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  • Ornstein-Zernike equation  (4)
  • Podospora mitochondrial DNA  (3)
  • Springer  (7)
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  • Springer  (7)
  • 1
    ISSN: 1432-0983
    Keywords: Podospora mitochondrial DNA ; Senescence-associated plasmid ; Intron secondary structure ; Intronic reading frames
    Source: Springer Online Journal Archives 1860-2000
    Topics: Biology
    Notes: Summary Recently, the nucleotide sequences for three “mitochondrial plasmids” associated with senescence of Podospora anserina were determined (Cummings et al. 1985). One of these sequences, corresponding to the plasmid termed ε senDNA, contains three class I introns, all within a protein coding sequence equivalent to the mammalian “URF1” gene. Here, we present primary and secondary structure analyses for two of these introns as well as a partial analysis for the third, which extends beyond the DNA sequence determined. With regard to both primary and secondary structure, the closest known relative of intron 1 is the self-splicing intron in the large ribosomal RNA gene of Tetrahymena. One secondary structure domain at the periphery of intron 1 and Tetrahymena models is also present in intron 2. The latter intron is the longest known class I member and contains remnants of two protein-coding sequences, one of which is split by the other. Evolutionary processes that might be responsible for the unusual structure of introns 1 and 2 are discussed.
    Type of Medium: Electronic Resource
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  • 2
    ISSN: 1432-0983
    Keywords: Podospora mitochondrial DNA ; Intron secondary structure ; Intron reading frames ; Group I and group II introns
    Source: Springer Online Journal Archives 1860-2000
    Topics: Biology
    Notes: Summary The DNA sequence of a 26.7 Kilobase pair (103 base pairs = 1 Kb) region of the mitochondrial genomes of races s and A from Podospora anserina was determined. Within this region, the 24.5 Kb cytochrome oxidase subunit I gene was located and its exon sequences determined by computer analysis comparisons with other fungal genes. The Podospora COI gene was interrupted by two group II introns (one in race s) and fourteen group I introns ranging in size from about 2.2 Kb to 404 bp. Earlier studies on secondary structure analysis, as well as comparison of their open reading frames (ORFs), showed that the two group II introns were closely related. The fourteen group I introns were representatives of three subgroupings (IB, C and a new category, subgroup ID). Two of these group I introns were separated by just a single exon codon. The analysis of all these introns is discussed in comparison with other fungal introns as well as with the known Podospora anserina introns.
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  • 3
    ISSN: 1432-0983
    Keywords: Podospora mitochondrial DNA ; Introns ; Excision ; Amplification plasmids
    Source: Springer Online Journal Archives 1860-2000
    Topics: Biology
    Notes: Summary The complete 94,192 bp sequence of the mitochondrial genome from race s of Podospora anserina is presented (1 kb=103 base pairs). Three regions unique to race A are also presented bringing the size of this genome to 100,314 bp. Race s contains 31 group I introns (33 in race A) and 2 group II introns (3 in race A). Analysis shows that the group I introns can be categorized according to families both with regard to secondary structure and their open reading frames. All identified genes are transcribed from the same strand. Except for the lack of ATPase 9, the Podospora genome contains the same genes as its fungal counterprts, N. crassa and A. nidulans. About 20% of the genome has not yet been identified. DNA sequence studies of several excision-amplification plasmids demonstrate a common feature to be the presence of short repeated sequences at both termini with a prevalence of GGCGCAAGCTC.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    Springer
    Journal of statistical physics 24 (1981), S. 405-412 
    ISSN: 1572-9613
    Keywords: Ornstein-Zernike equation ; soft-core fluid ; Yukawa closure ; electrolyte ; fused salts
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract A model for dense electrolytes and fused salts is proposed which incorporates both the known long-range asymptotic form for the direct correlation function and a parametric form for the total correlation function appropriate to a soft-core interaction potential. A special case extending the MSA for the restricted primitive model for electrolytes is discussed in some detail.
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  • 5
    Electronic Resource
    Electronic Resource
    Springer
    Journal of statistical physics 21 (1979), S. 659-667 
    ISSN: 1572-9613
    Keywords: Ornstein-Zernike equation ; Baxter's factorization ; softcore ; Yukawa closure
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract A model for simple fluids is proposed in which the radial distribution function has a parametric form appropriate to a soft-core fluid for interparticle separationr ⩽ R, whereR is some range parameter. Forr 〉 R, the direct correlation function is assumed to be of Yukawa form. The Ornstein-Zernike equation is solved for this system, yielding the radial distribution and the total correlation function for the entire range of interparticle separation. Methods of relating the model fluid to a real fluid by assigning values to the parameters are discussed.
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  • 6
    Electronic Resource
    Electronic Resource
    Springer
    International journal of thermophysics 11 (1990), S. 97-107 
    ISSN: 1572-9567
    Keywords: critical phenomena ; integral equation approximations ; numerical methods ; Ornstein-Zernike equation
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract A new numerical technique for solving the Ornstein-Zernike equation is described. It is particularly useful in solving the Ornstein-Zernike equation for approximations and pair potentials (such as the Percus-Yevick and mean spherical approximations for finite ranged potentials) which imply a finiteranged direct correlation function since for such approximations the numerical technique is essentially exact. The only approximation involved in such cases is the discretization of direct and total correlation functions over the finite range on which the direct correlation function is nonzero. Thus, the new method avoids truncation of the total correlation function and should permit the critical point and spinodal curve to be mapped out with greater accuracy than is permitted by existing methods. Preliminary explorations on the stability and accuracy of the method are described.
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  • 7
    Electronic Resource
    Electronic Resource
    Springer
    International journal of thermophysics 6 (1985), S. 573-584 
    ISSN: 1572-9567
    Keywords: critical phenomena ; integral-equation theory ; Ornstein-Zernike equation ; Percus-Yevick theory
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract There has been much recent interest in the behavior of integral-equation theories for the distribution functions of a fluid near the critical point and in the two-phase region. For most systems, implementation of these theories necessitates numerical solution of the integral equations. However, for two examples, the adhesive hard sphere fluid in the Percus-Yevick approximation and the hard sphere plus Yukawa tail model in the mean spherical approximation, analytical solutions of the Ornstein-Zernike equation are available. In this work we consider the comparison of results obtained via numerical methods with the analytical solution of the Percus-Yevick equation for the adhesive hard sphere fluid. This complements a recent study by us of the mean spherical approximation for the hard sphere plus Yukawa tail fluid. This allows us to examine carefully how errors arise in the numerical solutions. We examine the accuracy of numerical calculations of the critical exponents as well as the interpretation of solutions obtained in the coexistence region. We discuss the implications of this work for applications to more realistic potentials where only numerical solutions are available.
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