Chapter 5: Isothermal Reactor Design: Conversion


Rate Constants From Semilog Graphs

This example shows how to determine the rate constant for a reaction by finding the slope of a line on semilog paper. Please refer to Example 5.1 from the text. This example picks up from step 5 in the text (bottom of page 152).

\(-\frac{dC_A}{dt} = kC_A \quad (E4-1.3)\)

5. Evaluate. For isothermal operation, \(k\) is constant, so we can integrate this equation (E4-1.3).

\( -\int_{C_{A_0}}^{C_A} \frac{dC_A}{C_A} = \int_0^t k \,dt = k \int_0^T dt \)

Using the initial condition that when \(t = 0\), then \(C_A = C_{A_0}\). The initial concentration of A after mixing the two volumes together is 1.0 kmol/m³ (1 mol/L).

Integrating yields:

\( \ln \frac{C_{A_0}}{C_A} = kt \) (E4-1.4)

The concentration of ethylene oxide at any time \( t \) is:

\( C_A = C_{A_0} e^{-kt} \) (E4-1.5)

The concentration of ethylene glycol at any time \( t \) can be obtained from the reaction stoichiometry:

\( \text{A + B} \longrightarrow \text{C} \) \( N_C = N_{A_0} X = N_{A_0} - N_A \)

For liquid-phase reactions \( V = V_0 \):

\( C_C = \frac{N_C}{V} = \frac{N_C}{V_0} = C_{A_0} - C_A = C_{A_0} \left( 1 - e^{-kt} \right) \) (E4-1.6)

Rearranging and taking the logarithm of both sides yields:

\[ \ln \frac{C_{A_0} - C_C}{C_{A_0}} = -kt \quad \text{(E4-1.7)} \]

We see that a plot of \(\ln[(C_{A_0} - C_C)/C_{A_0}]\) as a function of \(t\) will be a straight line with a slope \(-k\). Calculating the quantity \((C_{A_0} - C_C)/C_{A_0}\) (Table E4-1.3) and then plot:

Table E4-1.3
\( t \) (min) \( C_C \) (kmol/m\(^3\)) \( \frac{C_{A_0} - C_C}{C_{A_0}} \)
0.0 0.000 1.000
0.5 0.145 0.855
1.0 0.270 0.730
1.5 0.376 0.624
2.0 0.467 0.533
3.0 0.610 0.390
4.0 0.715 0.285
6.0 0.848 0.152
10.0 0.955 0.045

Graph showing the normalized concentration (CA0 - C) / CA0 versus time (t) in minutes for a reaction. The data points are connected by a straight line, with time values ranging from 1 to 10 minutes. Figure E4-1.1 is labeled below the graph.

\( k = \frac{\ln 10}{t_2 - t_1} = \frac{2.3}{8.95 - 1.55} = 0.311 \, \text{min}^{-1} \quad \text{(E4-1.8)} \)

The rate law becomes:

\( \boxed{-r_A = (0.311 \, \text{min}^{-1}) C_A} \quad \text{(E4-1.9)} \)

This rate law can now be used in the design of an industrial CSTR.

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