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  • 1
    Keywords: Nuclear structure. ; Electronic books.
    Description / Table of Contents: Enhanced by a number of solved problems and examples, this volume will be a valuable resource to advanced undergraduate and graduate students in chemistry, chemical engineering, biochemistry biophysics, pharmacology, and computational biology.
    Type of Medium: Online Resource
    Pages: 1 online resource (397 pages)
    Edition: 1st ed.
    ISBN: 9781000072327
    Series Statement: Foundations of Biochemistry and Biophysics Series
    DDC: 572
    Language: English
    Note: Cover -- Half Title -- Series Page -- Title Page -- Copyright Page -- Dedication -- Table of Contents -- Preface -- Acknowledgments -- Author -- Section I: Probability Theory -- 1: Probability and Its Applications -- 1.1 Introduction -- 1.2 Experimental Probability -- 1.3 The Sample Space Is Related to the Experiment -- 1.4 Elementary Probability Space -- 1.5 Basic Combinatorics -- 1.5.1 Permutations -- 1.5.2 Combinations -- 1.6 Product Probability Spaces -- 1.6.1 The Binomial Distribution -- 1.6.2 Poisson Theorem -- 1.7 Dependent and Independent Events -- 1.7.1 Bayes Formula -- 1.8 Discrete Probability-Summary -- 1.9 One-Dimensional Discrete Random Variables -- 1.9.1 The Cumulative Distribution Function -- 1.9.2 The Random Variable of the Poisson Distribution -- 1.10 Continuous Random Variables -- 1.10.1 The Normal Random Variable -- 1.10.2 The Uniform Random Variable -- 1.11 The Expectation Value -- 1.11.1 Examples -- 1.12 The Variance -- 1.12.1 The Variance of the Poisson Distribution -- 1.12.2 The Variance of the Normal Distribution -- 1.13 Independent and Uncorrelated Random Variables -- 1.13.1 Correlation -- 1.14 The Arithmetic Average -- 1.15 The Central Limit Theorem -- 1.16 Sampling -- 1.17 Stochastic Processes-Markov Chains -- 1.17.1 The Stationary Probabilities -- 1.18 The Ergodic Theorem -- 1.19 Autocorrelation Functions -- 1.19.1 Stationary Stochastic Processes -- Homework for Students -- A Comment about Notations -- References -- Section II: Equilibrium Thermodynamics and Statistical Mechanics -- 2: Classical Thermodynamics -- 2.1 Introduction -- 2.2 Macroscopic Mechanical Systems versus Thermodynamic Systems -- 2.3 Equilibrium and Reversible Transformations -- 2.4 Ideal Gas Mechanical Work and Reversibility -- 2.5 The First Law of Thermodynamics -- 2.6 Joule's Experiment -- 2.7 Entropy -- 2.8 The Second Law of Thermodynamics. , 2.8.1 Maximal Entropy in an Isolated System -- 2.8.2 Spontaneous Expansion of an Ideal Gas and Probability -- 2.8.3 Reversible and Irreversible Processes Including Work -- 2.9 The Third Law of Thermodynamics -- 2.10 Thermodynamic Potentials -- 2.10.1 The Gibbs Relation -- 2.10.2 The Entropy as the Main Potential -- 2.10.3 The Enthalpy -- 2.10.4 The Helmholtz Free Energy -- 2.10.5 The Gibbs Free Energy -- 2.10.6 The Free Energy, , H.(T,µ) -- 2.11 Maximal Work in Isothermal and Isobaric Transformations -- 2.12 Euler's Theorem and Additional Relations for the Free Energies -- 2.12.1 Gibbs-Duhem Equation -- 2.13 Summary -- Homework for Students -- References -- Further Reading -- 3: From Thermodynamics to Statistical Mechanics -- 3.1 Phase Space as a Probability Space -- 3.2 Derivation of the Boltzmann Probability -- 3.3 Statistical Mechanics Averages -- 3.3.1 The Average Energy -- 3.3.2 The Average Entropy -- 3.3.3 The Helmholtz Free Energy -- 3.4 Various Approaches for Calculating Thermodynamic Parameters -- 3.4.1 Thermodynamic Approach -- 3.4.2 Probabilistic Approach -- 3.5 The Helmholtz Free Energy of a Simple Fluid -- Reference -- Further