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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 94 (1991), S. 1543-1554 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We consider polyampholyte polymers containing both positive and negative monomers randomly dispersed along the chain. Neutral chains collapse into a globule due to attractive electrostatic interactions. The behavior of the charges inside the globule is similar to that of charges in a small volume of simple electrolyte. A screening length κ−1p coming from the polymeric charge may be defined as in Debye–Hückel theory. The internal structure of the globule is that of close packed blobs of radius equal to the screening length. When salt is added this further screens the interactions and reduces the attractions. The globule begins to increase in size when the concentration of salt becomes larger than the concentration of charge on the polymer itself. Screened Coulomb interactions in a neutral chain behave like a negative contribution to excluded volume. For a chain in a good solvent there is a θ salt concentration at which the net excluded volume becomes zero. Chains are swollen above this concentration of salt, and collapsed below this concentration. For small sections of chain the Coulomb interactions are unscreened and cannot be treated as a modification to excluded volume. Chains with a strong net charge of one sign tend to behave as conventional polyelectrolyte with charges of only one sign. We determine the criterion for the value of the net charge at which the repulsions (polyelectrolyte effect) begin to dominate the attractions (polyampholyte effect). The predictions are found to be in good qualitative agreement with experiments.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 100 (1994), S. 640-648 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We investigate models for the growth of crystals of monodisperse polymer chains. A transition from extended chain crystals to folded chain crystals occurs as the temperature is changed which is governed by the kinetics of adsorption and desorption of chains at the growth surface. Folded chains may build up on the surface of growing extended chain crystals and slow down the growth. This effect is particularly strong at the transition temperature, where the folded chains are marginally stable. Hence there is a sharp minimum in the growth velocity at this point. We compare the results of the model to experiments on crystallization of long alkanes and poly (ethylene oxide) fractions. In some cases there is an instability in the growth surface leading to patterns of crevices resembling those seen during the thickening of folded chain alkane lamellae. Sliding and rearrangement of molecules underneath the crystal surface is important to allow smooth surface growth. Sliding processes are also the dominant factor controlling the growth rate at temperatures close to the transition.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 105 (1996), S. 7152-7157 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: When RNA secondary structures predicted by free energy minimization programs are compared with the structures obtained by phylogenetic comparison it is found that there are often substantial differences. Here we consider a sample of large RNA molecules including 16S and 23S ribosomal RNA, and RNaseP RNA, and compare the minimum free energy and phylogenetic structures for domains of different size within the molecule. The pattern of differences between the structures is consistent with the idea that the native structures are influenced by the kinetics of the folding process, rather than solely by free energy minimization. It is found that the free energy of small domains in the phylogenetic structure of size 100 bases or less is usually much lower (i.e., more stable) than the average value of the minimum free energy of typical domains of corresponding size, whereas the reverse is true for large domains. We interpret these results using a picture of the folding process where short range secondary structure elements form first, which gradually rearrange to form domains of larger and larger size. Once low free energy domains of a moderate size are formed, these structures will remain trapped, because free energy barriers associated with structural rearrangement will be too large. The result is a structure containing small low free energy domains linked by a few longer range helices which fit in as best they can at a later stage of folding. We also discuss other possible causes of error in the predicted minimum free energy structures, and conclude that the difference between the minimum free energy and the phylogenetic structures cannot simply be put down to errors in the free energy parameters used in the model. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 108 (1998), S. 4305-4314 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Polymer crystallization in dilute solution is studied by three-dimensional Monte-Carlo simulations using the bond fluctuation model. We study monodisperse chains of moderate length, intended to model recent experiments on monodisperse alkanes with length of a few hundred carbon atoms, and we also investigate chain folding of very long polymers. For monodisperse flexible chains we observe both extended-chain and once-folded-chain crystals. The simulations illustrate the range of defects and irregularities which we expect to find in polymer crystals. The roughness of the top and bottom surfaces of the lamellae is measured. Chain ends can be seen as cilia emerging from the surfaces. Folds are found to occur with approximately equal frequency on top and bottom surfaces. Although most chain folds are aligned perpendicular to the growth direction, a significant number of chains folding parallel to the growth direction are found as defects. The simulation includes a chain stiffness parameter which has an important effect on chain folding kinetics. When chains are semi-flexible the crystals formed are extremely irregular with many defects including holes and blocks of extended chains within the folded chain lamellae. For very long chains we show that the lamellar thickness is determined by the folding kinetics. The thickness diverges as the temperature approaches the infinite chain melting point T∞. For T→T∞, the thickness is close to the theoretical minimum thickness, which indicates the dominant importance of the entropic barrier in crystallization. © 1998 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 114 (2001), S. 6958-6959 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Monodisperse long-chain alkanes such as C198H398 form lamellar crystals in both extended- and folded-chain forms. Folded-chain crystals are in a meta-stable equilibrium with polymer solution at a concentration CF. The crystal growth rate is virtually zero at this point, due to the self-poisoning phenomenon. If extended-chain crystallization is initiated from this state, a wave of crystallization proceeds through the solution, termed the dilution wave. The solution concentration falls as the wave passes, until a value CE is reached that is in equilibrium with the extended-chain crystal phase. We write down a reaction-diffusion equation to describe the dilution wave, and show that this is equivalent to Fisher's equation, which has previously been used to describe many other traveling wave phenomena. Numerical solutions of the equation are used to show examples of the wave shape. © 2001 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    Springer
