Two isomeric butadiene–N‐(acetoxy­phenyl)maleimide Diels–Alder adducts: supramolecular structure directed by C—H⋯X (X = O and π) hydrogen bonds and perpendicular dipole carbonyl–carbonyl inter­actions

The mol­ecular and supramolecular structures of 2‐(1,3‐dioxo‐2,3,3a,4,7,7a‐hexa­hydro‐1H‐isoindol‐2‐yl)phenyl acetate, C₁₆‐H₁₅NO₄, (I), and its para isomer, 4‐(1,3‐dioxo‐2,3,3a,4,7,7a‐hexa­hydro‐1H‐isoindol‐2‐yl)phenyl acetate, (II), are reported. The torsion angle between the succinimide and benzene rings depends on the position of the acet­oxy substitution [89.7 (1) and 61.9 (1)° for (I) and (II), respectively]. The twist of the acet­oxy group relative to the mean plane of the benzene ring is almost independent of the acet­oxy position [66.0 (1) and 70.0 (1)°]. Packing inter­actions for both compounds include soft C—H⋯X (X = O and Ph) inter­actions, forming chains of centrosymmetric dimers and inter­linked chains for (I) and (II), respectively. In addition, three perpendicular dipole C=O⋯C=O inter­actions contribute to the supramolecular structure of (II).     

Heterometallic hexanuclear isobutyrate clusters based on di- and tripodal alcohols

Four hexanuclear coordination clusters containing $\{{\mathrm{M}}_4^{\mathrm{II}}{\mathrm{M}}_2^{\mathrm{III}}\}$ cores of edge-sharing coordination octahedra exemplify how mixed-spin derivatives of a homonuclear parent structure, [${\mathrm{Mn}}_4^{\mathrm{II}}{\mathrm{Mn}}_2^{\mathrm{III}}{\mathrm{L}}_8$(N–O)₄], can be realized by a ligand ‘shrink-wrapping’ approach, resulting in [${\mathrm{Mn}}_2^{\mathrm{II}}{\mathrm{Co}}_2^{\mathrm{II}}{\mathrm{Mn}}_2^{\mathrm{III}}{\mathrm{L}}_8$(N–O)₄]- and [${\mathrm{Co}}_4^{\mathrm{II}}{\mathrm{Fe}}_2^{\mathrm{III}}{\mathrm{L}}_8$(N-O)₄]-type clusters (L = isobutyrate, N–O = methyldiethanolamine, n-butyldiethanolamine, or triethanolamine). The resulting core structures are either virtually isostructural to the parent structure or differ in the placement of the peripheral metal ions, depending on the mix of structure-directing carboxylate and alkoxyamine ligands with large, flexible alkyl chains. Whereas the $\{{\mathrm{Mn}}_4^{\mathrm{II}}{\mathrm{Mn}}_2^{\mathrm{III}}\}$ and {${\mathrm{Co}}_4^{\mathrm{II}}{\mathrm{Fe}}_2^{\mathrm{III}}$} complexes show dominant antiferromagnetic exchange, ferrimagnetic coupling features are exhibited by two {${\mathrm{Mn}}_2^{\mathrm{II}}{\mathrm{Co}}_2^{\mathrm{II}}{\mathrm{Mn}}_2^{\mathrm{III}}$} clusters.     

Photoconductive semiconductor switches

Optically activated GaAs switches operated in their high-gain mode are being used or tested for pulsed power applications as diverse as low-impedance, high-current firing sets in munitions; high impedance, low-current Pockels cell or Q-switch drivers for lasers; high-voltage drivers for laser diode arrays; high-voltage, high-current, compact accelerators; and pulsers for ground penetrating radar. This paper will describe the properties of high-gain photoconductive semiconductor switches (PCSS), and how they are used in a variety of pulsed power applications. For firing sets, we have switched up to 7 kA in a very compact package. For driving Q switches, the load is the small (30 pF) capacitance of the Q switch which is charged to 6 kV. We have demonstrated that we can modulate a laser beam with a subnanosecond rise time. Using PCSS, we have demonstrated gain switching a series-connected laser diode array, obtaining an optical output with a peak power of 50 kW and a pulse duration of 100 ps. For accelerators, we are using PCSS to switch a 260 kV, 60 kA Blumlein. A pulser suitable for use in ground-penetrating radar has been demonstrated at 100 kV, 1.3 kA. This paper will describe the specific project requirements and switch parameters in all of these applications, and emphasize the switch research and development that is being pursued to address the important issues     

Determining membrane capacitance by dynamic control of droplet interface bilayer area

By making dynamic changes to the area of a droplet interface bilayer (DIB), we are able to measure the specific capacitance of lipid bilayers with improved accuracy and precision over existing methods. The dependence of membrane specific capacitance on the chain-length of the alkane oil present in the bilayer is similar to that observed in black lipid membranes. In contrast to conventional artificial bilayers, DIBs are not confined by an aperture, which enables us to determine that the dependence of whole bilayer capacitance on applied potential is predominantly a result of a spontaneous increase in bilayer area. This area change arises from the creation of new bilayer at the three phase interface and is driven by changes in surface tension with applied potential that can be described by the Young-Lippmann equation. By accounting for this area change, we are able to determine the proportion of the capacitance dependence that arises from a change in specific capacitance with applied potential. This method provides a new tool with which to investigate the vertical compression of the bilayer and understand the changes in bilayer thickness with applied potential. We find that, for 1,2-diphytanoyl-sn-glycero-3-phosphocholine membranes in hexadecane, specific bilayer capacitance varies by 0.6-1.5% over an applied potential of ±100 mV.     

Increasing the RF energy per pulse of an RKO

The Air Force Research Laboratory RKO source has recently demonstrated the ability to convert electron beam power to RF power until the termination of the electron beam pulse, achieving a power of 1.5 GW at an energy of 170 J. These results represent an increase in power of 25-30% in power and energy extracted from this source. This paper discusses the principal research areas encountered in lengthening the RF pulse (FWHM) from 50 ns to the present 120 ns and the associated increase in the RF energy