Reading -- 4: Ideal Gas and the Harmonic Oscillator -- 4.1 From a Free Particle in a Box to an Ideal Gas -- 4.2 Properties of an Ideal Gas by the Thermodynamic Approach -- 4.3 The chemical potential of an Ideal Gas -- 4.4 Treating an Ideal Gas by the Probability Approach -- 4.5 The Macroscopic Harmonic Oscillator -- 4.6 The Microscopic Oscillator -- 4.6.1 Partition Function and Thermodynamic Properties -- 4.7 The Quantum Mechanical Oscillator -- 4.8 Entropy and Information in Statistical Mechanics -- 4.9 The Configurational Partition Function -- Homework for Students -- References -- Further Reading -- 5: Fluctuations and the Most Probable Energy -- 5.1 The Variances of the Energy and the Free Energy. , 5.2 The Most Contributing Energy E* -- 5.3 Solving Problems in Statistical Mechanics -- 5.3.1 The Thermodynamic Approach -- 5.3.2 The Probabilistic Approach -- 5.3.3 Calculating the Most Probable Energy Term -- 5.3.4 The Change of Energy and Entropy with Temperature -- References -- 6: Various Ensembles -- 6.1 The Microcanonical (petit) Ensemble -- 6.2 The Canonical (NVT) Ensemble -- 6.3 The Gibbs (NpT) Ensemble -- 6.4 The Grand Canonical (µVT) Ensemble -- 6.5 Averages and Variances in Different Ensembles -- 6.5.1 A Canonical Ensemble Solution (Maximal Term Method) -- 6.5.2 A Grand-Canonical Ensemble Solution -- 6.5.3 Fluctuations in Different Ensembles -- References -- Further Reading -- 7: Phase Transitions -- 7.1 Finite Systems versus the Thermodynamic Limit -- 7.2 First-Order Phase Transitions -- 7.3 Second-Order Phase Transitions -- References -- 8: Ideal Polymer Chains -- 8.1 Models of Macromolecules -- 8.2 Statistical Mechanics of an Ideal Chain -- 8.2.1 Partition Function and Thermodynamic Averages -- 8.3 Entropic Forces in an One-Dimensional Ideal Chain -- 8.4 The Radius of Gyration -- 8.5 The Critical Exponent ν -- 8.6 Distribution of the End-to-End Distance -- 8.6.1 Entropic Forces Derived from the Gaussian Distribution -- 8.7 The Distribution of the End-to-End Distance Obtained from the Central Limit Theorem -- 8.8 Ideal Chains and the Random Walk -- 8.9 Ideal Chain as a Model of Reality -- References -- 9: Chains with Excluded Volume -- 9.1 The Shape Exponent ν for Self-avoiding Walks -- 9.2 The Partition Function -- 9.3 Polymer Chain as a Critical System -- 9.4 Distribution of the End-to-End Distance -- 9.5 The Effect of Solvent and Temperature on the Chain Size -- 9.5.1 θ Chains in d = 3 -- 9.5.2 θ Chains in d = 2 -- 9.5.3 The Crossover Behavior Around -- 9.5.4 The Blob Picture -- 9.6 Summary -- References. , Section III: Topics in Non-Equilibrium Thermodynamics and Statistical Mechanics -- 10: Basic Simulation Techniques: Metropolis Monte Carlo and Molecular Dynamics -- 10.1 Introduction -- 10.2 Sampling the Energy and Entropy and New Notations -- 10.3 More About Importance Sampling -- 10.4 The Metropolis Monte Carlo Method -- 10.4.1 Symmetric and Asymmetric MC Procedures -- 10.4.2 A Grand-Canonical MC Procedure -- 10.5 Efficiency of Metropolis MC -- 10.6 Molecular Dynamics in the Microcanonical Ensemble -- 10.7 MD Simulations in the Canonical Ensemble -- 10.8 Dynamic MD Calculations -- 10.9 Efficiency of MD -- 10.9.1 Periodic Boundary Conditions and Ewald Sums -- 10.9.2 A Comment About MD Simulations and Entropy -- References -- 11: Non-Equilibrium Thermodynamics-Onsager Theory -- 11.1 Introduction -- 11.2 The Local-Equilibrium Hypothesis -- 11.3 Entropy Production Due to Heat Flow in a Closed System -- 11.4 Entropy Production in an Isolated System -- 11.5 Extra Hypothesis: A Linear Relation Between Rates and Affinities -- 11.5.1 Entropy of an Ideal Linear Chain Close to