1. Reaction and Diffusion
where R* is the distance between the two colliding reactant molecules and D is the sum of the diffusion coefficients of the two reactant species (DA + DB).
where η is the viscosity of the medium. RA and RB are the hydrodynamic radius of A and B.
If we assume RA = RB = 1/2R*

2. 24.3 The material balance equation
(a) The formulation of the equation
the net rate of change due to chemical reactions
the overall rate of change
the above equation is called the material balance equation.

3. (b) Analytical solutions of the material balance equation
Using numerical method: Euler method or 4th order Runge-Kutta method to
Integrate the differential equation set.

4. Fig. 1 Snapshots of stationary 2D spots (A) and stripes (B) in a thin layer and 2D images of the corresponding 3D structures (A→B, C; B→E to G) in a capillary.
Snapshots of stationary 2D spots (A) and stripes (B) in a thin layer and 2D images of the corresponding 3D structures (A→B, C; B→E to G) in a capillary. Initial concentrations: [malonic acid] = 0.25 M; [H2SO4] = 0.20 M (A, B, D to G), 0.15 M (C); [NaBrO3] = 0.16 M (A and B), 0.20 M (D to G), 0.21 M (C); [ferroin] = 10 mM. ω = 13.9; ϕd = Inner diameter of capillaries: (B and C) 0.6 mm; (E to G) 0.3 mm. Bright regions correspond to high concentrations of the oxidized form of the catalyst. Dark bands at the capillary walls are due to a slight mismatch in refractive index. Scale bar, 1 mm.
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5. Fig. 3 Stationary structures in numerical simulations.
Stationary structures in numerical simulations. Spots (A), hexagonal close-packing (B), labyrinthine (C), tube (D), half-pipe (E), and lamellar (F) emerging from asymmetric [(A), (B), and (E)], symmetric [(D) and (F)], and random (C) initial conditions in a cylindrical domain. Numerical results are obtained from the model:
dx/dτ = (1/ε)[fz(q – x)/(q + x) + x(1 – mz)/(ε1 + 1 – mz) – x2] + ∇2x;
dz/dτ = x(1 – mz)/(ε1 + 1 – mz) – z + dz∇2z,
where x and z denote the activator, HBrO2 and the oxidized form of the catalyst, respectively; dz is the ratio of diffusion coefficients Dz/Dx; and τ is the dimensionless time. Parameters (dimensionless units): q = ; m = ; ε1 = 0.02; ε = 2.2; f = (A) 1.1, (B) 0.93, [(C) to (F)] 0.88; and dz = 10. Size of domains (dimensionless): diameter = 20 [(A) to (C) and (F)]; 14 [(D) and (E)]; height = 40.
Stationary structures in numerical simulations. Spots (A), hexagonal close-packing (B), labyrinthine (C), tube (D), half-pipe (E), and lamellar (F) emerging from asymmetric [(A), (B), and (E)], symmetric [(D) and (F)], and random (C) initial conditions in a cylindrical domain. Numerical results are obtained from the model: dx/dτ = (1/ε)[fz(q – x)/(q + x) + x(1 – mz)/(ε1 + 1 – mz) – x2] + ∇2x; dz/dτ = x(1 – mz)/(ε1 + 1 – mz) – z + dz∇2z, where x and z denote the activator, HBrO2 and the oxidized form of the catalyst, respectively; dz is the ratio of diffusion coefficients Dz/Dx; and τ is the dimensionless time. Parameters (dimensionless units): q = ; m = ; ε1 = 0.02; ε = 2.2; f = (A) 1.1, (B) 0.93, [(C) to (F)] 0.88; and dz = 10. Size of domains (dimensionless): diameter = 20 [(A) to (C) and (F)]; 14 [(D) and (E)]; height = 40.
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6. Transition State Theory (Activated complex theory)
Using the concepts of statistical thermodynamics.
Steric factor appears automatically in the expression of rate constants.

7. 24.4 The Eyring equation
The transition state theory pictures a reaction between A and B as proceeding through the formation of an activated complex in a pre-equilibrium:
A + B ↔ C‡
( `‡` is represented by `±` in the math style)
The partial pressure and the molar concentration have the following relationship:
pJ = RT[J]
thus
The activated complex falls apart by unimolecular decay into products, P,
C‡ → P v = k‡[C‡] So
Define
v = k2[A][B]

8. (a) The rate of decay of the activated complex
k‡ = κv
where κ is the transmission coefficient. κ is assumed to be about 1 in the absence of information to the contrary. v is the frequency of the vibration-like motion along the reaction-coordinate.

9. (b) The concentration of the activated complex
Based on Equation (or in 7th edition), we have
with ∆E0 = E0(C‡) - E0(A) - E0(B)
are the standard molar partition functions.
provided hv/kT << 1, the above partition function can be simplified to
Therefore we can write
qC‡ ≈
where denotes the partition function for all the other modes of the complex.
K‡ =

10. combine all the parts together, one gets
(c) The rate constant
combine all the parts together, one gets
then we get
(Eyring equation)
To calculate the equilibrium constant in the Eyring equation, one needs to know the partition function of reactants and the activated complexes.
Obtaining info about the activated complex is a challeging task.

11. (d) The collisions of structureless particles
A B → AB
Because A and B are structureless atoms, the only contribution to their partition functions are the translational terms:

12. 24.5 Thermodynamic aspects

13. Kinetics Salt Effect Ionic reaction A + B ↔ C‡ C‡ → P d[P]/dt = k‡[C‡]
the thermodynamic equilibrium constant
Then
d[P]/dt = k2[A][B]
Assuming is the rate constant when the activity coefficients are 1 ( )
Debye-Huckle limiting law with A = 0.509
log(k2) = log( ) + 2AZAZBI1/ (Analyze this equation)

14. Experimental tests of the kinetic salt effect

15. Example: The rate constant for the base hydrolysis of [CoBr(NH3)5]2+ varies with ionic strength as tabulated below. What can be deduced about the charge of the activated complex in the rate-determining stage? I
k/ko
Solution:
I1/
Log(k/ko)

16. 24.6 Reactive Collisions Properties of incoming molecules
can be controlled:
1. Translational energy.
2. Vibration energy.
3. Different orientations.
The detection of product molecules:
1. Angular distribution of products.
2. Energy distribution in the product.

17. 24.7 Potential energy surface
Can be constructed from experimental measurements or from Molecular Orbital calculations, semi-empirical methods,……

18. Potential energy is a function of the relative positions of all the atoms taking
Part in the reaction.

19. Crossing crowded dance floors.
Crossing crowded dance floors. In the dance that makes up a chemical reaction, an existing bond is broken (here, the C-H of the ring-shaped cyclohexane molecule) and a new one formed (a new C-H in the HCN product). The hydrogen atom (white sphere) is transferred to the CN radical, CN· + HC6H11 → HCN + C6H11·. (A) In the gas phase, the reactants collide unimpeded (the dance floor is clear). The straight red arrow shows a classical reactive trajectory superimposed on the potential energy surface. The contour map is a function of the lengths of the C-H bond being formed (vertical axis) and the one being broken (horizontal axis). Because the transition state (×) is early, the downhill descent directs kinetic energy into the newly forming H-CN bond. (B) In solution, the reactants move more chaotically across a crowded dance floor. Greaves et al. show that despite solvent friction, much of the energy released is still directed into the H-CN bond.
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20. Potential energy surfaces, pt. 2.

21. Various trajectories through the potential energy surface

22. 24.8 Results from experiments and calculations
(a) The direction of the attack and separation

23. Attractive and repulsive surfaces

24. Classical trajectories