1.1 高分子的基本概念 1.2 高分子化合物的基本特征 1.4 高分子化合物的命名和分类 1.5 聚合反应
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Approaches to Asymmetric Catalysis Organometallic catalysis Broad scope Ligand control Inert conditions -Cost and toxicity Bioorganic catalysis Highly selective High rate of reaction Limited scope
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How to analyse the errors of simulation results? Sustematic errors: Possible sources. 'poor equilibration; bad random number generator; 'system size effect. Practical method for detecting systematic errors: -longer simulation, different initial configurations; test random number generator, use different generators; simulation with larger systems
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Application of MR2T2 algorithm in statistical mechanics Canonical ensemble: Distribution function: p(rN)=exp(-E(rN)/KT)/Q Q= JdrN exp(-E(rN)/kT) Different states of the Markov chain: In the application of Metropolis algorithm to a simulation of molecular system, the states of the Markov chain correspond to different configurations of the molecular system
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Monte Carlo Integration Hit and miss method:Algorithm: ( 1) generate N uniform random numbers, (i=1, 2,..., N), on(a,b) and N uniform random numbers, (i=1, 2,..., N), on (0,c); (2) calculate g() and count the number of cases, Nhit for whichg() (3)I can be estimated by
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What is a Monte Carlo simulation? Monte Carlo simulation is numerical method based on the extensive use of random numbers for solving different problems. Remark: Monte Carlo simulation can be used tostudy not only stochastic problems (e.g., diffusion) but also non stochastic ones (Monte Carlo
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Molecular dynamics for continuous potentials Short history: The first MD simulation for a system interacting with a continuous potential (Lennard-Jones potential) was carried out by A. Rahman in1964. A. Rahman, Phys. Rev. 136, A405, (1964). Main differences between MD with continuous poentials and
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How to start up? Initial configuration: Criteria for choosing initial configuration: quick relaxation to the equilibrium state. Random initial configuration: Advantage: liquid-like, easy to generate. Drawback: substantial overlaps at high densities. Use: Monte-Carlo for systems without hard-core interactions. Not suitable for hard-core interactions and MD at high densities
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Necessary Background of Statistical Physics (2) when the velocity of the center of mass is fixed to zeroKinetic energy
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Why one needs statistics for describing physical phenomena? Any measurable macroscopic property is an average over a very huge number of microscopic configurations. Time scale of thermal fluctuations and basic relaxations~fs(femto second, 10-15 second). During the time interval necessary for realizing a measurement, a macroscopic system undergoes the change of its microscopic configuration for many many times!
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