Differential scanning calorimetry study of fluoride complexes of germanium, tungsten, uranium, lithium and gallium

Differential scanning calorimetry study of fluoride complexes of germanium, tungsten, uranium, lithium and gallium

Therraochiraica Act., 29 (1979) 147-155 O Elsevier Scientific Publishing C o m p a n y , A m s t e r d a m - Printed in T h e Netherlands DIFFERENTIA...

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Therraochiraica Act., 29 (1979) 147-155 O Elsevier Scientific Publishing C o m p a n y , A m s t e r d a m - Printed in T h e Netherlands

DIFFERENTIAL SCANNING CALORIMETRY STUDY OF FLUORIDE COMPLEXES OF GERMANIUM, TUNGSTEN, URANIUM, LITHIUM AND GALLIUM

AKIICHI KIGOSHI Research Institute o f Mineral Dressing and Metallurgy, Tohoku University, Sendal 980 (Japan)

(Received 9 March 1978)

ABSTRACT

The enthalpy and temperature of the sublimation, transition and dissociation o f nitrosyl fluoride-germanium, tungsten, uranium, lithium and gallium fluoride a d d u c t s were determined from D S C measurements. A closed-cell D S C technique was employed for this purpose and to postulate possible reaction mechanisms of the dissociation. INTRODUCTION

A series of the D S C measurements for the adducts o f acceptor fluorides with nitrosyl or nitryl fluorides 1-3 was extended to those o f the other five elements. It is k n o w n that the fluorides of germanium*, tungsten* and uranium* produce adducts with nitrosyl fluoride. The chemical formation of these reactions is as follows Ge + 5 N O F --,, N O G e F s + 4 N O W + 7 N O F --* N O W F 7 + 6 N O U+6NOF~NOUF6 +5NO

(1) (2) (3)

I t is probable that the fluorides of lithium and gallium also produce the fluoride complexes according to the following reactions 5 Li + 7 N O F --* (NO)2LisF7 + 5 N O 2 G a + 9 N O F ~ (NO)3Ga2F 9 + 6 N O

(4) (5)

MATERIALS AND EXPERIMENTAL

The fluoride complexes, N O G e F ~ , NOWFT, N O U F 6 , (NO)zLisF7 and (NO)3Ga2F 9 were prepared and analyzed as follows. The guaranteed metallic germanium was added little by little to the 80 mole ~o H F - 2 0 mole ~o NO2 solvent until the solution was almost saturated. After a violent reaction, colourless, transparent, needle-shaped crystals precipitated from the solution on cooling to --20°12. These crystals were separate d centrifugally from the solution. The same method was

14g applied to prepare N O W F v , t h o u g h a slight evacuation at r o o m t e m p e r a t u r e was necessary to eliminate the solvent adsorbed on the crystal surface. I n the case o f N O U F 6, the 80 mole % H F - 2 0 moIe % N O 2 solvent was a d d e d to metallic u r a n i u m in a reaction tube m a d e o f K e l - F plastic. The reaction tube was kept at r o o m temperature until all the metal h a d reacted satisfactorily. A whitish blue c o m p o u n d was obtained o n separating the solution centrifugally. I n this case, the atmosphere for all these treatments must be free from moisture as completely as possible, because the moisture, even a very small a m o u n t , reacts with N O U F ~ to p r o d u c e U F 4 which causes inevitable errors in the D S C m e a s u r e m e n t s for N O U F ~ . Since the 80 mole ~o H F - 2 0 mole Yo N O 2 solvent itself is hygroscopic, its addition to the metal was d o n e in a distillating m a n n e r in a d o s e d system. T h e X-ray diffraction p attern o f this whitish blue c o m p o u n d coincided with that o f N O U F 6 wh ich is listed o n the A S T M cards 5. I n the case o f ( N O ) 2 L i s F 7, the 80 mole ~o H F - 2 0 mole ~o N O z solvent was a d d e d to lithium c ar bona t e until the reaction was complete. A white precipitate was deposited by cooling the supernatant solution to --20°C. This precipitate was ~ p a r a t e d centrifugally from the solution, a n d was evacuated at --20 °C to eliminate the solvent a d s o r b e d o n the particle surface. I n the case o f (NO)3GazFg, a slight excess o f 80 mole ~o H F - 2 0 mole ~o N O z solvent was a d d e d little by little to the g u a r a n t e e d reagent metallic gallium. The sticky solution obtained was evacuated at 0 °C to constant weight. After this procedure, a colourless crystal o f gallium fluoride complex was obtained. All these c o m p o u n d s were analyzed for metal ion, fluorine a n d nitrogen. T h e quantitative analyses o f fluorine a n d nitrogen were p erfo rmed as previously described 6. Th e cont e nt o f g e r m a n i u m in the g e r m a n i u m fluoride complex was determined f r o m the constant weight which was attained by evacuating the solution o f a definite a m o u n t o f g e r m a n i u m in the 80 mole Yo H F - 2 0 mole 7o NO2 solvent at --10°C. It was confirmed b e f o r e h a n d t h a t the D S C curve for this sample coincided satisfactorily with that for N O G e F 5 previously prepared. The quantitative anaIysis o f tungsten was performed by weighing the tungstic acid anhydride which was precipitated from the aqueous solution o f N O W F 7 with hydrochloric acid. T h e a m o u n t o f u r a n i u m in N O U F 6 was determined by weighing the triuranium octoxide p r o d u c e d by igniting the a m m o n i u m ura na t e which was precipitated from the Uranyl solution. T h e a m o u n t o f lithium was d e t e r m i n e d by atomic-absorption sp ectro p h o to metry using a Hitachi M o d e l 208 atomic-absorption spectrophotometer. T h e co n ten t o f gallium was calculated f r o m the a m o u n t o f gallium used a n d the weight o f gallium c o m p o u n d obtained. These results are shown in Table 1. T h e reaction enthalpies a n d temperatures were determined using a RigakuD e n k i M o d e l DSC-8055 differential scanning calorimeter. T h e same m e t h o d s w e r e used as those whi c h have previously been described I -~. T h e D S C c h a m b e r was first evacuated a n d then filled with nitrogen. The evacuation was p erfo rmed at --20 °C for g e r m a n i u m a n d lithium, a n d at - - 1 0 ° C for gallium because their c o m p o u n d s were to be subjected to dissociation or sublimation at a higher temperature. D u r i n g each m e a s u r e m e n t nitrogen was allowed to flow t h r o u g h the sample c h a m b e r at a rate o f

