SAMPLE FINAL EXAM - SOLUTION Statistical Mechanics and

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SAMPLE FINAL EXAM - SOLUTION

Statistical Mechanics and Chemical Dynamics (Chem 130C)

(Dated: Jun 2, 2008)

1. A first-order rxn, A → P, goes only forward, with a rate constant of 10 s

− 1 . How long before

90% of A has turned into P? How would your answer change if there were a back rxn at rate 2 s

− 1

? Hint: In the second part, an equilibrium is established.

If the reaction goes only forward:

[ A ] = 0 .

1[ A ]

0

= [ A ]

0 e

− kt

; t = 0 .

23 s .

If there is a backward reaction:

K = k

1 k

− 1

=

[ P ]

[ A ]

= 5;

[ A ] eq

=

1

6

[ A ]

0

= 0 .

17[ A ]

0

.

So A never gets 10% of the original concentration.

2. For a first-order reaction, the activation barrier is calculated to be 100 kJ/mol, and 10% of the reactant vanishes in 20 minutes when performed in an ice bucket. How much would have been gone if it had been done at room temp (20 o C)? Hint: Arrhenius.

I use subscript 1 to denote room temperature and 2 for ice bucket.

1

293

1

273

!

= 20 .

23;

For first-order reaction: k

1 k

2

= exp −

100 × 10 3

8 .

314

[ A ] ln

[ A ]

0

= − kt ;

At ice bucket, the left hand side is ln 0 .

9 , so we know k

2

= 0 .

00527 min

− 1 temprature, k

1

= 20 .

23 k

2

= 0 .

107 min

− 1

, and for room

, plug in the above equation, we know [ A ] = 0 .

118[ A ]

0

, which means that 88 .

2% have been gone.

3. A rxn has the following simple mechanism: A → B + C, B → A, A+C → P, with rate constants k, k

0

, k

2 respectively. Use the steady-state approximation to show that this is first-order in [A], and find the effective rate constant for the rate of consumption of A. What conditions must the k ’s satisfy to make your answer accurate?

Use steady state approximation on B and C: d [ B ]

= k [ A ] − k

0

[ B ] = 0; dt d [ C ]

= k [ A ] − k

2

[ A ][ C ] = 0; dt

2

And we can solve for [B] and [C]:

[ B ] = k [ A ]

; k 0

Plug in the differential rate law for [A]:

[ C ] = k k

2

; d [ A ]

= − k [ A ] + k

0

[ B ] − k

2

[ A ][ C ] = − k [ A ] .

dt

This means that the effective rate constant is k . The steady state approximation is more accurate when the consumption rate is much greater than the formation rate, which means that k

0 k and k

2 k .

4. The reversible rxn A → P has rate constants 0.1 min

− 1 forward and 0.033 min

− 1 backwards. If

I start with 0.1 moles of A, what will be in my tank after an hour? Hint: This can be thought of as relaxing toward equilibrium.

I use k

1 to denote the rate constant for forward reaction, and k

2 for backward reaction.

d [ A ]

= − k

1

[ A ] + k

2

[ P ] = − k

1

[ A ] + k

2

([ A ]

0

− [ A ]); dt where the second equal sign used mass conservation. And we can do the integration: d [ A ]

( k

1

+ k

2

)[ A ] − k

2

[ A ]

0

= − ( k

1

+ k

2

) dt ;

( k

1 ln

( k

1

+ k

2

)[ A ] − k

+ k

2

)[ A ]

0

− k

2

2

[ A ]

0

[ A ]

0

= − ( k

1

+ k

2

) t ;

We plug in [ A ]

0

= 0 .

1 mol, and we get [ A ] = 0 .

0248 mol. (volume is the same)

Note: you can also use equilibrium as your reference point (and use an x to denote the deviation from equilibrium concentration), just as what we did in class.

5. I have 10 moles of Argon in 1 liter at room temperature, and I suddenly double the volume.

How is the mean velocity after the change related to that before? Repeat for, the collision frequency and the mean free path.

T does not change, so kinetic energy does not change, hence mean speed does not change.

λ = √ kT

2 σp

= kV

2 σnR

=

¯

; z

So we know as V is doubled, the mean free path becomes twice the original value; and the collision frequency decreases to half the original value (because ¯ does not change).

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