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CHEM 3411, Fall 2010<br />

<strong>Solution</strong> <strong>Set</strong> 8<br />

In this solution set, an underline is used to show the last significant digit of numbers. For instance in<br />

x = 2.51693<br />

the 2,5,1, and 6 are all significant. Digits to the right of the underlined digit, the 9 & 3 in the example, are not<br />

significant and would be rounded off at the end of calculations. Carrying these extra digits for intermediate values in<br />

calculations reduces rounding errors and ensures we get the same answer regardless of the order of arithmetic steps.<br />

Numbers without underlines (including final answers) are shown with the proper number of sig figs.<br />

1 Exercise 21.7b pg 826<br />

Given<br />

At T = 400 K, the rate of decomposition of a gaseous compound initially at a pressure of p 0 = 12.6 kPa, was<br />

v 1 = 9.71 Pa s −1 when 10.0 percent had reacted (extent of reaction ξ 1 = 0.100) and v 2 = 7.67 Pa s −1 when 20.0<br />

percent had reacted (ξ 2 = 0.200).<br />

In terms of given variables, this is written:<br />

T = 400 K<br />

p 0 = 12.6 kPa<br />

v 1 = 9.71 Pa s −1<br />

ξ 1 = 0.100<br />

v 2 = 7.67 Pa s −1<br />

ξ 2 = 0.200<br />

Find<br />

Determine the order of this reaction.<br />

Strategy<br />

In general, we know the rate of a reaction with a single reactant obeys an expression of the form<br />

v = dp<br />

dt = −kpn<br />

where p is the pressure of the reactants, n is the order of the reaction, and k is the rate constant.<br />

Additionally, we know the rate of the reaction at two different times (different reactant pressures) which gives us two<br />

the equations.<br />

1


CHEM 3411, Fall 2010<br />

<strong>Solution</strong> <strong>Set</strong> 8<br />

v 1 = −kp n 1<br />

v 2 = −kp n 2<br />

With some algebra we can solve for n from these two equations as we know v 1 , p 1 , v 2 , and p 2 .<br />

v 1<br />

p n 1<br />

= −k = v 2<br />

p n 2<br />

p n 2<br />

p n 1<br />

= v 2<br />

v 1<br />

(<br />

p2<br />

p 1<br />

) n<br />

= v 2<br />

v 1<br />

( ) ( )<br />

p2 v2<br />

n ln = ln<br />

p 1 v 1<br />

n =<br />

ln<br />

(<br />

v2<br />

v 1<br />

)<br />

ln<br />

(<br />

p2<br />

p 1<br />

)<br />

We can relates the pressures of the reactant, p 1 and p 2 , to the extent of reaction at each point in time, ξ 1 and ξ 2<br />

respectively. The extent of reaction ξ i at the i-th point in time is related to moles of reactant remaining n i and the<br />

initial moles of the reactant n 0 by<br />

n i = n 0 (1 − ξ i )<br />

From the ideal gas law we know that the moles of a gas and the pressure of the gas are proportional. This tells us<br />

the pressure of gas reactant p i at each i-th point in time is given by<br />

p i = p 0 (1 − ξ i )<br />

Substituting the expressions for p 1 and p 2 , p 1 = p 0 (1 − ξ 1 ) and p 2 = p 0 (1 − ξ 2 ) respectively, allows us to solve for<br />

the value of n.<br />

( )<br />

v<br />

ln 2<br />

v 1<br />

n = (<br />

ln<br />

p2<br />

ln<br />

=<br />

ln<br />

)<br />

p 1<br />

( )<br />

v 2<br />

v 1<br />

[<br />

p0 (1−ξ 2 )<br />

p 0 (1−ξ 1 )<br />

( )<br />

v<br />

ln 2<br />

v 1<br />

= [<br />

ln 1−ξ2<br />

ln<br />

= [<br />

ln<br />

= 2.0023<br />

]<br />

]<br />

1−ξ 1<br />

( )<br />

7.67✘✘✘<br />

Pa s<br />

9.71✘✘✘<br />

−1<br />

Pa s −1<br />

1−0.200<br />

1−0.100<br />

]<br />

2


CHEM 3411, Fall 2010<br />

<strong>Solution</strong> <strong>Set</strong> 8<br />

This tells us that within the uncertainty of the measurements n = 2.00, which is important as n should generally be<br />

