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Aug., 1949 SPECTROPHOTOMETRYOF WITH AROMATICHYDROCARBONS 2703

[CONTRIBUTION FROM THE CHEMICAL LABORATORYOF THE UNIWRSITY OF CALIFORNIA] A Spectrophotometric Investigation of the Interaction of Iodine with Aromatic Hydrocarbons

BY H. A. BENESIAND J. H. HILDEBRAND Introduction more puzzling, since it behaves as a normal non- The various colors of iodine in different solvents polar liquid. The only plausible explanation ap- have attracted the attention of investigators for peared to be the one we stated some time ago in a over half a century. Beckmann’ showed that the brief “Communication to the Editor,” as follows: differences are not due to any change in the molec- “A possible explanation for the presence of such ular weight of iodine and suggested solvation as a complex appears to lie in an acid-base interac- the cause of brown color. Lachman2 supported tion in the electron donoracceptor sense such as this explanation, pointing out that the solvents we see in the union of I-, the base, with 12, the which give a violet color are saturated, those acid, to form Ia-.”lo Evidence of basic character which give brown colors are unsaturated. He in is to be seen in its union with aluminum stated that small additions of alcohol to a solution chloride, l1 sulfur dioxide12 and trinitrobenzene. l3 of iodine in chloroform suffice to shift the color Additional evidence in support of this hypothesis stepwise from violet to brown. Hildebrand and is to be found in the recent work of Fairbrotherl4 Glascock3 found that when iodine and an alcohol who reports that iodine has an abnormally high di- were both added to a “violet” solvent, bromoform electric polarization in the solvents dioxane, iso- or bromide, the molal lowering of the butylene, p-xylene and benzene. He concludes freezing point was considerably less than additive, that the high polarization of iodine in these solu- indicating combination of iodine with alcohol. tions is due to the presence of a solvent-I +I - com- Furthermore, they investigated colorimetrically plex. the equilibria of iodine with ethyl alcohol, ethyl In order to obtain more definite evidence re- acetate and nitrobenzene dissolved together in a garding this hypothesis, we first prepared solu- “violet” solvent such as carbon tetrachloride, tions of iodine of equal concentration in carbon tet- chloroform or carbon disulfide, and found in each rachloride, benzene, toluene, xylene and mesityl- case an equilibrium constant corresponding to a ene. Finding that the color shifted by visibly dis- 1 : 1 compound. They calculated the heat of com- tinct steps from violet to brown, we decided to bination in one case. There followed a long series trace their complete absorption curves. We of investigations of the general problem, well sum- found, to our surprise, that the shifts in the visible marized by Gmelin4 and in a recent review by portion of the spectrum are comparatively minor, Kleinberg and Davidson.6 But the original divi- but that in the ultraviolet region bands appear sion of iodine solutions into two or more distinct with extinction coefficients many times larger than color classes became untenable with the work of those of the visible bands. We present below the Waentig, Groh’ and \X7alkers which showed that complete absorption of such solutions between the position of the absorption bands of iodine solu- 270 and 700 mp, followed by our interpretation of tions in the visible region moved gradually from them. violet to brown, the shift being only small in the Apparatus and Procedure.-The absorption curves were case of benzene in which the color of iodine is a measured by means of a Cary Recording Quartz Spectro- photometer, Model 11, manufactured by the Applied red-violet. Physics Corporation of Pasadena. Extinction measure- We have long been curious about the chemical ments made with this instrument were reproducible to 1yo. basis for iodine solvates. It is not a question of As a check on the absolute values of the extinction, one dipole moment, as Walkers concluded, for we have of the absorption curves for iodine in carbon tetrachloride was redetermined using an independently calibrated Beck- recently shown rather conclusively that the iodine man Quartz spectrophotometer, Model DU. The agree- , which would be altered by solvation ment between the two sets of values was within the experi- effects, bears little or no relation to the dipole mo- mental error of the Cary spectrophotometer. ment of the solvent mole~ule.