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  • 1
    ISSN: 1365-2958
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Biology , Medicine
    Notes: The PulO protein required for extracellular secretion of pullulanase by Klebsiella oxytoca is known to be highly homologous to two type IV prepilin peptidases, namely XcpA(PilD) (Pseudomonas aeruginosa) and TcpJ (Vibrio cholerae). The predicted prepilin peptidase activity of PulO was confirmed by showing that it could correctly process the product of the cloned pilE.1 type IV pilin structural gene from Neisseria gonorrhoeae in Escherichia coli. The P. aeruginosa prepilin peptidase and another putative prepilin peptidase, ComC from Bacillus subtilis, also processed prePilE. Subcellular fractionation showed that the pilE gene product that had been processed by PulO remained associated with the cytoplasmic membrane, as did the unprocessed precursor. PulO was also shown to process three of the four prePilE–PhoA hybrids tested. Southern hybridization experiments suggest that a PulO homologue is present in the N. gonorrhoeae chromosome.
    Type of Medium: Electronic Resource
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  • 2
    ISSN: 1476-4687
    Source: Nature Archives 1869 - 2009
    Topics: Biology , Chemistry and Pharmacology , Medicine , Natural Sciences in General , Physics
    Notes: [Auszug] An examination of the biology of the gonococcus suggested that there was an alternative mechanism to gene conversion for pilin antigenic variation. Piliated gonococci are naturally competent for DNA transformation throughout their life cycle9, and this process is dependent on homologous ...
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  • 3
    Electronic Resource
    Electronic Resource
    Springer
    Earth, moon and planets 22 (1980), S. 359-366 
    ISSN: 1573-0794
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences , Physics
    Notes: Abstract Fission from the Earth's mantle explains why the density of the Moon is similar to that of the Earth's mantle. If following the fission origin of the Moon, the Earth-Moon distance increases progressively, the Moon can recollect chemicals evaporated by the Earth but not volatile enough to be lost as gases. In this way, the surface of the Moon can be enriched in refractory elements as most of the authors have proposed. At 3 Earth radii the long geosynchronous phase allows the formation of a solid crust which will record the Earth's magnetic field and the equilibrium hydrostatic from at that distance. When geosynchronism is broken the Moon will recede; its shape will no longer fit the hydrostatic form. The crust will either break or will exercise pressure on the lower layers. Meteor craters will allow lava to come to the surface. Such flows will be very large where the shape of the crust does not fit at all the geosynchronous form. Large lava flows will appear this way on the near side where the shape has changed the most. The new lava flows no longer record the magnetic field of the Earth because with the end of the synchronous position the field is alternative for the Moon; only the remanent field can influence the new lava. Three out of five samples dated at 3.6 b.y. suggest nevertheless that the field decreased slowly without becoming alternative. This means that the geosynchronous phase may have lasted longer and put the Moon on a more distant orbit, as Alfvén and Arrhenius suggested. The interpretation of lunar magnetism as influenced by the Earth cannot discard any interpretation or suggestion of its own lunar magnetic process. It is quite possible that both mechanisms have worked as some samples show.
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  • 4
    Electronic Resource
    Electronic Resource
    Springer
    Earth, moon and planets 22 (1980), S. 347-358 
    ISSN: 1573-0794
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences , Physics
    Notes: Abstract The problem of the origin of the Moon has led to various hypotheses: simultaneous accretion, fission, capture, etc. These theories were based primarily on global mechanical considerations. New geological data (Turcotteet al., 1974; Kahn and Pompea, 1978) have led to fresh approaches and new versions of these theories. As suggested by Wise (1969) and O'Keefe (1972), the initial Earth may have taken unstable forms when radial segregation sped up the rotation. The Moon may have been created as the small part of the pyroid of Poincaré. Fission theory was mainly discarded, in the past, on the basis of energy considerations. We are now arriving at the conclusion that these considerations are void if the fission was followed by a very long period of geostationary rotation of the Moon at a distance of about 3 Earth radius (i.e., out of the Roche limit). Indeed the large amount of energy of the initial system could have been released slowly and therefore evacuated by losses of material and radiation. The accretion of the Earth and the radial segregation of heavy chemicals toward the center has led to a differential rotation of the different layers with a faster rotation at the center. During the geostationary period the Moon was synchronous with respect to the surface layer. That Earth-Moon system has both a correct angular momentum and a large stability provided that the viscosity of intermediate layers was small enough, which is in concordance with its high temperature. Even with a very hot system, a superficial cold layer appears because of its low conductivity and the radiation equilibrium with outer space. This implies a slow loss of energy: the geosynchronous Moon receded extremely slowly. During the geostationary period lithophile elements were extracted with water by the radial segregation and were deposited in the area facing the Moon. One massive continent was formed, as suggested by Grjebine (1978). As the continent became thicker and sank into the mantle, convection currents appeared and speeded up the cooling of the Earth. The viscosity increased and the synchronization between the Moon and the surface of the Earth became more difficult to maintain. When synchronism was broken important lunar tides transferred energy and momentum from the Earth to the Moon which receded toward its present position and the modification of its equilibrium shape explains the formation of lunar maria in the near side.