    Journal of molecular evolution 35 (1992), S. 454-465 
    ISSN: 1432-1432
    Keywords: Genetic distance ; Neutral theory ; Speciation
    Source: Springer Online Journal Archives 1860-2000
    Topics: Biology
    Notes: Summary We compare the behavior of the genetic distance between individuals in evolving populations for three stochastic models. In the first model reproduction is asexual and the distribution of genetic distances reflects the genealogical tree of the population. This distribution fluctuates greatly in time, even for very large populations. In the second model reproduction is sexual with random mating allowed between any pair of individuals. In this case, the population becomes homogeneous and the genetic distance between pairs of individuals has small fluctuations which vanish in the limit of an infinitely large population. In the third model reproduction is still sexual but instead of random mating, mating only occurs between individuals which are genetically similar to each other. In that case, the population splits spontaneously into species which are in reproductive isolation from one another and one observes a steady state with a continual appearance and extinction of species in the population. We discuss this model in relation to the biological theory of speciation and isolating mechanisms. We also point out similarities between these three models of evolving populations and the theory of disordered systems in physics.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    Springer
    Journal of mathematical biology 33 (1995), S. 677-702 
    ISSN: 1432-1416
    Keywords: Muller's ratchet ; Neutral evolution ; Mutation-selection balance ; Genealogical trees
    Source: Springer Online Journal Archives 1860-2000
    Topics: Biology , Mathematics
    Notes: Abstract We study the accumulation of unfavourable mutations in asexual populations by the process of Muller's ratchet, and the consequent inevitable decrease in fitness of the population. Simulations show that it is mutations with only moderate unfavourable effect that lead to the most rapid decrease in fitness. We measure the number of fixations as a function of time and show that the fixation rate must be equal to the ratchet rate once a steady state is reached. Large bursts of fixations are observed to occur simultaneously. We relate this to the structure of the genealogical tree. We derive equations relating the rate of the ratchet to the moments of the distribution of the number of mutations k per individual. These equations interpolate between the deterministic limit (an infinite population with selection present) and the neutral limit (a finite size population with no selection). Both these limits are exactly soluble. In the neutral case, the distribution of k is shown to be non-self-averaging, i.e. the fluctuations remain very large even for very large populations. We also consider the strong-selection limit in which only individuals in the fittest surviving class have offspring. This limit is again exactly soluble. We investigate the structure of the genealogical tree relating individuals in the same population, and consider the probability $$\bar P$$ (T) that two individuals had their latest common ancestor T generations in the past. The function $$\bar P$$ (T) is exactly calculable in the neutral limit and the strong-selection limit, and we obtain an empirical solution for intermediate selection strengths.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    Springer
    Genetica 102-103 (1998), S. 91-101 
    ISSN: 1573-6857
    Keywords: compensatory mutations ; random drift ; RNA evolution ; shifting balance
    Source: Springer Online Journal Archives 1860-2000
    Topics: Biology
    Notes: Abstract There are many examples of RNA molecules in which the secondary structure has been strongly conserved during evolution, but the base sequence is much less conserved, e.g., transfer RNA, ribosomal RNA, and ribonuclease P. A model of compensatory neutral mutations is used here to describe the evolution of the base sequence in RNA helices. There are two loci (i.e., the two sides of the pair) with four alleles at each locus (corresponding to A, C, G, U). Watson-Crick base pairs (AU, CG, GC, and UA) are each assigned a fitness 1, whilst all other pairs are treated as mismatches and assigned fitness 1-s. A population of N diploid individuals is considered with a mutation rate of u per base. For biologically reasonable parameter values, the frequency of mismatches is always small but the frequency of the four matching pairs can vary over a wide range. Using a diffusion model, the stationary distribution for the frequency x of any of the four matching pairs is calculated. The shape depends on the combination of variables β = 8Nu2/9s. For small β, the distribution diverges at the two extremes, x = 0 and x = 1-z, where z is the mean frequency of mismatches. The population typically consists almost entirely of one of the four types of matching pairs, but occasionally makes shifts between the four possible states. The mean rate at which these shifts occur is calculated here. The effect of recombination between the two loci is to decrease the probability density at intermediate x, and to increase the weight at the extremes. The rate of transition between the four states is slowed by recombination (as originally shown by Kimura in a two-allele model with irreversible mutation). A very small recombination rate r ∼ u2/s is sufficient to increase the mean time between transitions dramatically. In addition to its application to RNA, this model is also relevant to the ‘shifting balance’ theory describing the drift of populations between alternative equilibria separated by low fitness valleys. Equilibrium values for the frequencies of the different allele combinations in an infinite population are also calculated. It is shown that for low recombination rates the equilibrium is symmetric, but there is a critical recombination rate above which alternative asymmetric equilibria become stable.
    Type of Medium: Electronic Resource
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