The order is the sum of powers of concentration terms in the rate law. For an nth order reaction, units of k are (mol L^-1)^(1-n) s^-1. Applying this gives the stated orders and dimensions.
(i) second order, k: L mol^-1 s^-1; (ii) second order, k: L mol^-1 s^-1; (iii) order 3/2, k: L^1/2 mol^-1/2 s^-1; (iv) first order, k: s^-1.
Initial rate = (2.0 x 10^-6)(0.1)(0.2)^2 = 8.0 x 10^-9 mol L^-1 s^-1. From 2A + B → A2B, when [A] falls by 0.04 M, [B] falls by 0.02 M, so [B] = 0.18 M. New rate = (2.0 x 10^-6)(0.06)(0.18)^2 = 3.89 x 10^-9 mol L^-1 s^-1.
Initial rate = 8.0 x 10^-9 mol L^-1 s^-1; later rate = 3.89 x 10^-9 mol L^-1 s^-1.
When pressure is used instead of concentration, rate has units of pressure per time, i.e. bar min^-1. Since rate = k p^3/2, k has units (bar min^-1)/(bar^3/2) = bar^-1/2 min^-1.
Rate: bar min^-1; k: bar^-1/2 min^-1.
Reaction rate depends on the number and effectiveness of collisions. Increasing concentration or gas pressure usually increases collision frequency. Higher temperature increases the fraction of molecules with sufficient energy. Catalysts lower activation energy. Nature and physical state of reactants, including surface area for solids, also matter.
Concentration, temperature, pressure for gases, catalyst, nature of reactants and surface area affect reaction rate.
For second order dependence on a reactant, rate is proportional to [A]^2. Doubling [A] multiplies rate by 2^2 = 4. Reducing [A] to half multiplies rate by (1/2)^2 = 1/4.
(i) Rate becomes four times. (ii) Rate becomes one-fourth.
For many reactions, the rate constant approximately doubles for a 10 K rise in temperature near room temperature. Quantitatively, k = A e^(-Ea/RT), where A is the pre-exponential factor, Ea is activation energy, R is the gas constant and T is absolute temperature. A plot of ln k against 1/T is linear with slope -Ea/R.
The rate constant generally increases with temperature and is represented by the Arrhenius equation.
Average rate of disappearance of A between 30 s and 60 s = -Δ[A]/Δt = -(0.17 - 0.31)/(60 - 30) = 0.14/30 = 4.67 x 10^-3 mol L^-1 s^-1.
4.67 x 10^-3 mol L^-1 s^-1.
First order in A and second order in B gives rate = k[A][B]^2. Tripling B multiplies the rate by 3^2 = 9. Doubling both A and B multiplies the rate by 2 x 2^2 = 8.
(i) Rate = k[A][B]^2. (ii) Rate becomes 9 times. (iii) Rate becomes 8 times.
In experiments 1 and 2, [A] is constant while [B] changes from 0.30 to 0.10, but the rate is unchanged. Therefore order in B is zero. Comparing experiments 2 and 3, B does not matter, [A] doubles from 0.20 to 0.40 and rate changes by 1.43 x 10^-4/(5.07 x 10^-5) = 2.82. Thus 2^x = 2.82, giving x ≈ 1.5.
Order with respect to A = 1.5; order with respect to B = 0.
Comparing I and IV, [B] is constant, [A] increases 4 times and rate increases 4 times, so order in A is 1. Comparing II and III, [A] is constant, [B] doubles and rate becomes 4 times, so order in B is 2. Thus rate = k[A][B]^2. Using experiment I, k = 6.0 x 10^-3/(0.1 x 0.1^2) = 6.0 L^2 mol^-2 min^-1.
Rate = k[A][B]^2; k = 6.0 L^2 mol^-2 min^-1.
Since the reaction is first order in A and zero order in B, rate = k[A]. From experiment I, k = (2.0 x 10^-2)/0.1 = 0.20 min^-1. For experiment II, [A] = rate/k = (4.0 x 10^-2)/0.20 = 0.2 M. For III, rate = 0.20 x 0.4 = 8.0 x 10^-2. For IV, [A] = (2.0 x 10^-2)/0.20 = 0.1 M.
Experiment II [A] = 0.2 mol L^-1; Experiment III rate = 8.0 x 10^-2 mol L^-1 min^-1; Experiment IV [A] = 0.1 mol L^-1.
For a first order reaction, t1/2 = 0.693/k. Therefore (i) t1/2 = 0.693/200 = 3.47 x 10^-3 s; (ii) t1/2 = 0.693/2 = 0.347 min; (iii) t1/2 = 0.693/4 = 0.173 year.
(i) 3.47 x 10^-3 s; (ii) 0.347 min; (iii) 0.173 year.
Radioactive decay is first order. k = 0.693/5730 year^-1. With N/N0 = 0.80, t = (2.303/k)log(N0/N) = (5730/0.693)ln(1/0.80) = 1.85 x 10^3 years.
About 1.85 x 10^3 years.
