Effect of misalignment of air-coupled probes on Ao Lamb mode propagating in a metal plate

Proper alignment of air-coupled ultrasonic transducers for generation and reception of Lamb waves is vital in order to acquire a high amplitude wave group. Any misalignment with either the transmitter or the receiver or both adversely influences the amplitude of a Lamb mode. This paper reports a systematic attempt to quantify the reduction in the amplitude of the fundamental anti-symmetric Lamb mode (A_o) in a metal plate caused by misalignments in air-coupled probes. Three different types of misalignments – linear, orientation and synchronised orientation were deliberately introduced in the transducers, and experiments were performed on a 6 mm thick aluminium plate. Amplitudes of A_o mode measured at various configurations were normalised with that of A_o mode, captured in a reference configuration. Suitable curves fitted over the experimental data points revealed that Gaussian curves represent appropriately the variations in normalised amplitudes of A_o mode. Moreover, analytical expressions were derived to predict the difference in arrival times of Lamb mode(s) due to orientation and synchronised orientation misalignments.     

Annoyance and noise from road traffic

The cause of insufficient privacy in open plan offices is identified as the reduction of background noise level resulting from the installation of highly absorbent ceilings intended to enhance the performance of portable acoustic screens. The V-form ceiling is suggested as a ceiling design which may increase both screen performance and background level. The extent to which these variables are affected by the use of such a design is investigated by using an acoustic scale model technique. The experimental approach used enables the measurement of attenuation curves for different ceiling configurations and allows the full appraisal of screen performance. It is concluded from the investigation that a V-form ceiling can contribute only marginally to increased privacy in open plan offices by decreasing the Articulation Index for speaker/listener situations by about 0·1.     

Properties of a soft-sphere liquid from non-Newtonian molecular dynamics

A soft-sphere, inverse-12 liquid is simulated in both the isokinetic-isochoric and the isokinetic-isobaric ensemble using nonequilibrium molecular dynamics. The simulation for the isobaric ensemble is discussed in detail. The non-Newtonian characteristics of the liquid are clearly demonstrated; namely, the shear-rate-dependent pressure and density (shear dilatancy), the shear-rate-dependent shear viscosity (shear thinning), and evidence of normal pressure differences. For the first time, it is clearly shown that a significant component of isobaric shear thinning is due to shear dilatancy. The isochoric and isobaric results are checked for consistency. Simple empirical relations for the equation of state and transport properties of the fluid are presented.This is a publication in part of the National Institute of Standards and Technology (formerly NBS) and is not subject to copyright.     

Electrochemically programmed, spatially selective biofunctionalization of silicon wires

A method for the spatially selective biofunctionalization of silicon micro- and nanostructures is reported, and results are presented for both single-crystal silicon (111) or (100) surfaces. An electroactive monolayer of hydroquinone was formed on the surface of H-terminated silicon working electrodes via an olefin reaction with UV-generated surface radicals. Molecules presenting either cyclopentadiene or a thiol group can be immobilized onto the regions where the hydroquinone has been oxidized. Molecular size and crystal orientation are evaluated as important factors that dictate the electrode stability in aqueous solution under anodic potentials. Monolayers composed of smaller molecules on (111) surfaces exhibit the highest packing density and are more effective in preventing anodic oxidation of the underlying substrate. Voltammetry, X-ray photoelectron spectroscopy, and atomic force and fluorescence microscopy are utilized to interrogate the kinetic rates of biofunctionalization, the extent of surface coverage, monolayer quality, and the spatial selectivity of the process.     

The prediction of noise levels L10 due to road traffic

The authors have developed an improved procedure for predicting noise levels L₁₀ from road traffic. The new method has been adopted for use within England and Wales in connection with the Noise Insulation Regulations 1975 and for other aspects of planning. The formulation of the new procedure is discussed, and its overall performance assessed by reference to a comprehensive data bank specifically assembled for that purpose.     

Correction: Crystal structure and metallization mechanism of the π-radical metal TED

Radical electrons tend to localize on individual molecules, resulting in an insulating (Mott–Hubbard) bandgap in the solid state. Herein, we report the crystal structure and intrinsic electronic properties of the first single crystal of a π-radical metal, tetrathiafulvalene-extended dicarboxylate (TED). The electrical conductivity is up to 30 000 S cm⁻¹ at 2 K and 2300 S cm⁻¹ at room temperature. Temperature dependence of resistivity obeys a T³ power-law above T > 100 K, indicating a new type of metal. X-ray crystallographic analysis clarifies the planar TED molecule, with a symmetric intramolecular hydrogen bond, is stacked along longitudinal (the a-axis) and transverse (the b-axis) directions. The π-orbitals are distributed to avoid strong local interactions. First-principles electronic calculations reveal the origin of the metallization giving rise to a wide bandwidth exceeding 1 eV near the Fermi level. TED demonstrates the effect of two-dimensional stacking of π-orbitals on electron delocalization, where a high carrier mobility of 31.6 cm² V⁻¹ s⁻¹ (113 K) is achieved.

The molecular arrangement that enables metallic conduction in a single-component pure organic crystal is revealed by single-crystal X-ray diffraction.

