Disproportionation Equilibria and Rates in Perchloric and Hydrochloric

The data of Kasha and Sheline on rates aiid equilibria of the disproportionation reaction of plutoniuin(1V) to give plu- tonium(II1) and plutonium(V1)...
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Vol. 75

[CONTRIBUTION FROM T I E ~)EPARTMENT OF C H E M I S r R Y AND CHEMICAL ENGINEERING, AND UNIVERSITY O F CALIFORNIA, BERKELEY ]

RADIATION LABORATORY,

Disproportionation Equilibria and Rates in Perchloric and Hydrochloric Acid Solutions of Plutonium : Influence of a-Particles BY ROBERTE. CONNICK AND WILLIAM H. MCVEY RECEIVED MAY5, 1952 The data of Kasha and Sheline on rates aiid equilibria of the disproportionation reaction of plutoniuin(1V) to give plutonium(II1) and plutonium(V1) have been corrected for the reduction caused by the plutonium a-particles. I t was necessary to assume reaction paths for the a-particle-induced reduction, and one-electron reductions of Pu(V1) and Pu( IV) were chosen as most plausible. The disproportionation mechanism was found to be consistent with that previously deduced from the disproportionation of plutonium( V). The equilibrium for the disproportionation of plutonium(1V) exhibited approximately the expected fourth power dependence on hydrogen ion concentration in perchloric acid a t unit ionic strength and 25’. An apparent fifth.power dependence was obtained for hydrochloric acid solutions, not at constant ionic strength. The disproportionaton rate showed an inverse third power acid dependence in perchloric acid a t constant ionic strength and an apparent-3.5 power dependence in hydrochloric acid solutions, without added salt. Approximate values of 40 kcal. and f 6 0 e x . were calculated for the heat and entropy of activation of the disproportionation reaction in onemolar hydrochloric acid. The formal potentials of the Pu(II1)-Pu(V1) and Pu(1V)-Pu(V1) couples in one molar perchloric acid a t 25” are -1.043 2~ 0.003 and -1.022 =t0.002 volt, respectively. Thc corresponding values for one molar hydrochloric acid are -1.053 0.003 and -1.025 rt 0.002 volt. The discrepancy concerning chloride complexing of PuOz++ is nearly eliminated by the new values for the disproportionation equilibrium quotient. It is pointed out that the assumption of a small amount of complexing of P u f a by chloride ion would give complete agreement and evidence is advanced in support of this hypothesis.

*

htroduction.-Attention1** has been called to a discrepancy between the observed properties of plutonium(V1) with chloride ion and that calculated from e.m.f. and disproportionation equilibrium measurements. Spectral observations show plutonyl ion, PuOz++, to be appreciably complexed in one molar hydrochloric acid.3 The e.m.f. and equilibrium results indicate the unlikely result that plutonyl ion is more strongly complexed by perchlorate than by chloride ion.. The source of the discrepancy has been traced to an error in the equilibrium quotient for the reaction 3Puf4

+ 2Hz0 = ~ P u ++ PuOz++ ~ + 4H+

(1)

The average oxidation number of plutonium in a solution containing these species slowly decreases with time. The a-particles, from the disintegration of plutonium, in their passage through the solution produce species which bring about the red ~ c t i o n . ~When the rate of reduction by the CYparticle radiation becomes of the same order of magnitude as the rate of attainment of the disproportionation equilibrium of equation (l), then true equilibrium will not be established. The results of the calculations of this paper show that this correction is much more important than was previously suspected and that the apparent equilibrium quotients were seriously in error. Extensive measurements of the rate of reaction arid the equilibriuni quotient for reaction ( 1 ) in j~erchloric~ and hydrochloricb acids have been made by Kasha and Sheline. They studied the reaction as a function of acidity at 25” and obtained limited data on the effect of ionic strength and tcmperature. I n some cases “equilibrium” was approached from both sides. These data serve as the basis for the calculations presented here. (1) R. 13. Connick a n d W. II. hlcViey, T H I S. l o u n N ~ v . , 73, 17118 (1951). ( 2 ) R. E. Connick and W. H. I I c V e y , ibid., 74, 1311 ( 1 9 5 2 ) . (3) R. E. Connick, hl. Kasha. W. H. McVey a n d G. E. Sheline, “ T h e Transuranium Elements.” National Nuclear Energy Series, n i v i sinn IV, Vol. 11B, AlcCraw-Hill Book Co., E x . , N e n Y w k , N. \’., 1949, p. 659. Hereafter this bonk will be designated as 1. (1) h l . Kasha, ibid., p. 295. ( 5 ) A I . K a s h a a n d G. E. Sheline, ibid., p. 180.