~The alcohols are Exploratory absorption measurements of the iodine extraordinary dipoles, and their effect is readily solutions were made using quartz cells ranging from 1 mm. to 10 cm. in length. A matched pair of 2-cm. quartz understandable, but the case of benzene seemed cells was used for most of the subsequent measurements. (1) E. Beckmann, Z. physik. Chem., 5, 76 (1889). The measurements were made by first filling the cells with (2) A. Lachman, THISJOURXAL, 25, 50 (1903). solvent and obtaining a “blank” tracing over the desired (3) J. H. Hildebrand and B. L. Glascock, ibid., 31, 26 (1909). spectral region. The solvent in one of the cells was then (4) “Gmelins Handbuch der anorganischen Chemie,” R. J. replaced by the iodine solution to be measured and a second Meyer, editor, System No. 8, pp. 111-129, eighth edition (Berlin, tracing obtained over the same region. The absolute 1933). (5) J. Kleinberg and A. W. Davidson, Chem. Reus., 42, 601 (1948). (IO) H. A. Benesi and J. H. Hildebrand, ibid., 70, 2832 (1948). (6) P. Waentig, 2. physik. Chem., 68, 513 (1909). (11) C. Friedel and J. Crafts, Compf.rend., 85, 74 (1877). (7) J. Groh, 2. anorg. allgem. Chem., 162, 287 (1927). (12) Mazzetti and De Carli, Gam chim. ifal., 58, 36 (1928). (8) 0. J. Walker, Trans. Faraday SOL.,S1, 1432 (1935). (13) Hepp, Ann., 216, 376 (1882). (9) H. A. Benesi and J. H. Hildebrand, THIS JOURNAL,70, 3978 (14) F. Fairbrother, Nature. 160, 87 (1947); J. Chem. Soc., 1051 (1948). (1948). 2704 H. A. BENESIAND J. H. HILDEBRAND Vol. 71 value of log &/I at any given wave length, could be ob- portions of concd. sulfuric acid, rinsed with distilled , tained directly from the difference in height of the two then shaken with three portions of 10% hydroxide tracings. The concentration of the iodine in the solutions solution, rinsed with water, and finally shaken with mer- studied was adjusted so that the maximum value of log cury. The product was dried over calcium chloride and Io/I lay between 1 and 2. distilled. In making up these solutions, a relatively concentrated Ethylidene chloride (1,l-dichloroethane) by Eastman solution was first prepared by weighing out 0.1 g. of iodine Kodak Company was purified by the method described in a glass-stoppered, 25-ml. volumetric flask and making previously.9 up to volume with the appropriate solvent. The final n-Heptane by California Chemical Company was very solution was then prepared by pipeting a portion of this pure as evidenced by comparing its , den- concentrated solution of iodine into a separate volumetric sity and boiling point with the recently compiled data on flask and making up to volume. When a binary mixture hydrocarbons.16 It was therefore used directly after a of solvents was wanted, a mixture of liquids in the desired simple distillation. proportion was substituted for the pure solvent in the last was kindly donated to us by Mr. Loyd Frashier. step. The volumetric apparatus was calibrated in the It had been treated with potassium permanganate and usual way by weighing the volume of water needed to fill potassium hydroxide and then distilled. Subsequently, the apparatus to the mark. All solutions were freshly it was kept in contact with potassium hydroxide in an prepared directly before making absorption measurements. evacuated system for two days, with shaking at frequent This was especially critical in cases where iodine gradually intervals, and then distilled at room temperature. The reacts with the solvent to form a permanent iodo com- product was fractionally distilled in the normal manner. pound. Materials.-Reagent grade iodine by General Chemical Data and Discussion Company was stored over phosphorus pentoxide in a desic- cator and used without further treatment. Iodine in Aromatic Hydrocarbons.-The re- All of the liquids listed below were distilled through a sults of our absorption measurements of iodine 24-in. Vigreux column as the final step in purification. in the aromatic hydrocarbon solvents are sum- The first and last portions were discarded and the middle marized in Table I. In Fig. 1 they are compared portion, boiling within a O.ao-range, collected in a dry, glass-stoppered flask. In all cases, the boiling points with the absorption curves of iodine in carbon tet- were within 0.2” of the values given in Lange’s “Hand- rachloride and diethyl ether, which we chose to book of Chemistry.” represent violet and brown solutions, respectively. Because of the diverse reports in the literature6 concern- The toluene and 0- and p-xylene curves, which are ing the color of solutions of iodine in benzene, special care was taken to obtain