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Journal of Research of the National Bureau of Standards. Section A, Physics and Chemistry logoLink to Journal of Research of the National Bureau of Standards. Section A, Physics and Chemistry
. 1960 Dec 1;64A(6):515–519. doi: 10.6028/jres.064A.051

Heat of Formation of Titanium Trichloride

Walter H Johnson, Alexis A Gilliland, Edward J Prosen
PMCID: PMC5287342  PMID: 32196252

Abstract

A calorimetric comparison of the heat of hydrolysis of TiCl4(liq) with the heat of oxidation and hydrolysis of TiCl3(c) has been made. The following value is reported for the combination of these data according to the process:

TiCl3(c)+½I2(c)+HCl(g)TiCl4(liq)+HI(g),ΔH°(25°C)=8.37±0.30kcal/mole.

A combination of this value with −192.3 ±0.7 kcal/mole for the heat of formation of TiCl4(liq) and with the standard heats of formation of HCl(g) and HI(g) gives for TiCl3(c), ΔHf°(25 °C) = −172.4±0.8 kcal/mole.

1. Introduction

Several independent determinations of the heat of formation of titanium trichloride have been reported during the past few years [1, 2, 3, 4, 5, 6].1 The only values previously available were those estimated by Brewer, Bromley, Gilles, and Lofgren [7] and by Kubaschewski and Evans [8], which are now generally known to be low. The difficulties encountered in the purification of titanium trichloride and its reactivity toward oxygen and moisture have no doubt contributed to the scarcity of experimental data.

We conducted a number of experiments on the reaction between crystalline TiCl3 and gaseous chlorine in a calorimetric vessel originally designed for measurement of the heat of formation of boron trichloride [9]. Although TiCl3(c) is readily converted to TiCl4(g) by the action of chlorine at about 300 °C, a portion of the finely divided sample was carried away by the gas stream. The insertion of a glass wool plug tended to reduce the transfer of TiCl3, but the presence of adsorbed moisture introduced significant errors in the determination of the quantity of reaction.

We therefore decided to use a solution calorimeter to make a comparison between the heats of formation of TiCl3(c) and TiCl4(liq). When TiCl3(c) is added to aqueous acid containing an oxidizing agent, the titanium is converted to the tetravalent state; the resulting solution may be reproduced by adding TiCl4 to an acid solution which contains the reduced form of the oxidizing agent. The difference between the heats of formation of TiCl4 and TiCl3 may be determined from a combination of the heat of oxidation and hydrolysis of TiCl3 with the heat of hydrolysis of TiCl4 and with certain auxiliary data. This method is similar to that employed by Clifton and MacWood [1], except that the experiments were performed at 30 °C instead of 0 °C and iodine was used as the oxidizing agent instead of FeCl3.

2. Source and Purity of Materials

The TiCl4 and TiCl3 were prepared by the Inorganic Chemistry Section of the Chemistry Division. The purity of the TiCl4 was determined to be 99.99 mole percent by freezing point determinations made in the Pure Substances Section of the Chemistry Division. This material was the same as that used previously for the determination of the heat of formation of TiI4 [9].

The purity of the TiCl3 was determined by the Inorganic Chemistry Section to be greater than 99.8 percent. Analyses of the solutions obtained after hydrolysis indicated the purity to be 100 ± 0.2 percent.

The iodine, potassium iodide, and hydrochloric acid were reagent-grade materials used with no further purification. The hydriodic acid was redistilled and the constant-boiling fraction collected under a nitrogen atmosphere.

3. Apparatus and Procedure

The apparatus was the same as that used for the determination of the heat of formation of TiI4 [9], except for minor changes. Capillary inlet and exit tubes were inserted through the calorimeter head to permit removal of oxygen by flushing with nitrogen. Calorimeter temperatures were measured by means of a platinum resistance thermometer. The thermometric system, the apparatus for measurement of electrical energy, and the calorimetric procedure have been described in previous reports [11, 12].

3.1. Hydrolysis of TiCl4 (liq)

Samples, approximately 0.01 mole each, of the TiCl4 were transferred into thin-walled, spherical Pyrex bulbs and sealed in vacuum. The calorimetric solution consisted of 0.01 mole KI, 0.02 mole I2, 0.40 mole HC1, 0.01 mole HI, and 25.33 moles water. The iodine and KI were dissolved in a small quantity of water before adding the other materials; the HI was taken from a constant-boiling solution and the HCl from a prepared 4N solution. The remainder of the water was added to bring the total weight up to the previously calculated value. The calorimeter was then assembled, placed in the constant-temperature calorimeter jacket, the stirrer connected, and oxygen removed by flushing with nitrogen. The inlet and exit tubes were then closed, leaving a slight positive pressure of about 1 mm above atmospheric pressure in the calorimeter.

