THERMODYNAMICS OF THE HYDROCHLORINATION REACTION OF PROPYLENE
The hydrochlorination reaction of propylene
Submitted 1957-01-01 | RussiaRxiv: ru-195701.73743 | Translated from Russian

Abstract

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PHYSICAL CHEMISTRY

S. G. ENTELIS and N. M. CHIRKOV

THERMODYNAMICS OF THE HYDROCHLORINATION REACTION OF PROPYLENE

(Presented by Academician V. N. Kondrat’ev, November 24, 1956)

The hydrochlorination reaction of propylene

[
\mathrm{C_3H_6 + HCl \rightleftarrows u\text{-}C_3H_7Cl}
]

is reversible, but direct measurements of the equilibrium constants and of the heat of the process are lacking.

We assume, in accordance with tabulated data, that the heats of formation (\Delta H^0_{f\,298.2}) of propylene, hydrogen chloride, and isopropyl chloride are, respectively: (+4879) cal/mole ((^1)); (-22063) cal/mole ((^2)) and (-31000) cal/mole ((^3)), and that the entropies (S^0_{298.2}) are, respectively: (+63.8) cal/mole·deg ((^1)); (44.62) cal/mole·deg ((^2)) and (72.4) cal/mole·deg ((^3)). Hence the changes in heat content and entropy in the reaction will be (\Delta H_R = -13816) cal/mole, (\Delta S_R = -36.02) cal/mole·deg. Consequently:

[
2.3R K_p = 13816/T - 36.02.
\tag{1}
]

Table 1

Values of (\alpha_{\mathrm{d}}) and (\alpha_{\mathrm{an}}) in experiments on the hydrochlorination of propylene on (\mathrm{H_3PO_4}) with 72% (\mathrm{P_2O_5})

(T,\ ^\circ\mathrm{C}) (p_{\mathrm{C_3H_6}_0}), mm Hg (p_{\mathrm{HCl}_0}), mm Hg (\alpha_{\mathrm{d}}) (\alpha_{\mathrm{an}})
70 50 50 0.380 0.380
70 100 100 0.322 0.350
70 200 200 0.512 0.523
70 300 300 0.788 0.787
100 200 200 0.326 0.322
160 200 200 0.475 0.480
180 200 200 0.456 0.441

Experimentally, the heat of reaction was measured by Thomsen ((^4)):

[
\Delta H_R = -11960 \ \text{cal/mole}.
]

In our experiments the equilibrium was studied by pressure in a static apparatus (we used the same apparatus as in work ((^5))) at temperatures of 100, 120, 140, 160, and 180°C; the catalyst was orthophosphoric acid with 72% (\mathrm{P_2O_5}). Equilibrium was reached both from the side of HCl and (\mathrm{C_3H_6}) and from the side of (u\text{-}\mathrm{C_3H_7Cl}). Attainment of equilibrium by the system was determined from the complete cessation of pressure change. In those cases where it was not possible to observe a complete cessation of the reaction, the equilibrium pressure was found by extrapolation to zero rate on a pressure—reaction-rate graph. The corrections usually introduced were very small.

Before the measurements were carried out, it was found that (u\text{-}\mathrm{C_3H_7Cl}) is, under our conditions, the only reaction product. For this purpose, in a flow apparatus in the presence of the catalyst—phosphoric acid on porous glass—at (T = 100^\circ\mathrm{C}), an amount of the reaction product between HCl and (\mathrm{C_3H_6}) sufficient for distillation was obtained. Distillation of the dry product on a column with an efficiency of 16 theoretical plates showed,

that the entire product distills in the range 33.3–34.5° C and has (n_D^{15} 1.3810) (literature data: (n_D^{15} 1.3811) and b.p. 34.8° C).

Since observations of the course of the reaction were made by the change in pressure in the system, (\Delta p), it was first necessary to establish that there was a correspondence between the value of (\Delta p) and the extent of reaction (\alpha). A series of experiments was carried out in which, in addition to (\Delta p), the change in the amount of HCl ((\Delta N)) in the system was analyzed acidimetrically. Table 1 gives the values (\alpha_{\mathrm{p}}=\Delta p/p_0) and (\alpha_{\mathrm{an}}=\Delta N/N_0), where (p_0) and (N_0) are, respectively, the initial pressure and the initial amount of HCl in the system.