benzene of high purity. Thiophene- omitted to prevent over-crowding Fig. 1, would free benzene was fractionally crystallized three times, two have fallen stepwise between curves 3 and 4. The thirds of the benzene being collected on a Buchner funnel molar extinction coefficient, e, plotted in Fig. 1 is at each stage. During the final crystallization the tem- calculated from the relation perature of the mixturz of and liquid benzene re- mained constant to 0.01 , The wet benzene that was col- e = (log,, Io/I)lml (1) lected from the crystallization procedure was dried by dis- tillation and was kept over freshly prepared sodium wire where loglJo/l is the extinction of a layer of solu- in a glass-stoppered bottle. To see if the purification of tion 1 cm. deep containing m moles of iodine per benzene had any effect on the light absorption of its iodine solutions, two solutions of iodine were prepared using the TABLEI starting material and the final product as solvents. The ABSORPTIONOF IODINEIN AROMATICHYDROCARBONS absorption curves of these solutions were identical within [Ia] X 104 Log the experimental error of the measurements. Solvent moles per der IQ/I emax. Amax., UW Trifluoromethylbenzene (benzotrifluoride) , o-xylene, p-xylene, 1,3,5-trimethylbenzene (mesitylene), all by Visible Region Eastman Kodak Co., and toluene were purified by the Benzotrifluoride 7.50 1.31 870 512 following procedure. Each liquid was shaken with three 8.70 1.84 1060 Benzene 3.26” 1.64 1010 1 500 I :ccI. 6.91 1.45 1050 2 * C.H,CF, Toluene 16.48b 1.68 1020 497 8000 3 =&ti. 4 .C.YlCH,h o-Xylene 15.77b 1.67 1060 497 2.44 1080 495 v #-Xylene 11.30 2 5000 B 8.00 .-a, .* 1200 6 Mesitylene 9.20 2.211.88 117011200 490 9 2000 Ultraviolet Region 8 1000 : F1 0 0.696 1.36 9800 ’$ 800 800 3:: Benzene .163“ 0.79 9800 297 .9 ‘3 .326‘ 1.58 9700 u 600 i;; Toluene 1.648b 1.39 8400 306 500 o-Xylene 0.7& 0.66 8400 319 400 p-Xylene .904 1.34 7400 315 Mesitylene .920 1.53 333 200 200 8300 0 Measured in 5-cm. absorption cell. Measured in 1- 0 cm. absorption cell. All other measurements made using 2-cm. absorption cell. 280 350 450 550 Wave length, mp. (15) “Selected Values of Properties of Hydrocarbons,” Bureau of Standards Circular C461, Government Printing O5ce, Washington, Fig. 1.-Absorption of iodine in various solvents. 1947. Aug., 1949 SPECTROPHOTOMETRYOF IODINE WITH AROMATICHYDROCARBONS 2706 liter. The scale of the extinction coefficient has (3) been compressed tenfold between 1000 and 10,000 in the range 280400 mp. The values of the ex- where [c] = molar concentration of the complex, tinction coefficient and wave length at the absorp- 12.A,[I2] - [c] = molar concentration of free iodine, tion peaks are listed in columns 4 and 5 of Table I. and [A] - (c) = mole fraction of free aromatic hy- We call attention, first, to the peaks in the re- drocarbon, (c) in this term being expressed in gion, 280400 mp. We have assumed that these terms of mole fraction. Since [A] >> (c) we intense absorption peaks are characteristic of an replace [A]-(c) with [A]. The units of [c] and iodinearomatic hydrocarbon complex since these [I2]-[c] can be molarities because the concentra- bands do not appear in this region in the case of tions of these two substances will always be small violet solutions of iodine,.curve 1 in Fig. 1 being a in the solutions studied. In our experiments the typical example. Conclusive evidence for this as- original concentrations of the aromatic hydrocar- sumption will be given below. bon and the iodine are known. In order to deter- Second, the data in Table I show that the ab- mine K, however, we need to know more about sorption peaks in the 400-700 mp region are shifted [c]. We now assume that the intense absorption stepwise from curve 3 toward curve 5 as methyl bands in the ultraviolet region are due only to the groups are substituted for the atoms of presence of the iodine complex and that the ab- benzene, making it a better electron donor. On sorption of the free iodine is negligible in this the other hand, when a group like CF3-that re- region. The true molar extinction coefficient, E,, duces the electron in the ring-is substi- of the iodine complex at the wave length of maxi- tuted, the shift is less than in the case of benzene, mum absorption will then be given by the equation a result that was predicted from our hypothesis €0 = (log Ia/I)/[cIZ of acid-base interaction. (1)’ Third, the regular shifts in color, observed in the Thanks to our choice of units, we can eliminate aromatic hydrocarbon solutions with increase in [c] between equations (3) and (1)’, rearrange the the number of substituted methyl groups, are due resulting equation, and obtain the relation less to shifts in the main absorption band in the [Izll/log Io/I= KC) 1/[Al + 1/~o (4) visible region than to the increasing overlapping which is now in the form, y = mx + b. We have of the ultraviolet bands into the violet end of the made a tabular test of relation (4) in Table I1 for visible region. This explains why the color of the iodine-benzene and iodine-mesitylene equilib- mesitylene and ether solutions of iodine are almost ria at room temperature (22’) in the neutral identical even though their absorption peaks are solvents, carbon tetrachloride and n-heptane. The in quite different positions in the visible region. term on the left side of equation 4 has been desig- It should be noted that the values of emax. listed nated as y and is listed in the third column of Ta- in the lower section of Table I are not true molar ble 11. The values of e, were calculated from the extinction coefficients, for they are based upon the intercepts obtained when y is plotted against the concentration of iodine, not on the concentration reciprocal of the aromatic hydrocarbon concen- of the complex responsible for the existence of tration. A value of K was calculated for each set emax. Therefore, we know nothing thus far about of experimental measurements. the absolute or even the relative concentrations of According to the nomenclature listed under the complexes giving these ultraviolet absorpkion equation (3), K is related to the true thermody- bands. In order to obtain more information namic equilibrium constant by a proportionality about the iodine complexes, we added small, constant consisting of the ratio of the activity known amounts of benzene and mesitylene to coefficients of the various species entering the solutions of iodine in carbon tetrachloride. We equilibrium. Since the activity coefficient of again found the absorption peaks characteristic each of these species is undoubtedly different in of the corresponding iodine complexes in the ul- the two solvents it is not surprising that the K of traviolet region, whose extinctions were directly a particular system changes as the solvent is proportional to the benzene and mesitylene con- changed. We were able to calculate the activity centrations. Noting that the extinction of the coefficients of the iodine and the aromatic hydro- iodine complex in the case of pure benzene (see carbons from their “solubility parameters” by Table I) was directly proportional to the iodine means of the Van Laar-HildebrandScatchard concentration, we concluded that the following euuation equilibrium existed. V241Y61 - 62)Z I2 + A I- I2.A (2) log 72 = 2.303RT where A denotes an aromatic hydrocarbon. In This type of calculation is described el~ewhere.~ what follows we show how we obtained the quan- These values together with our equilibrium data titative information we sought by varying the allowed us to calculate the solubility parameter of aromatic hydrocarbon and iodine concentrations the iodine complex, which was found to be approx- over a wide range in a neutral solvent. imately the arithmetical mean of the iodine and The equilibrium constant, K,for the above re- aromatic hydrocarbon solubility parameters. In action is defined by the equation order to determine how much the value of K devi- 2706 H. A. BENESLAND J. H. HILDEBRAND Vol. 71

TABLEI1 only slightly from curve 1; hence, we may con- I*-BENZENE EQUILIBRIUMIN CARBON TETRACHLORIDE; clude that in the visible region the iodine complex

eo E 15,400 must have an absorption almost identical with (9) x lor, that of free iodine, most of the additional absorp- Val X [AI, cm-moles moles per liter mol. fr. per liter K tion in the former case arising from the over-lap- 3.26 1.000 10.29 1.73 ping of the ultraviolet bands. 6.96 0.924 10.58 1.73 AS an indirect test of our results, we have con- 10.42 .812 10.98 1.80 sidered the abnormally high solubJity of iodine in 10.42 ,619 12.59 1.74 benzene, 4.82 mole per cent. at 25O, reported by 17.40 .213 24.9 1.65 Hildebrand and Jenks.l6 The solubility calcu- 43.5 .0862 51.0 1.70 lated from their solubility parameters assuming 21.8 .0433 93.0 1.74 no interaction is approximately 2.5 mole per cent. The ratio of these two values is in reasonable Av. = 1.72 agreement with the ratio between total and un- Iz-C~H~Equilibrium in C7H16; e, = 18,000 solvated iodine calculated from the absorption 3.26 1.000 10.29 1.18 measurements, as stated above. 43.5 0.1252 43.6 1.18 Iodine in other Organic Solvents.