Advances in Chemical Physics, Volume 3 - download pdf or read online

By Stuart A. Rice, Aaron R. Dinner

ISBN-10: 0470143495

ISBN-13: 9780470143490

ISBN-10: 0470698284

ISBN-13: 9780470698280

The Advances in Chemical Physics sequence offers the chemical physics and actual chemistry fields with a discussion board for serious, authoritative reviews of advances in each sector of the self-discipline. full of state of the art study pronounced in a cohesive demeanour no longer came upon somewhere else within the literature, each one quantity of the Advances in Chemical Physics sequence serves because the ideal complement to any complicated graduate classification dedicated to the research of chemical physics.


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Extra resources for Advances in Chemical Physics, Volume 3

Example text

The quantity R i is what we should coinpare with D1-l(z). Since we saw in the calculations for diffusion th a t D,(c) does not occur a t all in the final integral in the variational principle, we shall now consider a system of chemical reactions with arbitrary reaction order. For tht' flux we may write J . == 70. ,i+~ - ~ z 1 . ~1L I , i + where, as above, J i is the flux from species i to species i 1, the m i j ' s are transition probabilities (or rate constants), ci concentration and ql,i the power to which the concentration is raised in the kinetic equation.

A. Equations of Change . . . . . . . . . B. One-Dimensional Time-Dependent Equations . . . C. One-Dimensional Steady-State Equations . . . . D . Boundary Conditions . . . . . . . . . 60 60 63 65 66 I11. Flames Produced by an Exothermic Unimolecular Reaction . A. The Flame Equations . . . . . . . . B. Ignition Temperature Model . . . . . . . C. Arrhenius Kinetics . . . . . . . . . D . The Effect of the Kinetic Energy Terms . . . . E . Approximate Solutions .

Z)2 - (d/dX)2 ( D / c )(dclds) = 0 or - (2/c) ( d / d x ) D ( x(dcldx) ) + D [ ( l / R T()2 p j 2 x ) l =~ 0 (27) In order that this be the equation for timeindependent diffusion, viz. ( d / d x ) [ D ( x ) ( d c / d x ) ]= 0 (23) we must have 2,u/dx = 0, that is, the diffusion process must have reached equilibrium. For systems in which the time-independent state is not an equilibrium state (or very close to equilibrium) this variational principle cannot be used. However, Prigogine15showed that when 42 THOR A .

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Advances in Chemical Physics, Volume 3 by Stuart A. Rice, Aaron R. Dinner

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