Calorimeter temperatures were noted at 2-minute intervals during the initial rating-period, after which the sample bulb was crushed and temperatures measured at 1-minute intervals until thermal equilibrium was reestablished. Temperatures were then noted at 2-minute intervals during a final rating-period.

The rate of hydrolysis was quite rapid, the hydrolysis being essentially complete within one minute. In a few cases some of the calorimetric solution was splashed upon the upper walls of the vessel; in such cases the experiment was discarded. The reaction produced no noticeable difference in the color of the solution.

The calorimeter was calibrated in the same manner, except that an empty bulb was used and the temperature rise was derived from a carefully measured quantity of electrical energy introduced into the system.

3.2. Hydrolysis of TiCl3(s)

Samples, approximately 0.01 mole each, of the finely divided TiCl3 were transferred into glass bulbs in a dry-box under an atmosphere of nitrogen. The bulbs were capped while in the box, then removed and sealed.

The calorimetric solution was the same as that used for the experiments with TiCl4, except that the HI was omitted and the quantities of iodine and HCl were increased to 0.025 and 0.41 mole respectively. The calorimetric procedure was the same as that described for the TiCl4 experiments.

The rate of hydrolysis was quite rapid at first, but quickly slowed down; the hydrolysis was not complete after 1½ hrs at 25 °C. We found it necessary to raise the calorimeter temperature to 30 °C in order to obtain complete hydrolysis within one hour. The resulting solutions developed some turbidity after standing in air for a few hours. In a few cases the solutions were stored in completely filled and stoppered amber bottles; in these cases no turbidity appeared even after several days.

The system was calibrated with electrical energy, at 25 and at 30 °C, using both the initial and final solutions in order to obtain ΔCp for the actual calorimetric process. The effective heat capacity of the empty calorimeter was determined by substituting a known weight of distilled water for the calorimetric solution.

3.3. Heat of Solution of Iodine

The iodine samples, approximately 0.005 mole each, were sealed into glass bulbs. The calorimetric solution was the same as used for TiCl3 experiments, except that only 0.02 mole of iodine was used. Because the solution of iodine resulted in a relatively small drop in the calorimeter temperature, it was possible to calibrate the actual system immediately prior to the measurement of the heat of solution and it was not necessary to duplicate the system exactly for replicate experiments.

3.4. Heat of Dilution of Hydrochloric Acid

A solution of hydrochloric acid containing 13.5 moles of water per mole of HCl was prepared. Samples of this solution, each containing approximately 0.01 mole of HC1, were sealed into glass bulbs. The calorimetric solution consisted of 0.10 mole KI, 0.02 mole I2, 0.40 mole HCl, and 25.195 moles of water. Since the increase in the calorimeter temperature was smell, it was possible to calibrate the actual system before each experiment as described above.

4. Data and Calculations

Values from the 1955 table of International Atomic Weights [13] were used in all calculations. Except where specified to the contrary, the final temperature and pressure were 25 °C and 1 atmosphere. One thermochemical calorie is taken as equivalent to 4.1840 joules.

The results of the calibration experiments on the TiCl4 system are given in table 1. E is the electrical energy introduced into the system as measured by a method described previously [11, 12]. ΔRc is the temperature rise of the calorimetric system as measured with a particular platinum resistance thermometer and bridge, corrected by a method described previously [14]. The energy equivalent of the system Es, is the ratio of the quantity of electrical energy to the resulting rise in temperature:

Es=EΔRc.

Table 1.

Results of the calibration experiments on the TiCl4 system

Experiment E ΔRc Es




j ohm j/ohm
1………….. 1939.62 0.090254 21491
2………….. 1937.46 .090022 21522
3………….. 1936.64 .090053 21506
4………….. 1934.99 .090001 21500
5………….. 1936.37 .090235 21459
6………….. 1931.84 .090000 21465


 Mean 21490
 Standard deviation of the mean ±10

The results of the experiments on the hydrolysis of T1Cl4 are given in table 2, where Δe is the deviation in the energy equivalent of the actual system from that of the calibrated system, ΔRc is the temperature rise of the system, and q is the total energy evolved in the actual process. The following relationship was used:

q=(Es+Δe)(ΔRc).

Table 2.

