Transient Uncoupling Induces Synchronization

Finding conditions that support synchronization is a fertile and active area of research with applications across multiple disciplines. Here we present and analyze a scheme for synchronizing chaotic dynamical systems by transiently uncoupling them. Specifically, systems coupled only in a fraction of their state space may synchronize even if fully coupled they do not. Although, for many standard systems, coupling strengths need to be bounded to ensure synchrony, transient uncoupling removes this bound and thus enables synchronization in an infinite range of effective coupling strengths. The presented coupling scheme thus opens up the possibility to induce synchrony in (biological or technical) systems whose parameters are fixed and cannot be modified continuously.Comment: 5 pages, 6 figure

Optimal strain gage location for determination of mode I stress intensity factor for orthotropic laminates using a single strain gage

The present work discusses a robust method developed for determination of mode I stress intensity factor (KI) of orthotropic laminates using a single strain gage and based on a three parameter strain series representation ahead of the crack tip. Appropriate radial location of the strain gage ahead of the crack tip is important in the sense that strain gages placed either very near or very far from the crack tip might lead to inaccuracies in the estimated SIFs due to 3D effects near the crack tip or inaccurate strain field representation at farther distances. The theoretical formulation has been presented for determination of angular location, orientation and the upper bound on the radial location (rmax) for pasting the strain gage which could be subsequently used for accurate determination of KI. Numerical simulations have been presented considering edge cracked [902/0]10S carbon-epoxy orthotropic laminates to illustrate the determination of rmax and KI of such laminates

Synthesis, structure, spectral and electron-transfer properties of octahedral-[Co<SUP>III</SUP>(L)<SUB>2</SUB>]<SUP>+</SUP>/[Zn<SUP>II</SUP>(L)<SUB>2</SUB>] and square planar-[Cu<SUP>II</SUP>(L){OC(=O)CH<SUB>3</SUB>}] complexes incorporating anionic form of tridentate bis(8-quinolinyl)amine [N<SUP>1</SUP>C<SUB>9</SUB>H<SUB>6</SUB>-N<SUP>2</SUP>-C<SUB>9</SUB>H<SUB>6</SUB>N<SUP>3</SUP>, L<SUP>-</SUP>] ligand

The reaction of bis(8-quinolinyl)amine [N1C9H6-N2H-C9H6N3, LH] with CoII(ClO4)2 . 6H2O in methanol under aerobic conditions results in a new class of [CoIIIN6]+ (1+) chromophore incorporating an sp2-amido nitrogen center (N2) in the ligand frame. During the course of the reaction, the cobalt ion has been oxidized from its starting +2 oxidation state to +3 state in 1. The reaction of LH with the Cu-acetate yields monomeric square planar complex, [CuII(L){OC(=O)CH3}] (2). The same copper complex 2 is also obtained from Cu(ClO4) . 6H2O in presence of CH3COONa as base. On the other hand, the reaction of Zn(ClO4) . 6H2O with LH results in octahedral complex ZnII(L)2 (3). The Cu(II) complex 2 displays a four-line EPR spectrum at room temperature. Crystal structure of the free ligand (LH) shows that the amine proton [N(2)H] is hydrogen-bonded with the terminal quinoline nitrogen centers [N(1) and N(3)]. The crystal structure of 1 confirms the meridional geometry of the complex cation. The square planar geometry of copper complex 2 is confirmed by its crystal structure where the acetate function behaves as a monodentate ligand. The free ligand, LH, is found to be highly acidic in acetonitrile-water (1:1) medium and correspondingly the amine proton (NH) readily dissociates leading to its L- form even in absence of any external base. The pKb value of L- is determined to be 2.6. Both cobalt and copper complexes do not show any expected spin-allowed d-d transitions, possibly have masked by the intense charge-transfer transitions. However, in case of cobalt complex 1, one very weak unusual spin-forbidden 1A1g &#8594; 3T1g transition has been observed at 935 nm. The quasi-reversible cobalt (III)&#8596; cobalt(II) reduction of 1 is observed at E0, -1.0 V versus SCE. The reactions of bis(8-quinolinyl)amine [N1C9H6-N2H-C9H6N3, LH] with CoII(ClO4)2 . 6H2O, ZnII(ClO4)2 . 6H2O and CuII-acetate result in octahedral-[CoIII(L-)2]+ and [ZnII(L-)2] and square planar-[CuII(L-){-OC(=O)CH3}] complexes, respectively, incorporating an sp2-amido nitrogen center (N2) in the coordinated ligand frame of L. The structural, spectral and electrochemical aspects of the complexes have been described