-To make 21.8 .0643 78.4 1.19 sure that the intense absorption bands appearing 17.40 ,292 22.6 1.13 in solutions of iodine in aromatic hydrocarbons 24 1 .01312 398 1.08 were characteristic of the aromatic hydrocarbons 1081 .00254 2000 1.10 only, we measured absorption spectra of iodine in Av. = 1.15 diethyl ether, acetone, n-heptane, carbon tetra- chloride, carbon disulfide and 1,l-dichloroethane 12-CeH3(CH3)8 Equilibrium in CCl,; so = 9300 in the region from solvent absorption in the ultra- 9.20 1.000 12.02 7.2 violet to 700 mp. We found no absorption bands 49.5 0.0281 62.9 7.3 analogous to those of the iodine-aromatic hydro- 1597 ,0281 63.5 7.2 carbon complexes in the region 270-400 mp. Al- 99.0 .01398 121.6 7.0 though the absorption spectra of most of these io- Av. = 7.2 dine solutions have already been measured, we are summarizing our results in Table I11 for com- I~--C~Hs(CH&Equilibrium in C,HI6; eo = 9900 parison with the measurements of other investiga- 9.20 1.ooo 12.02 5.3 tions. All of the absorption curves are broad sym- 11.88 0.208 19.12 5.4 metrical peaks with a form similar to curve 1 in 39.6 .0420 56.4 5.2 Fig. 1. Therefore, only the values of Xmax, and Av. = 5.3 emax. for the absorption peaks are tabulated. ates from the thermodynamic equilibrium con- TABLE111 stant we then calculated all of the activity coef- This investigation Other investigations ficients entering into this type of equilibrium. Solvent Amax., mp e-x. Amax., mg emax. We found that the activity coefficient of the com- ( CBH~a0 462 880 456' 1030' plex is largely canceled by the product of the ac- (CHdiCO 363 6100 46017 45017 tivity coefficients of the iodine and aromatic hy- C7H;e 520 910 a. ... drocarbon, the degree of cancellation depending cc14 517 930 51g8 9008 on the solvent used. Our values of K are there- Cs1 518 1120 518' 1170' fore the same order of magnitude as the thermo- CHICHCli 503 870 *. ... dynamic equilibrium constant. It is evident from Table I11 that the absorption The data listed in Table I1 have supplied us with spectrum of iodine in acetone is very unusual. the following important results. First, our The absorption peak appears in the ultraviolet measurements confirm the earlier evidence that region and the value of emax. is of a higher order of the iodine complex consists of one of io- magnitude than those of the other solutions listed dine bound to one molecule of aromatic hydrocar- in Table 111. The absence of an absorption peak bon. Second, the iodine-mesitylene complex is in the visible region shows that the absorption is more stable than the iodine-benzene complex. not of the type encountered in the case of the More specifically, in a solution of iodine in pure aromatic hydrocarbons. The large discrepancy benzene at room temperature, about 60 mole per between our values for Lax. and emax and those of cent. of the iodine is tied up as an iodine-benzene Getman" may possibly be attributed to the well complex; in a mesitylene solution of iodine, 85 known reaction of iodine with acetone to form the mole per cent. of the iodine is bound to mesitylene. a-iodo-derivatives. Our acetone was purified These quantitative results place our hypothesis of very carefully and the absorption spectrum of acid-base interaction on a much firmer basis. the iodine solution remained unchanged for sev- Although our results show that in benzene and (16) J. H. Hildebrand and C. A. Jenks, THISJOURNAL, 42, 2180 mesitylene solution most of the iodine is in the (1920). form of a complex, curves 3 and 4 of Fig. 1 differ (17) F. H. Getman, ibid., SO, 2883 (lQ28). Aug., 1949 SODIUMIODIDE AND PHASESEPARATION IN SODIUM- 2707 era1 hours. However, the value of emax. of iodine in above. With the exception of iodine in trifluoro- unpurified acetone dropped rapidly, two-thirds of methylbenzene, each of the aromatic hydrocarbon the iodine having reacted in fifteen minutes. We solutions had an intense absorption band in the suggest, therefore, that Getman had not purified ultraviolet region which we have shown to be char- his acetone sufficiently to remove the impurity acteristic of a complex containing one iodine and that catalyzes the reaction between iodine and one aromatic hydrocarbon molecule. acetone. The equilibrium between iodine and the aro- Acknowledgment.