Method.-For each experiment the rate and equilibrium quotient were obtained by a graphical method. In order to apply the method, rate laws for both the disproportionation reaction and the reduction reaction, arising from the a-particles, must be assumed. The correctness of the former is tested by the linearity of the resulting plot. I t has been shown6 .that there are only two plausible mechanisms for the oxidation-reduction reactions between plutonium ions in acidic s o h tions. According to available experimental data6 the one by which such reactions actually occur is I’u(1V)

+ Pu(1V)

* Rl

Pu(V)

+ Pu(II1)

(2)

Pu(II1)

+ Pu(V1)

(3)

ki

Pu(1V)

+ PU(V)

ki k4

Reaction (3) is a rapid equilibrium’ while reaction (2) is rate determining. The equilibrium quotient for the disproportionation reaction, with the hydrogen ion dependence omitted, and for reaction (3) are defined as K. = ( I I I ) ~ v I ) / ( I V ) ~ Kb .= (III)(vI)/(Iv)(v)

(4) (5)

wlierc parentheses indicate the molar concentration, Le., xnoles per liter of solution, of the enclosed plutonium species. Nothing is known experimentally about the mechanism of the reduction induced by a-particles. I t is not possible to analyze the data without knowledge of this mechanism. Fortunately, one can make a plausible choice. A survey8 of the oxidationreduction chemistry of plutonium shows that the P u + ~ - - P ucouple + ~ and the PuOz+-Pu02++ couple are highly reversible in such reactions. On the contrary the Pu+4-PuOz+ couple is very irreversible. This behavior is explained by the fact that only an electron transfer occurs in reactions of the ( 6 ) R E. Connick, i b i d . , p. 268; THISJOURNAL, 71, 1528 (1949). ( 7 ) R I? Connick, X.1. Kasha, W. I€. h‘LcVey and G. E. Sheline. I, I,. ’27. ( 8 ) R. IS. Cunnick, U. S. Atomic Energy Couimission report CC3869, July 6, 1948.

475

DISPROPORTIONATION EQUILIBRIUM OP PLUTONIUM (IV)

Jan. 20, 1953

former two couples, but bonds must be formed or broken along with the electron transfer in the case of the P U + ~ P U Ocouple. ~+ It therefore seems safe to conclude that the net effect of the chemical species produced in the solution by a-particle radiation will be to reduce Pu+' to P u + ~ and PuOz*+ to P u O ~ + . We ~ may then write

+ Pa + Pu(V) kaz Pu(IV) + Pa + Pu(III)

Equations (12), (13) and (14) can then be written as

kal

Pu(V1)

(6)

(7)

All of the quantities in the above expressions, exwhere Pa indicates species produced by the a-par- cept kl and K., can be obtained readily from the ticles. The symbols Ral and Raz will be used for data of Kasha and Sheline. The rates were deterthe rates of reduction of plutonium in the respec- mined from slopes of plots of the concentrations of the various species versus time. The'average oxidative reactions. From equations ( 2 ) , (3), (6) and (7), the following tion number, which was used to evaluate Rm, was rate laws are obtained where R1,Rz, R3 and RI rep- calculated by the equationb resent the rates of the two forward and reverse 3(III) 4(IV) + 5(V) + 6(VI) average oxid. no. = steps of equations (2) and (3) (111) (IV) (vmvr