Equilibrium -- 11.6 Fourier's Law-A Continuum Example of Linearity -- 11.7 Statistical Mechanics Picture of Irreversibility -- 11.8 Time Reversal, Microscopic Reversibility, and the Principle of Detailed Balance -- 11.9 Onsager's Reciprocal Relations -- 11.10 Applications -- 11.11 Steady States and the Principle of Minimum Entropy Production -- 11.12 Summary -- References -- 12: Non-equilibrium Statistical Mechanics -- 12.1 Fick's Laws for Diffusion -- 12.1.1 First Fick's Law -- 12.1.2 Calculation of the Flux from Thermodynamic Considerations -- 12.1.3 The Continuity Equation -- 12.1.4 Second Fick's Law-The Diffusion Equation -- 12.1.5 Diffusion of Particles Through a Membrane -- 12.1.6 Self-Diffusion -- 12.2 Brownian Motion: Einstein's Derivation of the Diffusion Equation. , 12.3 Langevin Equation -- 12.3.1 The Average Velocity and the Fluctuation-Dissipation Theorem -- 12.3.2 Correlation Functions -- 12.3.3 The Displacement of a Langevin Particle -- 12.3.4 The Probability Distributions of the Velocity and the Displacement -- 12.3.5 Langevin Equation with a Charge in an Electric Field -- 12.3.6 Langevin Equation with an External Force-The Strong Damping Velocity -- 12.4 Stochastic Dynamics Simulations -- 12.4.1 Generating Numbers from a Gaussian Distribution by CLT -- 12.4.2 Stochastic Dynamics versus Molecular Dynamics -- 12.5 The Fokker-Planck Equation -- 12.6 Smoluchowski Equation -- 12.7 The Fokker-Planck Equation for a Full Langevin Equation with a Force -- 12.8 Summary of Pairs of Equations -- References -- 13: The Master Equation -- 13.1 Master Equation in a Microcanonical System -- 13.2 Master Equation in the Canonical Ensemble -- 13.3 An Example from Magnetic Resonance -- 13.3.1 Relaxation Processes Under Various Conditions -- 13.3.2 Steady State and the Rate of Entropy Production -- 13.4 The Principle of Minimum Entropy Production-Statistical Mechanics Example -- References -- Section IV: Advanced Simulation Methods: Polymers and Biological Macromolecules -- 14: Growth Simulation Methods for Polymers -- 14.1 Simple Sampling of Ideal Chains -- 14.2 Simple Sampling of SAWs -- 14.3 The Enrichment Method -- 14.4 The Rosenbluth and Rosenbluth Method -- 14.5 The Scanning Method -- 14.5.1 The Complete Scanning Method -- 14.5.2 The Partial Scanning Method -- 14.5.3 Treating SAWs with Finite Interactions -- 14.5.4 A Lower Bound for the Entropy -- 14.5.5 A Mean-Field Parameter -- 14.5.6 Eliminating the Bias by Schmidt's Procedure -- 14.5.7 Correlations in the Accepted Sample -- 14.5.8 Criteria for Efficiency -- 14.5.9 Locating Transition Temperatures -- 14.5.10 The Scanning Method versus Other Techniques. , 14.5.11 The Stochastic Double Scanning Method.
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 97 (1992), S. 5816-5823 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: As in the preceding paper (Paper I) we study here a model of chains with excluded volume enclosed in a "box'' on a square lattice. The system is simulated by the Metropolis Monte Carlo method and the entropy is extracted from the samples by using the "hypothetical scanning method.'' With this method each system configuration is treated as if it has been generated step by step with the scanning method (studied in Paper I). The transition probabilities are reconstructed and three approximations of the entropy are obtained. Thus the pressure and the chemical potential are calculated directly from the results of the entropy as in Paper I using standard thermodynamic relations. These results are found to be in a very good agreement with those obtained in Paper I, which are considered to be exact within the statistical error.