As can be seen from Table 1, in all the cases cited there is satisfactory agreement between (\alpha_{\mathrm{p}}) and (\alpha_{\mathrm{an}}).

In order to show that the equilibrium studied is a true one and is not associated with the presence of kinetic limiting phenomena, it must be reached both from the side of synthesis and from the side of decomposition of the product.

In Fig. 1 are shown the kinetic curves of the synthesis (1) and decomposition (2) of isopropyl chloride at 160° C in coordinates: pressure of (u)-(\mathrm{C_3H_7Cl}) in the reaction mixture—time. For convenience in comparing curves 1 and 2, the pressure is expressed in relative units; the initial pressure of (u)-(\mathrm{C_3H_7Cl}) in the decomposition reaction was taken as unity.

Fig. 1. Kinetic curves of the synthesis (1) and decomposition (2) of isopropyl chloride on orthophosphoric acid (72% (\mathrm{P_2O_5})). Amount of acid 1.2 g (calculated as 100% (\mathrm{H_3PO_4})); reactor volume 404.2 cm³.

Table 2

Equilibrium constants (K_p) of the reaction

[
\mathrm{C_3H_6 + HCl = u\text{-}C_3H_7Cl}
]

(T,\ ^\circ\mathrm{C}) (K_p,\ \mathrm{atm}^{-1}) Mean value (K_p) (T,\ ^\circ\mathrm{C}) (K_p,\ \mathrm{atm}^{-1}) Mean value (K_p)
100 151.0 151.0 14.6
120 57.0 58.8 13.8
120 60.5 58.8 6.5
140 25.4 25.8 160 13.5 12.6
140 27.4 25.8 14.3 12.6
140 24.4 25.8 13.8* 12.6
180 6.1 5.9 10.7 12.6
180 5.6 5.9 13.5* 12.6
13.1 12.6
12.6 12.6

* Equilibrium was reached from the side of decomposition.

For the synthesis reaction, 200 mm Hg of (u)-(\mathrm{C_3H_7Cl}) was taken; for the synthesis reaction, HCl and (\mathrm{C_3H_6}) in a 1:1 ratio were taken at a total pressure of 400 mm Hg. Obviously, when true thermodynamic equilibrium is attained, in both cases the composition of the equilibrium mixture must be the same. As can be seen from Fig. 1, both curves reach equilibrium at one and the same composition of the mixture HCl—(\mathrm{C_3H_6})—(u)-(\mathrm{C_3H_7Cl}).

The equilibrium constants of the reaction obtained in the experiments represented by curves 1 and 2 in Fig. 1 are close in magnitude and are equal, respectively, to 13.1 and 13.5 (\mathrm{atm}^{-1}). Table 2 gives the values found for the equilibrium constants

[
K_p=\frac{p_{u-\mathrm{C_3H_7Cl}}}{p_{\mathrm{HCl}}\,p_{\mathrm{C_3H_6}}}.
]

In Fig. 2 the data of Table 2 are presented in coordinates (\lg K_p—1/T). From the slope of the straight line, the heat of reaction was found to be

[
\Delta H_R=-13800\pm 300\ \mathrm{cal/mol}.
]

Knowing (\Delta H_R) and (K_p), one can find the change in entropy at

reaction: (\Delta S_R=-27.0\pm0.7) cal/mol·deg, whence for the equilibrium constant in the temperature interval (100\text{–}180^\circ\mathrm{C}) we obtain the expression

[
2.3R\lg K_p^{*}=13800/T-27.0.
\tag{2}
]

As can be seen, the heat of reaction found by us agrees well with the value (\Delta H_{R\,298.2}=-13816) cal/mol, calculated from tabulated data; however, (\Delta S_R) differs markedly from the calculated (\Delta S_{R\,298.2}=-36.02) cal/mol·deg. The difference in temperatures cannot explain the discrepancy in (\Delta S_R) of 9 entropy units. Although the values of (c_p) for the substances participating in the reaction of interest to us are unknown, the order of the change in entropy with temperature can be seen from the example of the hydrochlorination reaction of ethylene. The change in heat capacity in the course of the reaction is

[
\Delta c_p=c_{p\,\mathrm{C_2H_5Cl}}-c_{p\,\mathrm{C_2H_4}}-c_{p\,\mathrm{HCl}}
=
]

[
=-2.37\ \text{cal/mol·deg}
]

(calculated from the data of (²)), whence, according to the known formula

[
\Delta S_{RT}=\Delta S_{R\,298.2}-2.3\cdot2.37\cdot\lg\frac{T}{298.2}.
]

As can be seen from the formula, a change in temperature from 298.2 to 453 °K will cause a change in (\Delta S_R) of only 0.98 cal/mol·deg.

