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

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5.2 Kinetic gas theory 107<br />

• Momentum change due to wall collision, force on wall, and pressure:<br />

=2 × 1 (5.79)<br />

6<br />

• Gas pressure:<br />

y<br />

= = 1 <br />

= 1 × 2 × 1 (5.80)<br />

6<br />

= 1 3 2 (5.81)<br />

• Result for 1mol ( = <br />

<br />

with =6022 1 × 10 23 mol −1 and kin = 2<br />

2 ):<br />

= 1 3 2 = 2 3 kin = 2 3 × 3 2 = (5.82)<br />

I<br />

Correct derivation of the gas kinetic wall collision frequency:<br />

• Number of molecules with velocities in a volume of with =<br />

p <br />

2 + 2 + 2 (cf. Fig. 5.7) that will hit the area in the time :<br />

( )=| | ( )<br />

<br />

<br />

( )<br />

<br />

( )<br />

<br />

(5.83)<br />

• To find the number of all molecules hitting in , we have to integrate over all<br />

positive and over all (positive and negative) and , using the 1D-Maxwell-<br />

Boltzmann distributions ( ) = ( )<br />

<br />

,etc.:<br />

µ 32 <br />

= <br />

×<br />

2 <br />

Z ∞ Z ∞ Z ∞ µ<br />

| | exp − 2 <br />

2 <br />

0 −∞ −∞<br />

µ µ <br />

exp − 2 <br />

exp − 2 <br />

<br />

2 2 <br />

(5.84)<br />

We know that the distributions over and are normalized to 1. Hence, we<br />

only have to solve the integral over , which we do by the substitution<br />

µ 12 µ 12 µ 12 <br />

<br />

2 <br />

=<br />

y =<br />

y =<br />

(5.85)<br />

2 <br />

2 <br />

<br />

y<br />

Z ∞<br />

0<br />

µ <br />

| | exp − 2 <br />

=<br />

2 <br />

Z ∞<br />

0<br />

= 2 <br />

<br />

µ 2 <br />

<br />

Z ∞<br />

0<br />

12<br />

|| −2 µ 2 <br />

<br />

−2 = 2 <br />

<br />

1<br />

2 = <br />

<br />

12<br />

(5.86)<br />

(5.87)

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