    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 97 (1992), S. 5803-5815 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Using the scanning simulation method we study a system of many chains with excluded volume contained in a "box'' on a square lattice. With this method an initially empty box is filled with the chains monomers step by step with the help of transition probabilities. The probability of construction, P of the whole system is the product of the transition probabilities used and hence the entropy S is known, (S∼ln P). Thus the pressure and the chemical potential can be calculated with high accuracy directly from the entropy using standard thermodynamic relations. In principle, all these quantities can be obtained from a single sample without the need to carry out any thermodynamic integration. Various alternatives for performing the scanning construction are discussed and their efficiency is examined. This is important due to the fact that for lattice polymer models the scanning method is ergodic (unlike some dynamical Monte Carlo techniques). The computer simulation results are compared to the approximate theories of Flory, Huggins, Miller, and Guggenheim and to the recent improved theories of Freed and co-workers.
    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 92 (1990), S. 5144-5154 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Using the scanning simulation method we study the tricritical behavior at the Flory θ-point of self-avoiding walks (SAWs) with nearest neighbors attractions ε (ε〈0) on a simple cubic lattice (in the following paper we investigate tricritical trails on the same lattice). The tricritical temperature Tt is −ε/kBTt=0.274±0.006 (one standard deviation). The results for the radius of gyration G and the end-to-end distance R are consistent with the theoretical prediction νt=0.5 and with a logarithmic correction to scaling; the ratio G2/R2 =0.1659±0.0001 (calculated without taking into account correction to scaling) is only slightly smaller than the theoretical asymptotic value 1/6=0.1666.... The results for the partition function Z at Tt lead to γt=1.005±0.017 in accord with theory and to μt=5.058±0.014, where μt is the growth parameter; the correction to scaling in Z is found to be relatively small. For the chain length studied the divergence of the specific heat at Tt (αt(approximately-equal-to)0.3) is significantly larger than that predicted by theory, (ln N)3/11 (i.e., αt=0). Also, at Tt our data are affected by strong correction to scaling and are thus not consistent with the theoretical value of the crossover exponent φt=0.5.
    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 92 (1990), S. 5155-5161 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A self-attracting trail is a walk on a lattice which may intersect itself but two bonds are not allowed to overlap; an interaction energy ε (ε〈0) is associated with each self-intersection. Using the scanning simulation method, we study the tricritical behavior at the collapse transition of self-attracting trails of N≤250 steps on a simple cubic lattice. In the preceding paper (paper I) tricritical self-avoiding walks (SAWs) on the same lattice have been investigated. The tricritical temperature of trails is −ε/kBTt=0.550±0.004 (one standard deviation). The results for the radius of gyration, G, and the end-to-end distance, R, lead to νt=0.515±0.003, which is larger than νt=1/2, the theoretical prediction for SAWs. The ratio G2/R2=0.1676±0.0001 is slightly larger than 1/6=0.1666 ... predicted by theory for SAWs; The results for the partition function at Kt lead to γt=1.040±0.005 (as compared to the theoretical prediction for SAWs γt=1) and to the growth parameter value μt=5.0023±0.0020. The crossover exponent, φt, is approximately 0.5 as expected for SAWs at tricriticality; this value is significantly smaller than that found for SAWs in paper I. The results of G, R, and Z at Kt are found to be inconsistent with logarithmic corrections to scaling. However, we do not think that the above differences between trails and SAWs are sufficient to suggest unequivocally that the two models belong to different universality classes.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 89 (1988), S. 2514-2522 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The scanning method is a computer simulation technique for polymer chains, which is especially suitable to handle chains with finite interactions and chains that are subject to various geometrical constraints. A chain is constructed step by step with the help of transition probabilities, obtained by scanning the possible continuations of the chain in future steps (called future chains). We discuss in detail the efficiency of the method and for that we study certain autocorrelation functions for three lattice models: self-avoiding walks (SAWs) on a square lattice, a random walk model for polymer adsorption and trails with attractive interactions. We demonstrate that for SAWs the scanning method is significantly more efficient than the related method of Rosenbluth and Rosenbluth. We also develop and test a new procedure in which the transition probabilities are obtained, not by exact enumeration of all the future chains, but from a relatively small sample of future chains, generated by another scanning procedure. This "double scanning'' process is expected to be useful for complex macromolecules such as polypeptides.