For first order reaction, t = (2.303/k)log([A]0/[A]). Here [A] = [A]0/16, so t = (2.303/60)log16 = 4.62 x 10^-2 s.
4.62 x 10^-2 s.
For first order radioactive decay, N = N0(1/2)^(t/t1/2). With N0 = 1 mg and t1/2 = 28.1 years, after 10 years N = (1/2)^(10/28.1) = 0.781 mg. After 60 years N = (1/2)^(60/28.1) = 0.228 mg.
After 10 years: 0.781 mg; after 60 years: 0.228 mg.
For a first order reaction, t = (2.303/k)log(a/(a - x)). For 90% completion, t90 = (2.303/k)log(100/10) = 2.303/k. For 99% completion, t99 = (2.303/k)log(100/1) = 2(2.303/k). Hence t99 = 2t90.
t99% = 2 t90%.
For 30% decomposition, 70% remains. k = (2.303/40)log(100/70) = 8.92 x 10^-3 min^-1. Therefore t1/2 = 0.693/k = 77.7 min.
77.7 min.
For A(g) → products with one extra mole of gas formed, partial pressure of reactant at time t is PA = 2P0 - Pt. With P0 = 35.0 mm, at 360 s PA = 70 - 54 = 16 mm. k = (2.303/360)log(35/16) = 2.17 x 10^-3 s^-1. At 720 s, PA = 70 - 63 = 7 mm, giving k = 2.24 x 10^-3 s^-1. Thus k ≈ 2.2 x 10^-3 s^-1.
k ≈ 2.2 x 10^-3 s^-1.
For SO2Cl2(g) → SO2(g) + Cl2(g), pressure of SO2Cl2 at time t is 2P0 - Pt. At 100 s, PSO2Cl2 = 1.0 - 0.6 = 0.4 atm. k = (2.303/100)log(0.5/0.4) = 2.23 x 10^-3 s^-1. When total pressure is 0.65 atm, PSO2Cl2 = 1.0 - 0.65 = 0.35 atm. Rate = kP = (2.23 x 10^-3)(0.35) = 7.8 x 10^-4 atm s^-1.
7.8 x 10^-4 atm s^-1.
Arrhenius equation is k = A e^(-Ea/RT), so A = k e^(Ea/RT). Substituting k = 2.418 x 10^-5 s^-1, Ea = 179900 J mol^-1, R = 8.314 J mol^-1 K^-1 and T = 546 K gives A = 3.93 x 10^12 s^-1.
A = 3.93 x 10^12 s^-1.
The units of k indicate a first order reaction. [A] = [A]0e^-kt = 1.0 e^-(2.0 x 10^-2)(100) = e^-2 = 0.135 mol L^-1.
0.135 mol L^-1.
For first order decay, fraction remaining = (1/2)^(t/t1/2). Thus fraction after 8 h = (1/2)^(8/3) = 0.157.
0.157 of the sample remains.
Compare k = Ae^-Ea/RT with k = (4.5 x 10^11 s^-1)e^-28000K/T. Therefore Ea/R = 28000 K, so Ea = 28000 x 8.314 = 2.33 x 10^5 J mol^-1 = 233 kJ mol^-1.
Ea = 233 kJ mol^-1.
For Arrhenius form in common logarithms, log k = log A - Ea/(2.303RT). Thus Ea/(2.303R) = 1.25 x 10^4 K, so Ea = 2.303 x 8.314 x 1.25 x 10^4 = 2.39 x 10^5 J mol^-1. If t1/2 = 256 min, k = 0.693/(256 x 60) = 4.51 x 10^-5 s^-1. Substituting in log k = 14.34 - 1.25 x 10^4/T gives T ≈ 669 K.
Ea = 239 kJ mol^-1; T ≈ 669 K.
Use log(k2/k1) = Ea/(2.303R)(1/T1 - 1/T2). Here k1 = 4.5 x 10^3 s^-1, k2 = 1.5 x 10^4 s^-1, T1 = 283 K and Ea = 60000 J mol^-1. Solving gives T2 = 297 K, or about 24°C.
297 K, approximately 24°C.
For equal times, k298/k308 = log(100/90)/log(100/75). This gives the ratio of rate constants. Using log(k308/k298) = Ea/(2.303R)(1/298 - 1/308), Ea ≈ 7.67 x 10^4 J mol^-1. Then Arrhenius equation k = Ae^-Ea/RT with A = 4 x 10^10 s^-1 and T = 318 K gives k ≈ 1.02 x 10^-2 s^-1.
Ea ≈ 76.7 kJ mol^-1; k at 318 K ≈ 1.02 x 10^-2 s^-1.
Use log(k2/k1) = Ea/(2.303R)(1/T1 - 1/T2). Here k2/k1 = 4, T1 = 293 K and T2 = 313 K. Thus Ea = 2.303R log4 x (T1T2)/(T2 - T1) = 5.29 x 10^4 J mol^-1 = 52.9 kJ mol^-1.
52.9 kJ mol^-1.