Fig. 2. Temperature dependence of the equilibrium constant (K_p\ \mathrm{atm}^{-1}) for the reaction (\mathrm{C_3H_6+HCl \rightleftarrows u\text{-}C_3H_7Cl}).

Fig. 2. Temperature dependence of the equilibrium constant (K_p\ \mathrm{atm}^{-1}) for the reaction (\mathrm{C_3H_6+HCl \rightleftarrows u\text{-}C_3H_7Cl}).

For clarity we have given in Table 3 the values of the maximum depths of conversion (\alpha_\infty=\Delta p_\infty/p_0), where (\Delta p_\infty) is the maximum change of pressure in the reaction in mm Hg, and (p_0) is the initial partial pressure of one of the components in a mixture of composition 1:1 in mm Hg. The values (\alpha_\infty) were calculated by the formula:

[
\alpha_\infty=\left(1+\frac{A}{2}\right)-\sqrt{\left(1+\frac{A}{2}\right)^2-1},
\quad \text{where}\quad A=\frac{760}{K_p p_0}.
]

Table 3

Values of (\alpha_\infty) for the hydrochlorination reaction of propylene

(T=70^\circ\mathrm{C},\ K_p=775\ \mathrm{atm}^{-1*}) (T=70^\circ\mathrm{C},\ K_p=775\ \mathrm{atm}^{-1*}) (T=70^\circ\mathrm{C},\ K_p=775\ \mathrm{atm}^{-1*}) (T=70^\circ\mathrm{C},\ K_p=775\ \mathrm{atm}^{-1*}) (T=100^\circ\mathrm{C},\ K_p=151\ \mathrm{atm}^{-1}) (T=100^\circ\mathrm{C},\ K_p=151\ \mathrm{atm}^{-1}) (T=100^\circ\mathrm{C},\ K_p=151\ \mathrm{atm}^{-1}) (T=100^\circ\mathrm{C},\ K_p=151\ \mathrm{atm}^{-1}) (T=120^\circ\mathrm{C},\ K_p=59.5\ \mathrm{atm}^{-1}) (T=120^\circ\mathrm{C},\ K_p=59.5\ \mathrm{atm}^{-1}) (T=120^\circ\mathrm{C},\ K_p=59.5\ \mathrm{atm}^{-1}) (T=120^\circ\mathrm{C},\ K_p=59.5\ \mathrm{atm}^{-1})
(p_0), mm 50 100 200 250 50 100 200 500 50 100 200 500
(\alpha_\infty) 0.88 0.94 0.93 0.94 0.63 0.80 0.84 0.90 0.61 0.70 0.77 0.84

From Table 3 it is seen that reversibility begins to have an appreciable effect only at (120^\circ\mathrm{C}); at (100^\circ\mathrm{C}), and still more at (70^\circ\mathrm{C}), reversibility is small.

Institute of Chemical Physics
Academy of Sciences of the USSR

Received
6 XI 1956

CITED LITERATURE

  1. E. J. Prosen, F. D. Rossini, J. Res. Bur. Stand., 36, 296 (1946).
  2. Select. Val. Chem., Thermodyn. Prop. Circ. Nat. Bur. Stand., 500 (1952).
  3. J. L. Franklin, Trans. Farad. Soc., 48, 443 (1952).
  4. J. Thomsen, Thermochem. Untersuch., 4, 372.
  5. S. G. Entelis, N. M. Chirkov, ZhFKh, 30, issue 11 (1956).

* The value of (K_p) for (70^\circ\mathrm{C}) was calculated from equation (2).

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THERMODYNAMICS OF THE HYDROCHLORINATION REACTION OF PROPYLENE