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  • 5
    Electronic Resource
    Electronic Resource
    Springer
    Celestial mechanics and dynamical astronomy 34 (1984), S. 65-93 
    ISSN: 1572-9478
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract In the first part of this paper [Marchal, Yoshida, Sun Yi-Sui 1985] we have analyzed three-body systems satisfying the condition r≦kR where k is a suitable constant, r the mutual distance of the two masses of the “binary” and R the distance between the center of mass of the binary and the “third mass”. That condition r≦kR puts limits on the acceleration of the third mass and these limits allow us to determine the corresponding “escape velocities”. In this second part we look for initial conditions under which the inequality r≦kR will remain forever satisfied and we develop the corresponding tests of escape and their applications. This leads to a major improvement of the knowledge of the nature of three-body motions especially in the vicinity of triple close approaches. The region of bounded motions is much smaller than was generally expected and numerical computations of particular solutions show that we approach very near to the true limit.
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  • 6
    Electronic Resource
    Electronic Resource
    Springer
    Celestial mechanics and dynamical astronomy 12 (1975), S. 115-129 
    ISSN: 1572-9478
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract For the general three-body problem we show the existence and describe regions in physical space and configuration space where motion cannot occur. The description of these regions turns out to be most similar to the Hill regions of the circular restricted problem of three bodies. These regions depend upon the constants of energy and angular momentum.
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  • 7
    Electronic Resource
    Electronic Resource
    Springer
    Celestial mechanics and dynamical astronomy 9 (1974), S. 381-393 
    ISSN: 1572-9478
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The three-body problem is decomposed into the motion of the binarym 1,m 2 and the motion of the third massm 3 with respect to the center of masses ofm 1 andm 2. Some limitations are assumed on the motion of the binarym 1,m 2 which imply limits on the motion ofm 3; in favourable cases these limits are within the same type of evolution and thus analytic sufficient for the hyperbolic-elliptic escape and for the ‘ejection without escape’: the ejected massm 3 reaches a bounded distance and falls back towardm 1 andm 2. The limitations assumed on the motion of the binarym 1,m 2 are verified with the help of the energy integral. The new criteria are compared with those given in the literature. They are generally more efficient. In particular they are the only ones which can be used with zero or negative radial velocity of the massm 3. They can even be used sometimes at time minus infinity, that is infinitely before the passage of a star near a binary system.
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  • 8
    Electronic Resource
    Electronic Resource
    Springer
    Celestial mechanics and dynamical astronomy 33 (1984), S. 193-207 
    ISSN: 1572-9478
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract Let us consider a three-body system with three given pointmasses and let us analyze its bounded solutions with a given angular momentum. Among these bounded solutions we found the three usual families of elliptic Euler solutions, with collinear central configurations, and a beautiful result would have been the following: ‘The greatest lower bound of the moment of inertia (with respect to the center of masses) for these elliptic Euler solutions is also the greatest lower bound for all bounded solutions of the same masses and angular momentum’. With the help of a new efficient test of escape we found that the greatest lower bound is always at least 99.9% of the above desired value and we think that the above conjecture is always true. This new test also leads to many adjacent results and especially, for the present, to the smallest delimitation of the zone of bounded motions. As other tests ours uses the Jacobi decomposition of the three-body motion with r being the mutual distance of the two masses of the ‘binary’ and R the distance between the center of mass of the binary and the ‘third mass’. The study is divided into two parts. In the first we analyze the motion of the third mass, its acceleration and its escape velocities when, with a suitable scalar k, a condition of the type r≦kR remains forever satisfied. In the second part we will look for initial conditions under which the inequality r≦kR will remain forever satisfied and we will develop the corresponding test and its applications.
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  • 9
    Electronic Resource
    Electronic Resource
    Springer
    Celestial mechanics and dynamical astronomy 26 (1982), S. 311-333 
    ISSN: 1572-9478
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The notion of Hill stability is extended from the circular restricted 3-body problem to the general three-body problem; it is even extended to systems of positive energy and the Hill's curves with their corresponding forbidden zones are generalized. Hill stable systems of negative energy present a hierarchy: they have a close binary that can be neither approached nor disrupted by the third body. This phenomenon becomes particularly clear with the distance curves presentation. The three limiting cases, restricted, planetary and lunar are analysed as well as some real stellar cases.
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  • 10
    Electronic Resource
    Electronic Resource
    Springer
    Celestial mechanics and dynamical astronomy 32 (1984), S. 15-28 
    ISSN: 1572-9478
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Description / Table of Contents: Résumé En utilisant les résultats de Sundman et de Birkhoff ainsi que les études sur les courbes de Hill généralisées, on développe une nouvelle méthode pour calculer un minorant du moment d'inertie pour les orbites bornées dans le problème des trois corps. On obtient ainsi des valeurs beaucoup plus élevées que dans les résultats classiques. On montre en particulier que lorsque I'intégrale de I'énergie tend vers zéro ce minorant tend vers le minimum du moment d'inertie du mouvement parabolique d'Euler correspondant de même moment cinétique: c'est alors la limite inférieure.
    Notes: Abstract Using the results of Sundman and Birkhoff as also the studies on the generalized Hill's curves, we develop a new method for computing a lower bound of the moment of inertia for the bounded orbits in the general three-body problem. Thus we obtain much higher values than in the classical results. We show for instance, that when the integral of the energy goes to zero, this lower bound goes to the minimum moment of inertia of the corresponding parabolic Euler motion of the same angular momentum: it is then the greatest lower bound.
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