Results of the experiments on the hydrolysis of TiCl4

Experiment Δe ΔRc q TiCl4 mole −ΔH(25 °C)






j/ohm ohm j kj/mole
1…………. 7.9 0.069850 1501.7 0.0062711 239.46
2…………. 9.7 .082721 1778.3 .0074704 238.04
3…………. 11.0 .091447 1966.2 .0082202 239.20
4…………. 10.2 .085143 1830.6 .0076219 240.18
5…………. 12.2 .099699 2143.8 .0089877 238.53


 Mean 239.08
 Standard deviation of the mean ±0.37

The data given in table 2 for the hydrolysis of TiCl4 correspond to the process:

TiCl4(liq)+[10KI+2I2+HI+40HCl+2533H2O](soln)[Ti4++4Cl+10KI+2I2+HI+40HCl+2533H2O](soln);ΔH(25°C)=57.14±0.18kcal/mole. (1)

The results of the calibration experiments on the TiCl3 system and of the oxidation and hydrolysis experiments on TiCl3 are given in tables 3 and 4 respectively. These experiments were conducted at 30 °C in order to increase the rate of hydrolysis. Because of the relatively long period of time required for the establishment of thermal equilibrium, we failed to adjust the system precisely to a final temperature of 30 °C. A correction (qt) for the thermal coefficient of the process was made to correct all data to this temperature. The data given in table 4 correspond to the process:

TlCl3(c)+[10KI+2.5I2+41HCl+2533H2O](soln)[Ti4++4Cl+10KI+2I2+HI+40HCl+2533H2O](soln),ΔH(30°C)=51.87±0.21kcal/mole. (2)

Table 3.

Results of the calibration experiments on the TiCl3 system

Experiment E ΔRc Es(30° C)




j ohm j/ohm
1…………. 2282.25 0.105484 21636.0
2…………. 2420.74 .111916 21630.0
3…………. 2447.40 .113123 21634.9
4…………. 2407.39 .111278 21634.0
5…………. 2406.49 .111193 21642.5


 Mean 21635.5
 Standard deviation of the mean ±2.0

Table 4.

Results of the TiCl3 oxidation and hydrolysis experiments

Experiment Δe ΔRc q qt TiCl3 mole −ΔH(30 ° C)







j/ohm ohm j j kj/mole
1……….. 11.5 0.126488 2738.09 5.59 0.0127267 215.58
2……….. 7.8 .089936 1946.51 −0.13 .0089266 218.04
3……….. 8.4 .095814 2073.79 −0.26 .0095228 217.74
4……….. 8.2 .095842 2074.38 −0.31 .0095531 217.11
5……….. 10.1 .109841 2377.57 −0.15 .0109743 216.64


 Mean 217.02
 Standard deviation of the mean ±0.44

The value of ΔCp for the process corresponding to eq (2) was determined to be −82 cal/°C mole, this gives for eq (2),

ΔH(25°C)=51.46±0.21kcal/mole.

The results of the experiments on the heat of solution of iodine, given in table 5, correspond to the process:

½I2(c)+[10KI+2I2+41HCl+2533H2O](soln)[10KI+2.5I2+41HCl+2533H2O](soln);ΔH(25°C)=1.101±0.035kcal/moleI2. (3)

Table 5.

Results of the experiments on the solution of iodine

Experiment Es —ΔRc q I2mole ΔH (25 ° C)






j/ohm ohm j kj/mole
1………. 21231 0.001051 22.31 0.0050000 4.462
2………. 21463 .000850 18.24 .0041636 4.381
3………. 21438 .000912 19.55 .0044386 4.405
4………. 21605 .001088 23.51 .0050785 4.629
5………. 21454 .001149 24.65 .0050579 4.874
6………. 21468 .001013 21.75 .0048742 4.462
7………. 21574 .001086 23.43 .0049308 4.752
8………. 21535 .001136 24.46 .0049956 4.896


 Mean 4.608
 Standard deviation of the mean ±0.074

The results of the experiments on the dilution of hydrochloric acid are given in table 6 and correspond to the process:

[HCl+13.5H2O](soln)+[10KI+2I2+40HCl+2519.5H2O](soln)[10KI+2I2+41HCl+2533H2O](soln);ΔH(25°C)=0.603±0.004kcal/moleHCl. (4)

Table 6.