an integer. With n = 2 the reaction kinetics are second order.<br />

<strong>Solution</strong><br />

Second order (n = 2.00)<br />

3


CHEM 3411, Fall 2010<br />

<strong>Solution</strong> <strong>Set</strong> 8<br />

2 Exercise 21.10b pg 826<br />

Given<br />

A second-order reaction of the type A + 2B → P was carried out in a solution that was initially 0.050 mol dm −3 in<br />

A and 0.030 mol dm −3 in B. After t = 1.0 h the concentration of B had fallen to 0.010 mol dm −3<br />

(In out textbook there is an error where the last sentence had A written in place of B.)<br />

In terms of given variables, this is written:<br />

[A] 0 = 0.050 mol dm −3<br />

[B] 0 = 0.030 mol dm −3<br />

[B] t=1.0 h = 0.010 mol dm −3<br />

Find<br />

• (a) Calculate the rate constant k r .<br />

• (b) What is the half-life of the reactants?<br />

Strategy<br />

For part (a) we can use the integrated rate law equation for a second order reaction of the form A + 2B → P as given<br />

in Table 21.3 (pg 295) of our textbook.<br />

k r × t =<br />

1<br />

[B] 0 − 2[A] 0<br />

ln [A] 0 ([B] 0 − x)<br />

([A] 0 − x) [B] 0<br />

where x is the extent of reaction (in concentration units) and thereby also the concentration of product P at time t.<br />

We know that at t = 1.0 h (t = 3600 s) the concentration of B is [B] = 0.010 mol dm −3 , which implies 0.020 mol dm −3<br />

of B have reacted at this point in time. The chemical equation for this reactions tells us that for each 2 mol of B<br />

that react, 1 mol of product will be formed. Hence, x = [P] = 0.010 mol dm −3 at this point in time (t = 3600 s).<br />

Using this value of x at time t = 3600 s we can solve for the rate constant k r .<br />

k r = 1 t<br />

1<br />

ln [A] 0 ([B] 0 − 2x)<br />

[B] 0 − 2[A] 0 ([A] 0 − x) [B] 0<br />

= 1<br />

3600 s × 1<br />

0.030 mol dm −3 − 2 × 0.050 mol dm −3 × ln 0.050 mol ( dm−3 0.030 mol dm −3 − 2 × 0.010 mol dm −3)<br />

(<br />

0.050 mol dm −3 − 0.010 mol dm −3) 0.030 mol dm −3<br />

= 0.003474 dm 3 mol −1 s−1<br />

In determining the half-lives of each reactant we will again use the integrated rate law equation from our textbook.<br />

For each reagent, we’ll determine the value of x (concentration of product [P]) at the point where half of the reactant<br />

is used up. We can then solve for the time t when the reaction reaches this value of x.<br />

For reactant A, the half-life concentration is [A] = 1 2 [A] 0 = 0.025 mol dm −3 and using the chemical equation for the<br />

reaction we find x = 0.025 mol dm −3 when [A] reaches this half-life concentration.<br />

