| 25E3b | The dimensions of k are
dim of R / { (dim of [A])×(dim of [B])2 } = { amount × length-3 × time-1 } / { amount×length-3 }3 = length6 × amount-2 × time-1 In mol, L, s units, the units of k are L2 mol-2 s-1
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| 25E5b | The rate law is
R = kpa = kp0a(1-f)a where a is the reaction order and f the fraction reacted (so that 1-f is the fraction remaining). Thus, R1/R2 = kp0a(1-f1)a / [ kp0a(1-f2)a ] = [(1-f1) / (1-f2)]a and a = ln(v1 / v2) / ln[(1-f1) / (1-f2)] = ln(9.71 / 7.67) / ln[(1-0.100) / (1-0.200)] = 2.00 |
| 25E8b | From Table 25.3, we see that for
kt = { 1 / ( [B]0 - 2[A]0 ) } × ln[ { [A]0×([B]0 - 2x) } / { ([A]0 - x)×[B]0 } ]
k = { 1 / [(3.6×103 s)×(0.080 - 2×0.075)×(mol/L)] } × ln{ [0.075×(0.080 - 0.060)] / [(0.075 - 0.030)×0.080] } = 3.47×10-3 L mol-1 s-1 t½ = { 1 / [k([B]0 - 2[A]0)] } × ln ( { [A]0×([B]0 - 2×½[A]0) } / { ½[A]0[B]0 } ) which reduces to t½ = { 1 / [ k([B]0 - 2[A]0) ] } × ln(2 - 2[A]0/[B]0) = { 1 / [(3.47×10-3 L/mol s-1)×(-0.070 mol/L)] } × ln[ 2 - (0.150/0.080)] = 8561 s = 2.4 hours
The half-life in terms of B is
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| 25E13b |
The rate constant is given by
k = A e-Ea/RT so at 50°C, it is 1.70×10-2 L/mol s-1 = A e-Ea / {(8.3145 J/mol K-1)×([24+273] K)} and at 50°C, it is 2.01×10-2 L/mol s-1 = A e-Ea / {(8.3145 J/mol K-1)×([37+273] K)} Dividing the two rate constants yields (1.70×10-2)/(2.01×10-2) = e[-Ea/8.3145 J/mol K-1]×[(1/297 K) - (1/310 K)] } so ln(1.70/2.01) = [-Ea/8.3145 J/mol K-1]×[(1/297 K) - (1/310 K)] and Ea = - (8.3145 J/mol K-1) × [(1/297 K) - (1/310 K)]-1 × ln(1.70/2.01) = 9.9×103 J/mol = 9.9 kJ/mol
With the activation energy in hand, the prefactor can be computed
from either rate constant value
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| 25E17b |
The effective rate constant is related to the individual steps by
1/k = [ka'/(kakb)] + 1/[kap] so (1/k1) - (1/k2) = (1/ka)[(1/p1) - (1/p2) ka = [(1/p1) - (1/p2)]×[(1/k1) - (1/k2)]-1 = [(1/1.09×103 Pa) - (1/25 Pa)] × [(1/1.7×10-3 s-1) - (1/2.2×10-4 s-1)]-1 = 9.9×10-6 s-1 Pa-1 |
| 25P4 |
An examination of the data shows that the half-life remains constant
at about 2 minutes. Therefore, the reaction is first-order.
This can be confirmed by fitting any two pairs of data to the
integrated first-order rate law, solving for k from each pair,
and checking to see that they are the same to within experimental error.
ln([A]/[A]0) = - kt (10b, A=N2O5)
Values of k may be determined in a similar manner at all other times. The average value of k obtained is 5.48×10-3 s-1. The constancy of k, which varies only between 5.83 and 5.85×10-3 s-1, confirms that the reaction is first-order. A linear regression of ln[A] against t yields the same result. |
| 25P22 |
kt = [ 1 / (n-1) ]×[ (1/[A]n-1) - (1/[A]0n-1) ] (Ex. 25.15a, n<>1)
at t=t½, kt½ = [1/(n-1)]×[(2/[A]0)n-1 - (1/[A]0)n-1] at t=t¾, kt¾ = [1/(n-1)]×[(4/3[A]0)n-1 - (1/[A]0)n-1] Hence t½/t¾ = [ 2n-1 - 1 ] / [ (4/3)n-1 - 1 ] |
| 25P31 |
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