Local switching of chemical patterns through light-triggered unfolding of creased hydrogel surfaces

Visible light induces switching of surface chemical patterns based on hybrid gels of thermally responsive poly(N-isopropyl acrylamide) copolymer networks containing iron oxide nanoparticles. The swelling of these hybrid gels is reduced upon illumination (see picture), allowing controlled unfolding of creased features formed owing to an elastic surface instability.     

The conformations of 1,2-acenaphthene derivatives and steric interaction of contiguous nitroxy groups

Inter-oxygen distances and conformational flexibility were estimated for cis- and trans-1,2-acenaphthenediol from X-ray data, intramolecular hydrogen bonding, the kinetics of glycol cleavage, and cyclization experiments. The optical and NMR spectra of the isomeric dinitrate esters and related compounds in solution showed significant differences. The symmetric and anti-symmetric stretching bands of the nitroxy group occurred at 1276 ± 2 cm⁻¹ and 1639 ± 7 cm⁻¹ respectively in the trans-dinitrate and in ethyl and benzyl nitrates and were shifted to higher frequencies by 9 cm⁻¹ and 16 cm⁻¹ respectively in the cis-dinitrate. The analogy to similar effects observed in cyclic 1,2-diketones, -haloketones, and o-halonitrobenzenes suggested intramolecular interaction of the contiguous nitroxy groups.

The reaction of the dinitrates with pyridine at 25° was pseudo first-order and the ratio k_trans/k_cis of 6·5 was consistent with an E_CO mechanism involving nitroxy group interaction in the cis isomer.     

Bridging photochemistry and photomechanics with NMR crystallography: the molecular basis for the macroscopic expansion of an anthracene ester nanorod

Crystals composed of photoreactive molecules represent a new class of photomechanical materials with the potential to generate large forces on fast timescales. An example is the photodimerization of 9-tert-butyl-anthracene ester (9TBAE) in molecular crystal nanorods that leads to an average elongation of 8%. Previous work showed that this expansion results from the formation of a metastable crystalline product. In this article, it is shown how a novel combination of ensemble oriented-crystal solid-state NMR, X-ray diffraction, and first principles computational modeling can be used to establish the absolute unit cell orientations relative to the shape change, revealing the atomic-resolution mechanism for the photomechanical response and enabling the construction of a model that predicts an elongation of 7.4%, in good agreement with the experimental value. According to this model, the nanorod expansion does not result from an overall change in the volume of the unit cell, but rather from an anisotropic rearrangement of the molecular contents. The ability to understand quantitatively how molecular-level photochemistry generates mechanical displacements allows us to predict that the expansion could be tuned from +9% to −9.5% by controlling the initial orientation of the unit cell with respect to the nanorod axis. This application of NMR-assisted crystallography provides a new tool capable of tying the atomic-level structural rearrangement of the reacting molecular species to the mechanical response of a nanostructured sample.

NMR crystallography establishes absolute unit-cell orientations relative to the shape change, revealing the atomic-resolution mechanism for the nanorod''s photomechanical response.     

Carbon response characteristics of a micro-flame ionization detector

The carbon response characteristics of a recently noted micro-flame ionization detector (μFID) mode are examined in detail. The μFID supports an extremely small (30 nL) “upside-down” flame that is generated from a low counter-current flow of oxygen immersed in hydrogen. Ionization measurements made in the μFID are directly compared to those obtained from a conventional FID. In terms of reproducibility of response and relative sensitivity towards different types of hydrocarbons, the μFID and a conventional FID produce no major differences with respect to either of these characteristics for a variety of compounds examined. Of note, for replicate measurements made in each detector, the average %R.S.D. of response typically differs by less than 2% between the two devices, while the average normalized sensitivity differs by less than 4%. In contrast to this, regarding absolute sensitivity, the analyte signal from the conventional air-rich FID is found to be three times larger than that of the hydrogen-rich μFID mode explored here. This discrepancy is ascribed directly to the difference in flame stoichiometry between the two detectors.     

Random photografting of polymers to nanoparticles for well-dispersed nanocomposites

A simple method to achieve dispersion of nanoparticles (NPs) within polymer matrices by solution-state photografting of benzophenone (BP)-containing random copolymers is presented. A benzyl ether ligand that stabilizes NPs in solution while possessing selectivity toward hydrogen abstraction and subsequent coupling with BP was designed. This method for introducing grafts by ultraviolet (UV) light exposure affords control over the dispersion state in the resulting polymer films, as revealed by transmission electron microscopy and UV–visible spectroscopy. The evolution of the hydrodynamic sizes of particles as a function of UV dose suggests that the polymers “wrap” particles by forming multiple attachment points per chain because of the relatively rapid kinetics for the formation of subsequent attachments following the first grafting event for a given chain. In addition, the presence of unreacted BP groups allows for photolithographic patterning of well-dispersed nanocomposite films. © 2015 Wiley Periodicals, Inc. J. Polym. Sci., Part B: Polym. Phys. 2016, 54, 152–158