4


CHEM 3411, Fall 2010<br />

<strong>Solution</strong> <strong>Set</strong> 8<br />

Solving for the time t when this value of x is reached<br />

t 1/2 A = 1 1<br />

ln [A] 0 ([B] 0 − 2x)<br />

k r [B] 0 − 2[A] 0 ([A] 0 − x) [B] 0<br />

1<br />

=<br />

0.003474 s dm 3 mol −1 × 1<br />

0.030 mol dm −3 − 2 × 0.050 mol dm −3 ×<br />

ln 0.050 mol dm−3 ( 0.030 mol dm −3 − 2 × 0.025 mol dm −3)<br />

(<br />

0.050 mol dm −3 − 0.025 mol dm −3) 0.030 mol dm −3<br />

=D.N.E.<br />

Here we find an answer does not exist (D.N.E.) due to a negative value in the natural logarithm. On further inspection<br />

we find this lack of solution results from insufficient initial concentration of B for this amount of product P to be<br />

formed. Therefore the reaction never proceeds far enough for half of the initial concentration of A to be consumed.<br />

This explains why t 1/2 A does not exist.<br />

Repeating this process for B we find x = 0.0075 mol dm −3 when the concentration of B reaches its half-life value<br />

[B] = 1 2 [B] 0 = 0.015 mol dm −3 .<br />

t 1/2 B = 1 1<br />

ln [A] 0 ([B] 0 − 2x)<br />

k r [B] 0 − 2[A] 0 ([A] 0 − x) [B] 0<br />

1<br />

=<br />

0.003474 s dm 3 mol −1 × 1<br />

0.030 mol dm −3 − 2 × 0.050 mol dm −3<br />

× ln 0.050 mol dm−3 ( 0.030 mol dm −3 − 2 × 0.0075 mol dm −3)<br />

(<br />

0.050 mol dm −3 − 0.0075 mol dm −3) 0.030 mol dm −3<br />

=2181 s<br />

<strong>Solution</strong><br />

k r = 3.5 × 10 −3 dm 3 mol −1 s −1<br />

t 1/2 A = D.N.E.<br />

t 1/2 B = 2.2 × 10 3 s = 0.61 h<br />

5


CHEM 3411, Fall 2010<br />

<strong>Solution</strong> <strong>Set</strong> 8<br />

3 Exercise 21.13b pg 827<br />

Given<br />

The equilibrium A ⇋ B+C at T = 25 ◦ C is subjected to a temperature jump that slightly increases the concentrations<br />

of B and C. The measured relaxation time is τ = 3.0 µs. The equilibrium constant for the system is K = 2.0×10 −16 at<br />

T = 25 ◦ C, and the equilibrium concentration of B and C at T = 25 ◦ C are both [B] eq<br />

= [C] eq<br />

= 2.0 × 10 −4 mol dm −3 .<br />

In terms of given equations and variables, this is written:<br />

A ⇋ B + C<br />

T = 25 ◦ C<br />

τ = 3.0 µs = 3.0 × 10 −6 s<br />

K = 2.0 × 10 −16 mol dm −3<br />

[B] eq<br />

= [C] eq<br />

= 2.0 × 10 −4 mol dm −3<br />

Find<br />

Calculate the rate constants for the forward and reverse steps, k r and k ′ r respectively.<br />

Strategy<br />

In solving this problem we’ll follow a strategy similar to that of Example 21.4 (pg 798) of our textbook. We’ll<br />

begin by constructing the following equation for the rate of change of reactant A in terms of reactant and products<br />

concentrations.<br />

d [A]<br />

dt<br />

= −k r [A] + k ′ r [B] [C]<br />

Next, we’ll relates the instantaneous concentration of reactant and products to their equilibrium concentrations and<br />

the instantaneous deviation from equilibrium x.<br />

[A] = [A] eq<br />

+ x<br />

[B] = [B] eq<br />

− x<br />

[C] = [C] eq<br />

− x<br />

Substituting these expressions into our reaction rate equation gives the following.<br />