149 TABLE 1 COMPOSITION OF SAMPLE

Found (%)

Calculated (%)

NOGeFs

Ge F N

37.04 47.53 7.13

36.74 48.08 7.09

NOWF7

W F N

52.90 37.44 3.98

53.01 38.34 4.04

NOUF6

U F N

62.38 29.56 3.45

62.31 29.84 3.67

(NO)zLi~F7

Li F N

15.26 58.57 12.16

15.24 58.41 12.30

(NO)aGaeF0

Ga F N

34.92 42.10 10.03

34.82 42.70 10.49

30 ml min - I . 2 to 40 mg o f the sample was employed at a heating rate of 5 or 10°C rain-x. A fiat cylindrical closed cell with a pin-hole o n its surface was used. Cells made o f aluminum were used in the cases o f tungsten and lithium. I n the other cases, platinum cells were needed because the reaction between the aluminum cell and the sample was not negligibly small. The reaction temperature and the peak area o f each DSC curve were measured by the same m e t h o d as described previously a. RESULTS AND DISCUSSION

The DSC curve for the germanium fluoride complex is given in Fig. 1 (curve A). As shown in the figure, NOGeF5 sublimates simply without transition, melting or preceeding dissociation, which were observed for many fluoride complexes. The behaviour o f NOGeF5 was similar to that o f (NO)~SiF 2, NOPF~ and NOVF~, as described previously. The enthalpy a n d temperature o f sublimation estimated from the DSC curve are listed in Table 2. The DSC curve for the tungsten fluoride complex is given in Fig. 1 (curve B). As shown in this figure, two small peaks were observed before a decisive large peak, similar to the case o f NOSbF~. The former two p e a k s were entirely reversible, a n d neither weight changes nor melting reactions were observed with the peaks. Therefore, it is clear that these peaks originate from the transition o f the crystal lattice. At the higher temperature sublimation o f this material was observed. The enthalpies a n d

150

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(B) T

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200

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v

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300

v

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400

(= C )

F i g . 1- D S C c u r v e f o r 1NOGcF5 ( A ) and N O W F ~ (B).

TABLE 2 REACTIONENTHALpIESFOR NOGeFs AND NOWFv

Reaction

Temp. ( °C)

A H ( kcal mole-Z)

N O G e F s , sublimation N O W F T , transition

185 88 260 346

36.47 1.20 2.92 21,84

transition sublimation

-i'<3 IJ

E

(la J~ -o( j C [iJ

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200

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v-

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1

300

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Fig. 2. D S C curve for N O U F 0 .

