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Unformatted text preview: MIT OpenCourseWare http://ocw.mit.edu 5.72 Statistical Mechanics Spring 2008 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms . Chapter 1 Stochastic Processes and Brownian Motion Equilibrium thermodynamics and statistical mechanics are widely considered to be core subject matter for any practicing chemist [1]. There are plenty of reasons for this: A great many chemical phenomena encountered in the laboratory are well described by equi librium thermodynamics. The physics of chemical systems at equilibrium is generally well understood and mathemati cally tractable. Equilibrium thermodynamics motivates our thinking and understanding about chemistry away from equilibrium. This last point, however, raises a serious question: how well does equilibrium thermodynamics really motivate our understanding of nonequilibrium phenomena? Is it reasonable for an organometallic chemist to analyze a catalytic cycle in terms of ratelaw kinetics, or for a biochemist to treat the concentration of a solute in an organelle as a bulk mixture of compounds? Under many circum stances, equilibrium thermodynamics suces, but a growing number of outstanding problems in chemistry from electron transfer in lightharvesting complexes to the chemical mechanisms behind immune system response concern processes that are fundamentally out of equilibrium. This course endeavors to introduce the key ideas that have been developed over the last century to describe nonequilibrium phenomena. These ideas are almost invariably founded upon a statistical description of matter, as in the equilibrium case. However, since nonequilibrium phenomena con tain a more explicit timedependence than their equilibrium counterparts (consider, for example, the decay of an NMR signal or the progress of a reaction), the probabilistic tools we develop will require some timedependence as well. In this chapter, we consider systems whose behavior is inherently nondeterministic, or stochas tic , and we establish methods for describing the probability of finding the system in a particular state at a specified time. 1 2 Chapter 1. Stochastic Processes and Brownian Motion 1.1 Markov Processes 1.1.1 Probability Distributions and Transitions Suppose that an arbitrary system of interest can be in any one of N distinct states. The system could be a protein exploring different conformational states; or a pair of molecules oscillating be tween a reactants state and a products state; or any system that can sample different states over time. Note here that N is finite, that is, the available states are discretized. In general, we could consider systems with a continuous set of available states (and we will do so in section 1.3), but for now we will confine ourselves to the case of a finite number of available states. In keeping with our discretization scheme, we will also (again, for now) consider the time evolution of the system in terms of discrete timesteps rather than a continuous time variable. system in terms of discrete timesteps rather than a continuous time variable....
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 Spring '04
 RobertField
 Equilibrium

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