6


CHEM 3411, Fall 2010<br />

<strong>Solution</strong> <strong>Set</strong> 8<br />

d [A]<br />

= −k r [A] + k r ′ [B] [C]<br />

(<br />

dt<br />

)<br />

d [A] eq<br />

+ x<br />

) (<br />

= −k r<br />

([A]<br />

dt<br />

eq<br />

+ x + k r<br />

′<br />

dx<br />

(<br />

)<br />

dt = −k r [A] eq<br />

+ k r ′ [B] eq<br />

[C] eq<br />

+ x<br />

) ( )<br />

[B] eq<br />

− x [C] eq<br />

− x<br />

[<br />

−k r − k r<br />

′<br />

([B] eq<br />

+ [C] eq<br />

)]<br />

− k ′ rx 2<br />

The first right-hand term in parentheses can be set to zero by the condition that forward and backwards rates are<br />

equal at equilibrium.<br />

k r [A] eq<br />

= k ′ r [B] eq<br />

[C] eq<br />

−k r [A] eq<br />

+ k ′ r [B] eq<br />

[C] eq<br />

= 0<br />

Additionally, the k ′ rx 2 term can be neglected by assuming deviations from equilibrium are small enough to make x 2<br />

negligible relative to x. Therefore our expression for dx/dt simplifies to.<br />

dx<br />

[<br />

)]<br />

dt = x −k r − k r<br />

([B] ′ eq<br />

+ [C] eq<br />

This is simply the rate-equation for a first-order reaction and therefore the solution of this differential equation takes<br />

the form<br />

where the relaxation time-constant τ is given by<br />

x(t) = x 0 e −t/τ<br />

1<br />

)<br />

τ = k r + k r<br />

([B] ′ eq<br />

+ [C] eq<br />

As we know τ, [B] eq<br />

[C] eq<br />

we can solve for k r and k ′ r if we have one more equation with only these two terms as<br />

unknowns. Such an equation is found from the relationship of equilibrium constant K and forward reverse rates, k r<br />

and k ′ r respectively (Equation 21.27 pg 797)<br />

K = k r<br />

k ′ r<br />

Solving for k ′ r = k r<br />

K and substituting into our time-constant equation allows us to solve for k r.<br />

1<br />

τ = k r + k )<br />

r<br />

([B]<br />

K eq<br />

+ [C] eq<br />

k r =<br />

τ<br />

[<br />

1 + 1 K<br />

1<br />

)]<br />

([B] eq<br />

+ [C] eq<br />

1<br />

=<br />

[<br />

(<br />

3.0 × 10 −6 1<br />

s 1 +<br />

2.0×10 −16 mol dm 2.0 × 10<br />

−4<br />

mol dm −3 + 2.0 × 10 −4 mol dm −3)]<br />

−3<br />

= 1.667 × 10 −7 s −1 7


CHEM 3411, Fall 2010<br />

<strong>Solution</strong> <strong>Set</strong> 8<br />

Lastly, we’ll solve for k ′ r.<br />

k ′ r = k r<br />

K<br />

= 1.667 × 10−7 s −1<br />

2.0 × 10 −16 mol dm −3<br />

= 8.335 × 10 8 dm 3 mol −1 s −1<br />

<strong>Solution</strong><br />

k r = 1.7 × 10 −7 s −1<br />

k ′ r = 8.3 × 10 8 dm 3 mol −1 s −1 8


CHEM 3411, Fall 2010<br />

<strong>Solution</strong> <strong>Set</strong> 8<br />

4 Exercise 21.18b pg 827<br />

Given<br />

The mechanism of a composite reaction consists of a fast pre-equilibrium step with forward and reverse activation<br />

energies of E a (a) = 27 kJ mol −1 and E ′ a(a) = 35 kJ mol −1 , respectively, followed by an elementary step of activation<br />

energy E a (b) = 15 kJ mol −1 .<br />

In terms of given variables, this is written:<br />

E a (a) = 27 kJ mol −1<br />

E ′ a(a) = 35 kJ mol −1<br />

E a (b) = 15 kJ mol −1<br />

Find<br />

What is the activation energy of the composite reaction?<br />

Strategy<br />

Our textbook has discussed the kinetics of a such a reaction in Section 21.8 (pgs 809-811). The following expression<br />