An unedited 1.1 kb mitochondrial orfB gene transcript in the Wild Abortive Cytoplasmic Male Sterility (WA-CMS) system of Oryza sativa L. subsp. indica

<p>Abstract</p> <p>Background</p> <p>The application of hybrid rice technology has significantly increased global rice production during the last three decades. Approximately 90% of the commercially cultivated rice hybrids have been derived through three-line breeding involving the use of WA-CMS lines. It is believed that during the 21^stcentury, hybrid rice technology will make significant contributions to ensure global food security. This study examined the poorly understood molecular basis of the WA-CMS system in rice.</p> <p>Results</p> <p>RFLPs were detected for <it>atp6 </it>and <it>orfB </it>genes in sterile and fertile rice lines, with one copy of each in the mt-genome. The RNA profile was identical in both lines for <it>atp6</it>, but an additional longer <it>orfB </it>transcript was identified in sterile lines. 5' RACE analysis of the long <it>orfB </it>transcript revealed it was 370 bp longer than the normal transcript, with no indication it was chimeric when compared to the genomic DNA sequence. cDNA clones of the longer <it>orfB </it>transcript in sterile lines were sequenced and the transcript was determined unedited. Sterile lines were crossed with the restorer and maintainer lines, and fertile and sterile F₁hybrids were respectively generated. Both hybrids contained two types of <it>orfB </it>transcripts. However, the long transcript underwent editing in the fertile F₁hybrids and remained unedited in the sterile lines. Additionally, the editing of the 1.1 kb <it>orfB </it>transcript co-segregated with fertility restoring alleles in a segregating population of F₂progeny; and the presence of unedited long <it>orfB </it>transcripts was detected in the sterile plants from the F₂segregating population.</p> <p>Conclusion</p> <p>This study helped to assign plausible operative factors responsible for male-sterility in the WA cytoplasm of rice. A new point of departure to dissect the mechanisms governing the CMS-WA system in rice has been identified, which can be applied to further harness the opportunities afforded by hybrid vigor in rice.</p

PRIMARY CELL CULTURE OF AEDES ALBOPICTUS MIDGUT CELLS: A PROSPECTIVE MODEL FOR IN VITRO STUDY OF ARBOVIRUSES

  Objective: Midgut cells play a key role in the propagation of mosquito borne Arboviruses. The existing mosquito cell lines for studying viral pathogenesis are derived either from larvae or from eggs since there is no cell line available from the mosquito midgut. Therefore, to delineate the in situ viral interaction which naturally occurs within the mosquito midgut and represent cellular pathogenesis in human beings, the present work was aimed to develop a primary cell line from the midgut cells of Aedes albopictus.Methods: The midgut cells of A. albopictus were collected, cultured and incubated at 28°C to study the growth after every 24 hrs for 7 days.Result: The primary cell culture showed an increasing growth pattern of columnar cells up to 48 hrs followed by decrease in cell population afterward. However, the number of stem cells increased significantly throughout the study period, and their population outnumbered the columnar cells after 72 hrs. There was no significant change of goblet cells and regenerating cells which were scanty in number throughout the experiment.Conclusion: The present method will help to develop the individual cell lines from mosquito midgut and study the host pathogen interaction in arboviral diseases in future

Non-commutative Quantum Mechanics in Three Dimensions and Rotational Symmetry

We generalize the formulation of non-commutative quantum mechanics to three dimensional non-commutative space. Particular attention is paid to the identification of the quantum Hilbert space in which the physical states of the system are to be represented, the construction of the representation of the rotation group on this space, the deformation of the Leibnitz rule accompanying this representation and the implied necessity of deforming the co-product to restore the rotation symmetry automorphism. This also implies the breaking of rotational invariance on the level of the Schroedinger action and equation as well as the Hamiltonian, even for rotational invariant potentials. For rotational invariant potentials the symmetry breaking results purely from the deformation in the sense that the commutator of the Hamiltonian and angular momentum is proportional to the deformation.Comment: 21 page