-We wish to express our matic hydrocarbons has been investigated in the appreciation to the Office of Naval Research neutral solvents, carbon tetrachloride and n-hep- for financial support of this research, and to the tane, and the results show that the iodine-mesi- American Chemical Society for the post-doc- tylene complex is more stable than the iodine- toral fellowship held by the junior author during benzene complex. These findings are strong evi- part of the period spent upon this research. dence for an acid-base interaction between iodine and aromatic hydrocarbons. S-arY Absorption measurements have also been made The absorption spectra of iodine in trifluoro- of iodine in carbon tetrachloride, carbon disulfide, methylbenzene, benzene, toluene, 0- and #-xylene n-heptane, ethyl ether, acetone and 1,l-dichloro- and mesitylene have been measured in the region ethane. No absorption bands analogous to those 270-700 mp. In the visible region, the absorption of the aromatic hydrocarbon solutions were found peaks of these solutions showed moderate shifts in the region 270400 mp. toward shorter wave lengths in the order listed BERKELEY4, CALIF. RECEIVEDFEBRUARY 23, 1949

[CONTRIBUTION FROM THE BAKERLABORATORY OF CHEMISTRY, CORNELL UNIVERSITY] Effect of Sodium oh the Phase Separation in the System Sodium-Ammonia BY M. J. SIENKO Kraus' has shown that solutions of sodium in mined as a function of decreasing temperature. liquid ammonia separate into two liquid phases The discontinuity in the slope of the resistance- which have an upper critical temperature of temperature curve corresponds to the temperature -41.6°.2 Similar behavior is observed in lithium at which phase separation occurs. and potassium solution^.^ In a report prepared for the Office of Naval Research Ogg suggests4 Experimental Procedure that the separation of these alkali metal-liquid The conductance cell is shown in Fig. 1. M indicates a thin-walled capillary of 1.5 mm. inner diameter across ammonia solutions into two liquid phases that are which the resistance is measured by means of tungsten both dziute solutions of metal in ammonia indi- electrodes in mercury-filled wells K and L. In order to cates an origin for the phase separation different check the apparatus and the possibility that the substitu- from that of other liquid phase separations, such tion of tungsten electrodes for platinum electrodes may as that in the system water-phenol, where one of have an effect on the temperature of phase separation, solu- tions were also prepared without any sodium iodide. The the conjugate solutions is rich in one component observed temperatures of phase separation were in excel- and the other, rich in the other component. The lent agreement with the results reported by Kraus and present investigation was undertaken to deter- Lucasse . The solutions were prepared by introducing into arm H mine the effect of a dissolved , sodium iodide, 0.50 ml. of an aqueous solution of sodium iodide (contain- on the phase separation in the system sodium- ing 0.52 millimole per ml. of solution) from a graduated ammonia and to determine the distribution of so- 1-ml. pipet. With stopcocks G closed and F open, the dium iodide between the two phases. Sodium io- solution was rinsed down into the cell with a few ml. of dide was selected since it is sensibly inert with re- distilled water. H was sealed and the water pumped off by gradual evacuation of the cell through A. The sodium spect to the two components of the system and iodide deposited in the capillary was degassed for twenty- has an appreciable solubility even in the concen- four hours at a pressure of 5 X mm. and a tempera- trated solutions. ture of about 80". Ammonia, stored over sodium in B, was allowed to diffuse through the cell while H was opened The temperature of phase separation for the and a section of glass tubing containing approximately the system sodium-ammonia in the presence of so- desired weight of sodium was introduced. H was re- dium iodide was investigated by the method of sealed and the cell re-evacuated and degassed for another Kraus and LucasseI2in which the resistance of a twenty-four hours. Heat was subsequently supplied given solution of sodium in ammonia was deter- from a spiral heater around H to just melt the sodium which flows through constriction J into the cell. (Experi- (1) C.A. Kraus, THISJOURNAL, 89, 1565 (1907) ments in which sodium was actually distilled into the cell (2) C. A. Kraus and W.W. Lucasse, ibid., 44, 1949 (1922). from a horizontal arm H without constriction J proved to (3) D. Loemer, M. J. Sienko and R. A. Ogg, Jr., unpublished. be rather lengthy and did not affect the reproducibility of (4) R. A. Ogg, Jr., mimeographed report dated at Stanford Uni- the final results.) J was heated with the tip of an versity on April 11, 1947. flame and H pulled off. Copper wires were introduced