Results of the experiments on the dilution of hydrochloric acid

Experiment Es ΔRc q HCl mole −ΔH(25 °C)






j/ohm ohm j kj/mole
1………….. 21622 0.001109 23.98 0.0094364 2.541
2………….. 21588 .000972 20.98 .0083074 2.525
3………….. 21441 .001158 24.83 .0099317 2.500
4………….. 21425 .001236 26.48 .0104966 2.523


 Mean 2.522
 Standard deviation of the mean ±0.008

The heats of solution of HCl(gas) and of HI (gas) have been calculated from available data [15] for the following processes:

HCl(gas)+13.5H2O(liq)[HCl+13.5H2O](soln); (5)
ΔH(25°C)=16.77±0.01kcal/mole,HI(gas)+[10KI+2I2+40HCl+2533H2O](soln)[10KI+2I2+HI+40HCl+2533H2O](soln);ΔH(25°C)=19.51±0.10kcal/mole. (6)

The heat involved in diluting the KI–I2–HCl solution by approximately 0.5 percent has been calculated to be negligible within the precision of these experiments. For simplification of calculations, however, the following process has been included:

13.5H2O(liq)+[10KI+2I2+40HCl+2519.5H2O](soln)[10KI+2I2+40HCl+2533H2O](soln);ΔH(25°C)=0.00±0.01kcal/mole. (7)

We may subtract eqs (1), (6), and (7) from the sum of eqs (2), (3), (4), and (5) to obtain the following theoretical process:

TiCl3(c)+½I2(c)+HCl(gas)TiCl4(liq)+HI(gas);ΔH°(25°C)=8.37±0.30kcal/mole. (8)

The change in enthalpy for eq (8) may be combined with −22.063±0.002 and 6.20±0.10 kcal/mole, the standard heats of formation of HCl(gas) and HI (gas) [15] respectively, to give:

TiCl3(c)+12Cl2(gas)TiCl4(liq);ΔH°(25°C)=19.89±0.32kcal/mole. (9)

By taking −192.3 ±0.7 kcal/mole for the heat of formation of TiCl4(liq) [16],2 we obtain:

TiCl3(c),ΔHf°(25°C)=172.4±0.8kcal/mole.

The results obtained from the experiments on the direct chlorination gave −19.9±1.3 kcal/mole for the process corresponding to eq (9).

The uncertainties assigned to the values given in this paper are over-all uncertainties obtained by combining twice the standard deviation of the mean for the calibration and reaction experiments with reasonable estimates of all other known sources of error.

5. Discussion

The value obtained in this investigation is essentially the same as that obtained by Clifton and MacWood [1] from measurements of the energies evolved when TiCl3(c) and TiCl4(liq) were dissolved in an aqueous solution of HC1 and FeCl3.

Schaffer, Bred, and Pfeffer [2] measured the heat of chlorination of TiCl3 at 57 °C and obtained −20.3 kcal/mole for the process corresponding to eq (9). They also measured the heat of reduction of TiCl4 at 153 °C, with mercury as the reducing agent, and obtained −19.8 kcal/mole for eq (9). The values which they reported for the heat of formation of TiCl3, however, were based upon the value calculated by Bichowsky and Rossini [17] for the heat of formation of TiCl4(liq), which has since been shown to be low. If we combine the data obtained by Schaffer, Bred, and Pfeffer with −192.3±0.7 kcal/mole for the heat of formation of TiCl4(liq), we obtain −172.0 and −172.5 kcal/mole for the heats of formation of TiCl3(c) obtained by the chlorination and reduction processes, respectively.

Krieve and Mason [3] studied the equilibrium:

TiCl3(c)+HCl(gas)=TiCl4(gas)+12H2(gas),

and obtained ΔH690= 10.4 kcal/mole. They estimated the ΔCp of the process to be −6 cal/deg mole, used Kelley’s value of 9.6 kcal/mole [18] for the heat of vaporization of TiCl4(liq) [2], and obtained −19.0 kcal/mole for eq (9). We have corrected their data by the use of 9.9 kcal/mole for the heat of vaporization of liquid TiCl4 [2] and have obtained −19.3 kcal/mole for the process corresponding to eq (9). Combination of this value with −192.3 kcal/mole for the heat of formation of TiCl4(liq), gives −173.0 kcal/mole for the heat of formation of TiCl3(c).

Krieve, Vango, and Mason [4] reacted Ti(c), TiCl2(c), and TiCl3(c) with chlorine under pressure in a nickel-bomb calorimeter to form TiCl4(liq). They obtained −190.0 and −20.9 kcal/mole for the heats of chlorination of Ti(c) and TiCl3(c), respectively, and reported −169.1 kcal/mole for the heat of formation of TiCl3(c). If we take their value for the heat of chlorination of TiCl3(c) and use our value for the heat of formation of TiCl4(liq), we obtain −171.4 kcal/mole for the heat of formation of TiCl3(c).

