[Cu<sub>2</sub>((+)-Cam)<sub>2</sub>Dabco]. Superficial chiral etching
of the porous achiral MOF represents an economic and efficient strategy
for enantioselective separation
Additional file 1 of Relationship between quantitative epicardial adipose tissue based on coronary computed tomography angiography and coronary slow flow
Supplementary Material