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151 TABLE 3 REACTION ENTHALPIES FOR NOUF6 AND (NO)2LisF7

Reaction

Temp. (°C)

A ft(kcal mole.-1)

NOUFo, transition sublimation (NO)zLisF7 ~ 5 LiF -t- 2 NOF

252 397 143

1.886 25.80 29.80(per mole of NOF)

temperatures o f transitions a n d sublimation estimated from the D S C curve are listed in Table 2. T h e D S C curve for the u r a n i u m fluoride complex is given in Fig. 2. As s h o w n in the figure, there was a sharp peak before a decisive large one. W i t h the former peak, neither a weight change n o r a ny other reactions were observed except for the reversible change in colour of whitish blue to d a r k blue. Therefore, it is clear that this p e a k originates from the transition o f the crystal lattice. A t the higher temperature, which c o r r e s p o n d e d to the last peak o f the D S C curve, sublimation o f this material was observed. T h e enthalpies a n d temperatures o f transition a n d sublimation estimated f r o m the D S C curve are listed in Table 3. As previously described, every sublimation p h e n o m e n o n for the a d d u c t o f N O F - a c c e p t o r fluoride was simple; that is, in these cases a deposit which was f o r m e d by the sublimation a n d following c o n d e n s a t i o n was confirmed to be the same material as the original 1. However, in the present case the d eco mp o s itio n o f N O U F 6 subseq u e n t to the sublimation m u s t be t a ke n into account. A d a r k green deposit was f o u n d a r o u n d the platinum cell after every D S C measurement. I n m o s t cases the same deposit was also f o u n d in the cell t h o u g h the a m o u n t was very small. I n general, a small a m o u n t o f light green fine p o w d e r coexisted with these deposits. This light green p r o d u c t w a s c onc l ude d to be U F 4 which was f o r m e d by decomposition o f the dendritic N O U F 6 , as described later. T h e m e a n values o f chemical analysis o f these materials were in g o o d agreement with the c o m p o s i t i o n o f U F 4 as follows: U : found, 75.26 ~o, calculated, 75.807o; F: found, 24.51 ~o, calculated, 24.20 ~o- It is suggested f r o m this fact that N O U F 6 d e c o m p o s e d in the v a p o u r phase as the following reaction, w h e n the v a p o u r was diluted by the nitrogen atmosphere. 2 N O U F 6 --* U F 4 + U F 6 -t- 2 N O F

(6)

This suggestion c ou l d be justified f r o m the fact that the weight o f the deposit r a k e d up after each D S C m e a s u r e m e n t was close to that o f U F 4 calculated from eqn. (6), as s h o w n in Table 4. I n mid-course o f the sublimation o f N O U F 6 , whitish blue dendrites were observed mixed in with the d a r k green deposit. T h e m e a n chemical c o m p o s i t i o n o f these materials was as follows: U, 73.31 ~o; F, 2 5 . 2 4 ~ ; N , 0 . 6 8 ~ . These values c o r r e s p o n d to 81.43 a n d 18.57 ~o o f U F 4 a n d N O U F 6, respectively, a n d the existence o f whitish blue dendrite in the deposit endorses the latter. T h e dendrite seems to be

152 TABLE 4 COMPARISON OF AMOUNT OF LrF4 FOUND AND CALCULATED

NOUF6 (rag)

Found (rag)

Calculated (rag)

1.99 12.19 12~1 13.65 13.90 12.17 14.90 15.16

1.93 11.86 12.49 12.91 13.58 13.66 13.98 15.25

4-69 28.85 30.40 31.41 33.03 33.25 34.01 37.11

f o r m e d by the c o n d e n s a t i o n o f some parts of the N O U F 6 v a p o u r or the recombination o f U F 4 , U F 6 a n d N O F . T h e existence o f the dendrite in mid-course o f the sublimation c oul d a c c o u n t for that o f the light green c o m p o u n d which was fo u n d mixed with the d a r k green deposit at the end o f the D S C measurement. The D S C curve for the fluoride c o m p l e x o f lithium is given in Fig. 3. As s h o w n in the figure, there was only one decisive p e a k different from the cases o f tungsten a n d uranium. With the reaction which causes this peak, a weight decrease of 43.07 ~o was observed_ This value is in g o o d a g r e e m e n t with the decrease in weight, 43.04 ~o, w h ere 2 moles o f N O F per 1 mole o f ( N O ) z L i s F 7 are evolved, leaving 5 moles o f LiF. T h e results o f the chemical analysis o f the solid p r o d u c t were f o u n d to be also in close

"z-

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-Temperature

F i g - 3- D S C c u r v e f o r ( N O ) e L i a F T .

