Molecular composites in thermosets

The synthesis of molecular composites where rigid polymer molecules are reinforcing elements in a thermoset bisimide matrix has been investigated. The approach has been designed to avoid phase separation by selecting systems where reaction of amine-terminated rigid and semiflexible oligomers with maleimide unsaturation occurs prior to crosslinking of the thermoset. This objective has been met for some compositions. The concentration and molecular weight of the rigid oligomers have been varied. The structure of the reinforcing polymer, the reactivity of the maleimide and the conditions for composite synthesis are variables of critical importance, and further work must determine the promise and limitations of this approach.     

A novel RNA motif based on the structure of unusually stable 2',5'-linked r(UUCG) loops

We have recently shown that hairpins containing 2',5'-linked RNA loops exhibit superior thermodynamic stability compared to native hairpins comprised of 3',5'-RNA loops [Hannoush, R. N.; Damha, M. J. J. Am. Chem. Soc. 2001, 123, 12368-12374]. A remarkable feature of the 2',5'-r(UUCG) tetraloop is that, unlike the corresponding 3',5'-linked tetraloop, its stability is virtually independent of the hairpin stem composition. Here, we determine the solution structure of unusually stable hairpins of the sequence 5'-G(1)G(2)A(3)C(4)-(U(5)U(6)C(7)G(8))-G(9)(U/T(10))C(11)C(12)-3' containing a 2',5'-linked RNA (UUCG) loop and either an RNA or a DNA stem. The 2',5'-linked RNA loop adopts a new fold that is completely different from that previously observed for the native 3',5'-linked RNA loop. The 2',5'-RNA loop is stabilized by (a). U5.G8 wobble base pairing, with both nucleotide residues in the anti-conformation, (b). extensive base stacking, and (c). sugar-base and sugar-sugar contacts, all of which contribute to the extra stability of this hairpin structure. The U5:G8 base pair stacks on top of the C4:G9 loop-closing base pair and thus appears as a continuation of the stem. The loop uracil U6 base stacks above U5 base, while the cytosine C7 base protrudes out into the solvent and does not participate in any of the stabilizing interactions. The different sugar pucker and intrinsic bonding interactions within the 2',5'-linked ribonucleotides help explain the unusual stability and conformational properties displayed by 2',5'-RNA tetraloops. These findings are relevant for the design of more effective RNA-based aptamers, ribozymes, and antisense agents and identify the 2',5'-RNA loop as a novel structural motif.     

Torification and factorization of birational maps

Building on work of the fourth author and Morelli's work, we prove the weak factorization conjecture for birational maps in characteristic zero: a birational map between complete nonsingular varieties over an algebraically closed field of characteristic zero is a composite of blowings up and blowings down with nonsingular centers.

     

Microcomputer interfaced stopped-flow spectrometer with interactive graphics

One problem in the use of stopped-flow rapid-mixing systems is that data can be collected much more rapidly than they can be digitized and analyzed. Microprocessor based systems can overcome this problem, but until now they have been expensive and have required experts to assemble the appropriate components.     

Total syntheses of (±)‐cis‐ and trans‐11‐methoxydeethyleburnamonine

The total syntheses of 11‐methoxydeethyleburnamonines ( 4 ) and ( 13 ) were carried out with use of 6‐methoxytryptophyl bromide ( 5 ) as starting material. Compound 5 was converted in three steps to trans‐ester 8 . Acid‐catalysed epimerization of 8 , lithium aluminum hydride reduction of the ester group, tosylation and substitution with cyanide gave the cis‐nitrile 12 . Acid‐induced cyclization of 12 yielded mainly (±)‐trans‐11‐methoxydeethyleburnamonine ( 13 ), whereas base‐induced cyclization gave (±)‐cis‐11‐methoxydeethyleburnamonine ( 4 ).     

Monte Carlo technique for very large ising models

Rebbi's multispin coding technique is improved and applied to the kinetic Ising model with size 600*600*600. We give the central part of our computer program (for a CDC Cyber 76), which will be helpful also in a simulation of smaller systems, and describe the other tricks necessary to go to large lattices. The magnetizationM atT=1.4*T _c is found to decay asymptotically as exp(-t/2.90) ift is measured in Monte Carlo steps per spin, and M(t = 0) = 1 initially.