Surface tension of an ideal solid: What does it mean?

The surface tension (ST) of an ideal (rigid, smooth, and inert) solid surface is usually calculated from a set of two equations: the Young equation and an additional equation that expresses the correlation between the individual STs of two phases and their interfacial tension. The present discussion suggests that this calculated ST may not be an appropriate characteristic of wettability of a solid surface. The reasons include the nonmeasurability of this ST and theoretical aspects related to the rigidity and inertness of an ideal solid. Instead, it is suggested to measure the contact angles of a set of a few standard liquids, from which a ‘wettability index’ can be calculated by properly averaging the wettability indices calculated for each of standard liquid. The optimal identity of these liquids and the optimal weights of the averages should be found by experimentation.     

Weighted least-squares in calibration: what difference does it make?

In univariate calibration, an unknown concentration or amount x(0) is estimated from its measured response y(0) by comparison with a calibration data set obtained in the same way for known x values. The calibration function y = f(x) contains parameters obtained from a least-squares (LS) fit of the calibration data. Since minimum-variance estimation requires that the data be weighted inversely as their true variances, any other weighting leads to predictable losses of precision in the calibration parameters and in the estimation of x(0). Incorrect weighting also invalidates the apparent standard errors returned by the LS calibration fit. Both effects are studied using Monte Carlo calculations. For the strongest commonly encountered heteroscedasticity, proportional error (sigma(i) proportional, varianty(i)), neglect of weights yields as much as an order of magnitude precision loss for x(0) in the small x region, but only nominal loss in the calibration mid-range. Use of replicates gives great improvement at small x but can underperform unweighted regression in the mid-to-large x region. Variance function estimation approximates minimum-variance, even though the true variance functions are not well reproduced. A relative error test applied to the calibration data themselves is predisposed to favor 1/y(2) (or 1/x(2)) weighting, even if the data are homoscedastic. This predisposition weakens when replicate measurements are taken and disappears when the test is applied to an independent set of data. The distinction between a priori and a posteriori parameter standard errors is emphasized. Where feasible, the a priori approach permits reliable assignment of weights, application of a chi(2) test, and use of the normal distribution for confidence limits.     

What does polycondensation mean?

This contribution has the function of an introduction to the entire volume. It deals with several fundamental definitions and classifications related to the chemistry of polycondensation processes, and it includes modifications of the classical theory of step-growth polymerizations.     

Thermochemical kinetics: does it still give insights?

This tutorial review revisits the subject of the seminal book written by Sidney Benson in 1968. A short summary of the nature of the subject is presented, including its place in the wider world of quantitative chemistry. A number of themes are selected to illustrate its previous and continuing usefulness in evaluating numerical values of important quantities, and probing ideas of reaction mechanism. These include strain enthalpies for biradical combination, chain reactions, why some reactions don't occur and the involvement of carbenes in hydrocarbon rearrangements.     

Modification of cellulose fibres with organosilanes: Under what conditions does coupling occur?

Different cellulose substrates and organosolv lignin were treated heterogeneously with organic solutions of trialkoxysilanes bearing variable function on the forth substituent. It was shown unambiguously for the first time that Si-OR does not react with the hydroxy groups of cellulose even at high temperature, whereas it condenses with the phenolic OH of lignin. The addition of moisture to these systems induces the partial hydrolysis of the siloxane moieties and the ensuing silanol groups can then react with the cellulose OH, but only at high temperature. Using the latter systems and a siloxane bearing a polymerizable function, it was possible to attach poly(methylmethacrylate) chains to the surface of cellulose fibres through a two-step procedure.     

H4(+): what do we know about it?

The potential energy surface of H(4)(+) has been analyzed and stationary points and minima of intersections characterized by benchmark multireference configuration interaction calculations with basis sets as large as augmented septuble zeta. No evidence for minima other than those of the well established stable C(2v) configuration has been found. Some of the results obtained previously at a lower level of ab initio theory had to be revised.     

Competition between alkenes in intramolecular ketene-alkene [2 + 2] cycloaddition: what does it take to win?

In the course of developing a new synthetic methodology using ketenes in sequential cycloaddition steps, we were faced with a competition problem with molecules containing a ketene tethered to more than one reacting partner. To pinpoint the electronic and tethering requirements for a chemoselective reaction, we undertook a series of ketene-alkene [2 + 2] cycloaddition competition experiments. Those experiments were conducted on molecules containing either two identical alkenes having different tether lengths or two alkenes having the same tether length but being electronically different. We demonstrated that the reaction is much faster for forming five-membered rings than six-membered rings and calculated the Hammett constant rho for intramolecular ketene-alkene [2 + 2] cycloadditions to be -1.39.     

SCC-DFTB: what is the proper degree of self-consistency?

The approximate SCC-DFTB method (Elstner, M.; Porezag, D.; Jungnickel, G.; Elsner, J.; Haugk, M.; Frauenheim, Th.; Suhai, S.; Seifert, G. Phys. Rev. B 1998, 58, 7260) is derived from DFT by a second-order expansion of the total energy expression. In this article, basic approximations and assumptions underlying the DFTB method are discussed in detail, and further extensions to include third-order terms are proposed. Further, the SCC-DFTB and semiempirical NDDO formalisms are compared to elucidate similarities and differences.     

A combined photoacoustic DSC for simultaneous temperature modulated measurements: does it really work?

