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Physical Chemistry 3: — Chemical Kinetics — - Christian-Albrechts ...

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7.3 Thermodynamic interpretation of transition state theory 163<br />

• Note: and are given above in units of lmol −1 s −1 (we may denote this by<br />

writing them as and ), while ∆ ª‡ and ∆ ª‡ used above are referred to<br />

the standard state for gases of ª =1bar.<br />

<strong>—</strong> For ideal gases, ∆ ‡ and ∆ ‡ are related via<br />

∆ ª‡ = ∆ ª‡ + ∆ ‡ ( )=∆ ª‡ − = ∆ +‡ − (7.87)<br />

<strong>—</strong> Likewise, ∆ ª‡ and ∆ +‡ for are related via<br />

∆ +‡ − ∆ ª‡ =<br />

y<br />

Z <br />

+<br />

ª<br />

Z<br />

<br />

+<br />

=<br />

ª<br />

<br />

= Z <br />

+<br />

ª<br />

<br />

= Z <br />

+<br />

ª<br />

∆ ‡ <br />

(7.88)<br />

<br />

= ∆ ‡ +<br />

ln<br />

+ 0 = +<br />

ª ∆‡ ln<br />

+ 0 = ª<br />

ª ∆‡ ln (7.89)<br />

+ 0 <br />

= ∆ ‡ ln + 0 <br />

(7.90)<br />

ª<br />

with ª =1barand + = +<br />

+ =1moll−1 .<br />

∆ ª‡ = ∆ +‡ − ln + 0 <br />

ª (7.91)<br />

c) Thermodynamic transition state theory for reactions in the liquid phase<br />

For reactions in condensed phases,<br />

∆ ≈ ∆ (7.92)<br />

and<br />

y<br />

£<br />

ABC<br />

‡ ¤<br />

‡ ( ) =<br />

[A] [BC] = ¡ +¢ ∆ ‡ exp<br />

≈ ¡ +¢ <br />

∆ ‡ exp<br />

µ− ∆+‡<br />

exp<br />

<br />

• for unimolecular reactions:<br />

( )= µ<br />

<br />

exp<br />

• for bimolecular reactions:<br />

( )= µ<br />

<br />

+ exp<br />

− ∆+‡<br />

µ− ∆+‡<br />

<br />

− ∆+‡<br />

<br />

<br />

<br />

µ− ∆+‡<br />

<br />

exp<br />

<br />

exp<br />

<br />

<br />

+‡<br />

∆<br />

exp<br />

µ−<br />

<br />

<br />

µ− ∆+‡<br />

<br />

µ− ∆+‡<br />

<br />

<br />

<br />

(7.93)<br />

(7.94)<br />

(7.95)<br />

(7.96)<br />

Note: The conversion between values for ∆ +‡ and ∆ ª‡ and, likewise, between<br />

values for ∆ +‡ and ∆ ª‡ for a given reaction in the liquid and gas phase requires<br />

some caution. 46<br />

46 See,e.g.,D.M.Golden,J.Chem.Ed.48, 235 (1971).

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