Skinner and Ruehrwein [5] measured the heats of solution of Ti(c) and TiCl3(c) in aqueous hydrofluroic acid. They obtained −170.0 kcal/mole for the heat of formation of TiCl3(c).

Altman, Farber, and Mason [6] have reported values of −169.4 and −171.0 kcal/mole for the heat of formation of TiCl3(c), based upon disproportionation and sublimation studies by Farber and Darnell [19, 20].

A summary of the results obtained by the various investigators is given in table 7. An examination of the results in this table indicates substantial agreement on the difference between the heats of formation of TiCl3(c) and TiCl4(liq).

Table 7.

Heat of formation of TiCl3 reported by the various investigators, kcal/mole at 25 °C

ΔHfTiCl3(s)ΔHfTiCl4(liq) ΔHfTiCl3(s) Reference



  19.9   172.4 1
  20.3   172.0 2
  19.8   172.5 2
  19.3   173.0 3
  20.9   169.1 4
  171.4 4
  170.0 5
  169.4 6
  171.0 6
  19.9±0.3   172.4±0.8 This investigation.

Footnotes

1

Figures in brackets indicate the literature references at the end of this paper.

2

The heat of vaporization of TiCl4(liq) has been taken as 9.9 ±0.2 kcal/mole from the calorimetric data of Schaffer, Breil, and Pfeffer [2].

6. References

  • 1.Clifton DG, MacWood GE. J Phys Chern. 1956;60:309. [Google Scholar]
  • 2.Schaffer H, Breil G, Pfeffer G. Z anorg u allgem Chem. 1954;276:325. [Google Scholar]
  • 3.Krieve WF, Mason DM. J Chem Phys. 1956;25:524. [Google Scholar]
  • 4.Krieve WF, Vango SP, Mason DM. J Chem Phys. 1956;25:519. [Google Scholar]
  • 5.Skinner GB, Ruehrwein RA. J Phys Chem. 1955;50:113. [Google Scholar]
  • 6.Altman D, Farber M, Mason DM. J Chem Phys. 1956;25:531. [Google Scholar]
  • 7.Brewer L, Bromley LA, Gilles PW, Lofgren NL. In: Paper No 6. Quill LL, editor. McGraw-Hill Book Company, Inc.; New York, N.Y.: 1950. (Chemistry and metallurgy of miscellaneous materials, thermodynamics, National Nuclear Energy Series IV-19B). [Google Scholar]
  • 8.Kubaschewski O, Evans ELL. Metallurgical thermochemistry. I. Academic Press Inc.; New York, 10, N. Y.: 1951. [Google Scholar]
  • 9.Johnson WH, Miller RG, Prosen EJ. J Research NBS. 1959;62:213. RP2956. [Google Scholar]
  • 10.Johnson WH, Gilliland AA, Prosen EJ. J Research NBS. 1959;63A:161. doi: 10.6028/jres.063A.009. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 11.Prosen EJ, Maron FW, Rossini FD. J Research NBS. 1951;46:106. RP2181. [Google Scholar]
  • 12.Eckman JR, Rossini FD. BS J Research. 1929;3:597. RP111. [Google Scholar]
  • 13.Wichers E. J Am Chem Soc. 1956;78:3238. [Google Scholar]
  • 14.Prosen EJ. In: Chapter 6 in Experimental thermochemistry. Rossini FD, editor. Interscience Publishers, Inc.; New York, N.Y.: 1956. [Google Scholar]
  • 15.Rossini FD, Wagman DD, Evans WH, Levine S, Jaffe I. NBS Cire. Vol. 500. U.S. Government Printing Office; Washington 25, D.C.: 1952. Selected values of chemical thermodynamic properties. [Google Scholar]
  • 16.Johnson WH, Nelson RA, Prosen EJ. J Research NBS. 1959;62:1. RP2928. [Google Scholar]
  • 17.Bichowsky FR, Rossini FD. Thermochemistry of the chemical substances. Reinhold Publishing Corp.; New York, N.Y.: 1936. [Google Scholar]
  • 18.Kelley KK. Bull. Vol. 383. U.S. Government Printing Office; Washington 25, D.C.: 1935. Contributions to the data on theoretical metallurgy, III. The free energies of vaporization and vapor pressures of inorganic substances, US Bureau of Mines. [Google Scholar]
  • 19.Farber M, Darnell AJ. J Chem Phys. 1956;25:526. [Google Scholar]
  • 20.Farber M, Darnell AJ. J Phys Chem. 1955;59:156. [Google Scholar]

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