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 92 (1990), S. 1248-1257 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The double scanning method (DSM) is a computer simulation technique suggested recently by Meirovitch [J. Chem. Phys. 89, 2514 (1988)]. This method is a variant of the usual or "single'' scanning method (SSM) of the same author, which was extended by us to polypeptides [Biopolymers 27, 1189 (1988); this paper is designated here as paper II]. The two methods are step-by-step construction procedures from which the entropy and the free energy can be estimated. The transition probabilities are obtained by scanning the so-called "future'' chains, which are continuations of the chain in future steps up to a maximum of b steps. With the SSM, the process is carried out by exact enumeration of the future chains; this is time consuming, and therefore b is limited to small values. With the DSM, on the other hand, only a relatively small sample of the future chains is generated by applying an additional scanning procedure. This enables one to increase b at the expense of approximating the transition probabilities. Increasing of b, however, is important in order to treat medium- and long-range interactions more properly. In this paper (as in our paper II), we apply the DSM to a model of decaglycine without solvent, described by the potential energy function ECEPP at 100 and 300 K. Using the SSM with the maximal value, b=4, we found in paper II that, at 100 K, the α helix rather than the statistical coil is the most stable state. The present DSM simulation at T=100 K (based on b=5) is more efficient than the SSM, and a structure with significantly lower energy than that of the α helix is found. It is argued that b can be increased further to 7 at this temperature. At 300 K the DSM, like the SSM, shows that the statistical coil is the most stable state of decaglycine. However, the DSM is found to be less efficient than the SSM. It is argued, however, that the DSM is expected to be advantageous (even at 300 K) to simulate more complex polypeptides that are stable in small regions of phase space (such as the α-helical state). Finally, it should be pointed out that the present method can be employed to treat a wide range of macromolecular models, such as those for synthetic polymers and nucleic acids.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 88 (1988), S. 4498-4506 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: This paper is the first in a series of papers in which polymer adsorption on a surface is studied by computer simulation using the "scanning method.'' This method is especially efficient to handle chain systems with finite interactions and geometrical constraints. Here we test the method by applying it to models of a single random walk (without excluded volume) on a simple cubic lattice, which are solved analytically; in the immediately following paper a self-avoiding walk model is treated. The scanning method is found to be extremely efficient, where walks of up to N=105 steps can be simulated reliably, leading thereby to very precise estimates of transition temperatures and critical exponents. In particular we test carefully for a lattice model the range of validity of scaling functions developed by Eisenrigler, Kremer and Binder [J. Chem. Phys. 77, 6296 (1982)] for a continuous model. We pay a special attention to corrections to scaling and demonstrate that they are strong above the transition temperature for 〈R2〉⊥, the perpendicular part of the mean-square end-to-end distance and for ρ(z), the monomer concentration profile. We show that at T=∞, the asymptotic regime, in which these corrections become negligible, is obtained for N≈40 000 for 〈R2〉⊥ but a significantly larger N is required for ρ(z). This means that this regime corresponds to a real polymer length that is not realized experimentally.
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 88 (1988), S. 4507-4515 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The scanning simulation method is applied to a model of polymer adsorption in which a single self-avoiding walk is terminally attached to an attracting impenetrable surface on a simple cubic lattice. Relatively long chains are studied, of up to 1000 steps, which enable us to obtain new estimates for the reciprocal transition temperature ||ε||/kBTa=θa =0.291±0.001 (ε is the interaction energy of a monomer with the surface), the crossover exponent φ=0.530±0.007 and the free energy exponents at Ta, γ1SB =1.304±0.006 and γ11SB =0.805±0.015. At T=∞ we obtain, γ1=0.687±0.005, γ11=−0.38±0.02, and the effective coordination number q=4.6839±0.0001, which are in good agreement with estimates obtained by other methods. At T〉Ta we demonstrate the existence of strong correction to scaling for the perpendicular part of the mean-square end-to-end distance 〈R2〉⊥ and for the monomer concentration profile ρ(z) (z is the distance from the surface). At T=∞ the leading correction to scaling term for 〈R2〉⊥ is c/Nψ, where c≈−0.9 and ψ≈0.4 is close to 0.5 obtained for the random walk model in the preceding paper. This means that the asymptotic regime, in which these corrections become negligible, corresponds to a large polymer length that is not realized experimentally. Close enough to Ta we demonstrate for our lattice model the validity of various scaling forms predicted by Eisenriegler, Kremer, and Binder [J. Chem. Phys. 77, 6296 (1982)] for a continuum model on the basis of the n-vector model.
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  • 10
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 98 (1994), S. 6241-6243 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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