Combination of two techniques, photoacoustic (PA) and differential scanning calorimetry (DSC), is a combination of quasi stationary thermodynamic DSC method and nonstationary dynamic PA method. Especially favorable and easy to realize is the combination with power compensated type of DSC. It has several advantages over the use of two techniques separately and allow to perform measurements simultaneously. The most obvious is simultaneous determination of thermodynamic properties such as specific heat, heat of transition and dynamic properties such as effusivity, thermal conductivity at the different phase transitions and complex specific heat at the glass transition. Unlike other temperature modulated techniques PA–DSC is especially suitable for studying polymer materials since their low thermal conductivity is an additional advantage. Conditions for simultaneous measurements are examined. It is proved that the combination of two techniques and necessary changes in construction do not essentially change adequate work of the instrument. A little disbalance of DSC operation due to the construction change can be corrected simply by recalibration. The procedures for testing and calibration for the proper operation of the combined PA–DSC are given together with some details of experimental methodology. Several measurements could serve as examples of widespread applicability of PA–DSC to study different types of phase transitions as well as time dependent processes such as glass transition.     

Elongated dihydrogen complexes: what remains of the H-H bond?

Of the several hundred examples of transition metal dihydrogen complexes that have been reported to date, the vast majority have H-H distances of less than 1.0 Angstrom. A small number of complexes have been reported with distances in the range of 1.1 to 1.5 Angstrom. These complexes have been termed elongated dihydrogen complexes. In this review, experimental methods for structure determination of such complexes are summarized, along with computational approaches which have proven useful in understanding the structures of these molecules.     

CO2 deactivation of supported amines: does the nature of amine matter?

Adsorption of CO(2) was investigated on a series of primary, secondary, and tertiary monoamine-grafted pore-expanded mesoporous MCM-41 silicas, referred to as pMONO, sMONO, and tMONO, respectively. The pMONO adsorbent showed the highest CO(2) adsorption capacity, followed by sMONO, whereas tMONO exhibited hardly any CO(2) uptake. As for the stability in the presence of dry CO(2), we showed in a previous contribution [J. Am. Chem. Soc.2010, 132, 6312-6314] that amine-supported materials deactivate in the presence of dry CO(2) via the formation of urea linkages. Here, we showed that only primary amines suffered extensive loss in CO(2) uptake, whereas secondary and tertiary amines were stable even at temperature as high as 200 °C. The difference in the stability of primary vs secondary and tertiary amines was associated with the occurrence of isocyanate as intermediate species toward the formation of urea groups, since only primary amines can be precursors to isocyanate in the presence of CO(2). However, using a grafted propyldiethylenetriamine containing both primary and secondary amines, we demonstrated that while primary amines gave rise to isocyanate, the latter can react with either primary or secondary amines to generate di- and trisubstituted ureas, leading to deactivation of secondary amines as well.     

Fragmentation of the conjugate base of 2-(1-hydroxybenzyl)thiamin: does benzoylformate decarboxylase prevent orbital overlap to avoid it?

The base-catalyzed addition of thiamin to benzaldehyde produces 2-(1-hydroxybenzyl)thiamin (HBnT), but in neutral solution HBnT undergoes base-catalyzed irreversible fragmentation into pyrimidine and thiazole derivatives. The fragmentation (rather than elimination) occurs in proportion to the extent that N1' is protonated or alkylated. Generating the conjugate base of HBnT by decarboxylation surprisingly leads to fragmentation independent of the state of N1'. Therefore, a cationic state at N1' specifically promotes removal of the C2alpha proton rather than the fragmentation process itself. It is suggested that benzoylformate decarboxylase, which generates a similar intermediate, exerts stereoelectronic control of the conformation of the carbanion, blocking fragmentation and facilitating protonation.     

One- and two-dimensional translational energy distributions in the iodine-loss dissociation of 1,2-C2H4I2+ and 1,3-C3H6I2+: what does this mean?

Threshold photoelectron photoion coincidence (TPEPICO) has been used to study the sequential photodissociation reaction of internal energy selected 1,2-diiodoethane cations: C(2)H(4)I(2)(+) → C(2)H(4)I(+) + I → C(2)H(3)(+) + I + HI. In the first I-loss reaction, the excess energy is partitioned between the internal energy of the fragment ion C(2)H(4)I(+) and the translational energy. The breakdown diagram of C(2)H(4)I(+) to C(2)H(3)(+), i.e., the fractional ion abundances below and above the second dissociation barrier as a function of the photon energy, yields the internal energy distribution of the first daughter, whereas the time-of-flight peak widths yield the released translational energy in the laboratory frame directly. Both methods indicate that the kinetic energy release in the I-loss step is inconsistent with the phase space theory (PST) predicted two translational degrees of freedom, but is well-described assuming only one translational degree of freedom. Reaction path calculations partly confirm this and show that the reaction coordinate changes character in the dissociation, and it is, thus, highly anisotropic. For comparison, data for the dissociative photoionization of 1,3-diiodopropane are also presented and discussed. Here, the reaction coordinate is expected to be more isotropic, and indeed the two degrees of freedom assumption holds. Characterizing kinetic energy release distributions beyond PST is crucial in deriving accurate dissociative photoionization onset energies in sequential reactions. On the basis of both experimental and theoretical grounds, we also suggest a significant revision of the 298 K heat of formation of 1,2-C(2)H(4)I(2)(g) to 64.5 ± 2.5 kJ mol(-1) and that of CH(2)I(2)(g) to 113.5 ± 2 kJ mol(-1) at 298 K.