Organic molecular solids are typically insulating due to their paired electrons in spatially localized s- and p-orbitals. The concept of charge-transfer (CT) between donor and acceptor¹ enabled the development of conducting molecular complexes (salts) including semiconducting perylene-bromine,² metallic tetrathiafulvalene (TTF)-tetracyano-p-quinodimethane (TCNQ),³ and polyacethylene doped with halogen molecules.⁴ A different strategy was proposed in the 1970s based on organic radicals with an open-shell electronic structure.⁵ π-Radicals such as neutral-,⁶ fully-conjugated⁷ and zwitterionic (betainic)⁸ molecules, with an unpaired electron in their singly occupied molecular orbital (SOMO), offered potential candidates. However, all these π-radicals were insulators or semiconductors with a finite bandgap, which is due to the SOMO being localized on an individual molecule. In the Mott–Hubbard model,⁹ the case of the π-radical solids can be described by the on-site Coulomb repulsion U being larger than the electronic bandwidth W (U/W > 1), in contrast to U/W < 1 in molecular metals like CT metal systems (Fig. 1a).Open in a separate windowFig. 1(a) Schematic representation of the electronic band structure of Mott–Hubbard insulators (left) and possible molecular metals (right), respectively. Solids formed from typical π-radicals possess large on-site Coulomb repulsion U compared with the electronic bandwidth W, resulting a finite bandgap (left). This requires a new mechanism to expand W and overcome U to achieve a metallic state at ambient pressure in π-radical crystals. (b) Molecular structure of the zwitterionic radical, tetrathiafulvalene-extended dicarboxylate (TED) with a symmetric intramolecular hydrogen bond.A straightforward approach to realize high conductivity in π-radical systems is to enhance the intermolecular interaction by applying high pressure.¹⁰ Bisdithiazolyl radical crystal achieved W ∼ 1 eV near the Fermi level and the room temperature conductivity σ_RT = 2 S cm⁻¹ under 11 GPa pressure.^10c An alternative route is to decrease the interatomic spacing by incorporating a metal ion. Introduction of a semimetal Se and intermolecular hydrogen bonding in a donor-type radical succeeded to improve a conductivity to σ_RT = 19 S cm⁻¹ but still required high pressure over 1 GPa for breaking its insulating character.^10d An organometallic compound with a transition metal, [Ni(tmdt)₂], by contrast, is known to form a three-dimensional (3D) Fermi surface with W = 0.48 eV and metallic conduction with σ_RT = 400 S cm⁻¹ at ambient pressure.¹¹ A breakthrough concept for expanding W at ambient pressure is desired for achieving metallization in pure organic π-radicals.Tetrathiafulvalene-extended dicarboxylate (TED) is an organic air-stable zwitterionic radical (Fig. 1b),¹² which was designed based on carrier generation induced by a stably-introduced protonic defect (–H⁺) in hydrogen-bonding molecules without adopting CT between multiple molecules.¹³ A polycrystalline film of TED exhibited metallic conduction at ambient pressure, but the mechanism has not been clarified yet due to lack of single crystal information.¹² Herein, we report the first crystal structure and intrinsic electronic properties of the recently grown single crystal TED. Structural analysis and quantum chemical simulations based on the single crystal reveal the origin of its metallic behavior.     

Effect of electric field switching on the electrophoretic mobility of single-stranded DNA molecules in polyacrylamide gels

We have examined the effects of pulsed electric fields on the separation of single-stranded DNA molecules in polyacrylamide sequencing gels. Using different electric field pulsing regimens, the mobilities of single-stranded DNA molecules can be retarded or increased as compared to conventional electrophoresis. These results indicated that pulsed field techniques can be applied to gel electrophoresis of small single-stranded DNA molecules.     

The crystal engineering of radiation-sensitive diacetylene cocrystals and salts

In this work we develop photoreactive cocrystals/salts of a commercially-important diacetylene, 10,12-pentacosadiynoic acid (PCDA, 1) and report the first X-ray crystal structures of PCDA based systems. The topochemical reactivity of the system is modified depending on the coformer used and correlates with the structural parameters. Crystallisation of 1 with 4,4′-azopyridine (2), 4,4′-bipyridyl (3), and trans-1,2-bis(4-pyridyl)ethylene (4) results in unreactive 2 : 1 cocrystals or a salt in the case of 4,4′-bipiperidine (5). However, salt formation with morpholine (6), diethylamine (7), and n-butylamine (8), results in highly photoreactive salts 12·7 and 1·8 whose reactivity can be explained using topochemical criteria. The salt 1·6 is also highly photoreactive and is compared to a model morpholinium butanoate salt. Resonance Raman spectroscopy reveals structural details of the photopolymer including its conformational disorder in comparison to less photoactive alkali metal salts and the extent of solid state conversion can be monitored by CP-MAS NMR spectroscopy. We also report an unusual catalysis in which amine evaporation from photopolymerised PCDA ammonium salts effectively acts as a catalyst for polymerisation of PCDA itself. The new photoreactive salts exhibit more reactivity but decreased conjugation compared to the commercial lithium salt and are of considerable practical potential in terms of tunable colours and greater range in UV, X-ray, and γ-ray dosimetry applications.

In this work we develop photoreactive cocrystals/salts of a commercially-important diacetylene, 10,12-pentacosadiynoic acid (PCDA, 1) and report the first X-ray crystal structures of PCDA based systems.     

A positron annihilation study of recovery of alpha-Zr from electron irradiation damage

Electron irradiation damage and its thermally-activated recovery has been studied in α-Zr by positron annihilation spectroscopy. The samples were irradiated with 1.5 MeV electrons at a nominal temperature of 295 K. The Doppler broadening technique was used and the results are reported in terms of peak (S) and wing (W) lineshape parameters. Recovery processes are evident over the range 300–670 K for S and from 300 to 600 K for W.