was developed for the activation energy of the composite reaction.<br />

E a = E a (a) + E a (b) − E ′ a(a)<br />

= 27 kJ mol −1 + 15 kJ mol −1 − 35 kJ mol −1<br />

= 7 kJ mol −1<br />

<strong>Solution</strong><br />

E a = 7 kJ mol −1 9


CHEM 3411, Fall 2010<br />

<strong>Solution</strong> <strong>Set</strong> 8<br />

5 Exercise 22.4b pg 872<br />

Given<br />

Consider the second-order reaction D 2 (g) + Br 2 (g) → 2DBr(g) at T = 450 K which is assumed to be elementary<br />

bimolecular. Further, take the collision cross-section as 0.30 nm 2 , the reduced mass as 3.930m u , and the activation<br />

energy as 200 kJ mol −1 .<br />

In terms of given equations and variables, this is written:<br />

D 2 (g) + Br 2 (g) → 2DBr(g)<br />

T = 450 K<br />

σ = 0.30 nm 2 = 0.30 × 10 −18 m 2<br />

µ = 3.930m u = 6.52592 × 10 −27 kg<br />

E a = 200 kJ mol −1<br />

Find<br />

Use the collision theory of gas-phase-reactions to calculate the theoretical value of the second-order rate constant for<br />

this reaction.<br />

Strategy<br />

We know the rate of a gas-phase bimolecular elementary (excluding steric requirements) is described by the following<br />

equation (Equation 22.12 pg 835)<br />

k r = N A σ¯c rel e −E a/RT<br />

Additionally, we know the average relative speed ¯c rel can be calculated from the Maxwell distribution. In Justification<br />

22.3 of our textbook this was calculated and this gives us a rate expression into which we can insert the given<br />

parameters of this reaction.<br />

( ) 1/2 8kT<br />

k r = N A σ<br />

e −Ea/RT<br />

πµ<br />

= 6.02214 × 10 23 mol −1 × 0.30 × 10 −18 m 2 ×<br />

( 8 × 1.38065 × 10 −23 J K −1 ) 1/2<br />

× 450 K<br />

3.1415 × 6.52592 × 10 −27 ×<br />

kg<br />

exp [ −200 × 10 3 J mol −1 / ( 8.31447 J K −1 mol −1 × 450 K )]<br />

= 1.715 × 10 −15 m 3 mol −1 s −1<br />

= 1.715 × 10 −12 dm 3 mol −1 s −1 10


CHEM 3411, Fall 2010<br />

<strong>Solution</strong> <strong>Set</strong> 8<br />

<strong>Solution</strong><br />

k r = 1.7 × 10 −12 dm 3 mol −1 s −1 11


CHEM 3411, Fall 2010<br />

<strong>Solution</strong> <strong>Set</strong> 8<br />

6 Exercise 22.6b pg 872<br />

Given<br />

Suppose that the typical diffusion coefficient for a reactant in aqueous solution at T = 25 ◦ C is D = 4.2×10 −9 m 2 s −1 .<br />

Further assume the critical reaction distance is R ∗ = 0.50 nm for the second-order diffusion controlled reaction with<br />

this reactant.<br />

In terms of given variables, this is written:<br />

T = 25 ◦ C<br />

D = 4.2 × 10 −9 m 2 s −1<br />

R ∗ = 0.50 nm = 5.0 × 10 −10<br />

Find<br />

The rate constant for this reaction.<br />

Strategy<br />

The rate constant of a diffusion-controlled reaction is given by Equation 22.18 (pg 840) from our textbook.<br />

k d = 4πR ∗ DN A<br />

= 4 × 3.1415 × 5.0 × 10 −10 m × 4.2 × 10 −9 m 2 s −1 × 6.02214 × 10 23 mol −1<br />

= 1.58915 × 10 7 m 3 mol −1 s −1<br />

= 1.58915 × 10 10 dm 3 mol −1 s −1<br />

<strong>Solution</strong><br />

k d = 1.6 × 10 10 dm 3 mol −1 s −1 12

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