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(°C)

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20o Temperature

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(" C )

Fig. 4- DSC curve for (NO)zGa2F9 (1) and (NO)zGaaFxl (ID.

agreement with the composition o f LiF. These facts indicate that the peak originated from the following reaction (NO)zLisF7 --~ 5 LiF + 2 N O F

(7)

The enthalpies and temperatures estimated from the DSC curve are listed in Table 3. A typical DSC curve for the gallium fluoride complex is given in Fig. 4 (curve I). The existence o f three dissociation reactions must be considered for (NO)aGa2F9With the reaction which causes the first peak (A), a weight decrease o f 12.35 ~o was observed. This value is close to the decrease in weight, 12.24~o, for the reaction where 1 mole of N O F dissociates per 1 mole o f (NO)aGa2Fg, leaving 2 moles o f N O G a F 4 . This indicates that the peak (A) was derived from eqn. (8). ( N O ) a G a F 9 --~ 2 N O G a F 4 + N O F

(8)

The decrease in weight o f 27.59~o was observed by the reaction which causes the second peak (B). This value is close to that o f the decrease in weight, 27.89 ~o, where 1 mole of N O F per 1 mole o f N O G a F 4 is evolved, leaving 1 mole o f G a F 3. However, it is suggested from the shape that the p e a k (B) is derived from two overlapping reactions. The material o f a definite composition was obtained with a weight decrease o f 9.14 ~ by heating the N O G a F 4 at !50 °C in the platinum cell for almost I h. This value is close to that o f the decrease in weight, 9.30~o, where 1 mole o f N O F per 3 moles o f N O G a F 4 is evolved, leaving 1 mole o f (NO)2GaaF1 t- T h e D S C curve for the material which was produced by this heating is also shown in Fig. 4 (curve II). The decrease in weight o f 20.31 ~ was observed by the reaction which causes the peak. This value is close to that o f the decrease in weight, 20.47 ~o, where 2 moles o f N O F per 1 mole o f

154 TABLE 5 REACTION ENTHALPIES ]FOR

(NO)aGasF9

Reaction

Temp. (°C)

A H (kcal per mole o f NO F )

(NO)aGasF9 --* 2 NOGaF4 + NOF 3 NOGaF4 --~ (NO)sGaaFll + NOF (NO)zGaaFxx --* 3 GaFz + 2 NOF

67 150 202

14.95 27.23 23.40

(NO)2Ga3F11 is evolved, leaving 3 moles o f G a F 3. The gallium content in the final product calculated from the decrease in weight was 55.03 Yo. This value and the result o f chemical analysis o n fluorine were close to the composition o f GaFa as follows: Ga: calculated, 55.02~o; F: found, 44.67 ~o, calculated, 44.98 ~o. T h e n , the peak (Bl), which is derived from the following dissociation reaction alone, was obtained by subtracting the peak in curve II from the peak (B) in curve I 3 N O G a F , ~ (NO)2Ga3F11 + N O F

(9)

Needless to say, the following reaction causes the peak in curve II ( N O ) 2 G a a F I t -~ 3 GaF3 + 2 N O F

(10)

The enthalpies a n d temperatures for reactions (8), (9) a n d (10) estimated from the D S C curves are listed in Table 5. CONCLUSION Adducts o f nitrosyl fluoride with fluorides o f germanium, tungsten, uranium, lithium a n d gallium were p r o d u c e d using 80 mole ~o H F - 2 0 mole ~o NO2 solvent. The following facts were found from the D S C measurements o f these adducts. (NO)zLisF7 is converted into LiF t h r o u g h one thermal dissociation step. Three thermal dissociation steps are observed for the reaction o f ( N O ) z G a z F 9 to the final form o f GaF3. N O G e F s sublimates without preceding reaction, b u t in the cases o f N O W F 7 a n d N O U F 6 one a n d two transitions are observed, respectively, prior to their sublimation. The enthalpies a n d temperatures o f all these reactions were estimated from the D S C curves. ACKNOWLEDGEMENTS

The author wishes to acknowledge Mr. Mitsuo Ohmi's help in chemical treatments o f the adducts, Mrs. Mitsue Ohhashi's assistance in the experiments a n d the translation o f the manuscript, and Mr. N o b u a k i Sato's effort in preparing the u r a n i u m fluoride adduct a n d its X-ray diffractometry.

• 155

REFERENCES 1 2 3 4 5 6

A . Kigoshi, Thermochim. Acta, 11 (1975) 35. A. Kigoshi, Thermochim. ,4cta, 12 (1975) 179. A. Kigoshl, Thermoehim. ,4eta, 16 (1976) 355. F- Seel, Angew. Chem., 77 (1965) 689. F . J . Musil, P. R. Ogle and K. E. Beu, GAT-T-533, Goodyear Atomic Corp., 1958; A S T M 11-246. A. Kigoshi and M. Ohmi, Sci. Rep. Res. Inst. Tohoku Univ. Set. ,4, 25 (1974) 14.