+

-

+

-

d(VI)/dt = Rs Rc RUI d(V)/dt = RI - Rz - R3 Rc Rai d(IV)/dt = 2R1 2112 - R3 14 Rm d(III)/dt Rr - Ro Ra Rc Raz

+

-

+

+ + + + - +

(8) (9) (10)

(11)

Because the concentration of Pu(V), and therefore d(V)/dt, was small in most of the experiments, equation (9) was combined with each of the others to give (12)

d(III) + dt

dt

= 2111

- 2x1 + Rei

+ Raz

(14)

Experimentally4p5it is found that, for a given set of conditions, the a-particles produce a constant rate of decrease of the average oxidation number of the plutonium. Therefore, in a single experiment the sum of Ra1 and Ra2 is a constant which will be denoted as Ra. It is equal to the rate of decrease of the average oxidation number multiplied by the total plutonium concentration. The rates Rl and Rz can be expressed in terms of the corresponding rate laws according to the mechanism of reaction ( 2 ) Ri

- RI

ki(IV)t

- k1(III)(V)

Substituting for the concentration of Pu(V) from equation ( 5 ) , which represents the rapid equilibrium of reaction (3), gives -4 -6

From the equality of the forward and back reactions a t equilibrium it can be shown that Ks = kiki/kck, = Kbki/kz

Therefore .

.

(9) It is interesting to note that hydrogen peroxide, which is probably one of the species produced by the a-particles, is known to reduce Pu(V1) to Pu(V) and Pu(1V) to Pu(II1) at a considerably greater rate than it reduces Pu(V) (R. E. Connick and W. H. McVey, ref. 8. p.

97ff.).

+

A plot of the left sides of equations (15), (16) and (17) as ordinate versus (III)2(VI)/(IV)3 as abscissa should give a single straight line whose intercept on the ordinate axis is k1 and on the abscissa axis is K.. It is easily shown that, if the rate law assumed in equations (2) and (3) is incorrect, a straight line will not be obtained and kl would of course have no meaning. However, the point a t which the curve crosses the abscissa axis would still give the equilibrium value of K.. Results.-Typical plots are shown in Figs. 1, 2 and 3, where, for convenience, the ordinate is actually the left side of equation (15), (16) or (17) multiplied by 0.01 times the total plutonium concentration. In the first two experiments the equilibrium of equation (1) was approached from the P u + ~ side, i.e., by disproportionation; in the third, by reproportionation. It is clear from the scatter of the points that no great accuracy can be claimed for the data.

t I

1 2 3 4 5 ( I I I ) ~ ~ v I ) / ( IxV )102. ~ Vig. 1 .--Equilibrium a n d rate of disproportionation of plutonium(1V) in 0.W4 .If perchloric acid at 35". 'IF" is the value of the left side of equation 15, 16 or 17, multiplied by 0.01 times the total plutonium concentration. The symbols 0 , O and 0 refer to Pu(III), Pu(1V) and Pu(VI),respect ively

0

.

Perchloric Acid.-These results are presented in Table 1. Kasha4 measured only the disproportionation reaction except for the 0.516 M acid experi-

used instead of the smoothed values given in reference (4). The experiment at 0.052 M perchloric acid was omitted because of uncertainties in the data and because of the unknown correction for hyThe latter cannot be estidrolysis of Pu+4.10,11 mated reliably because the molar extinction coefficients of the hydrolyzed species are unknown. b

TABLE I

3

VALUESOF K ,

X

AND

kl FOR PERCHLORIC ACID SOLUTIOXS AT 25 i 0.5'

k HClOd, moles/l.

1.992 0.994 ,516

I

,481 .lOlQ

-1 -

1 2 3 (III)~(vI)/(IV)x J 108. Fig. 2.-Equilibrium and rate of disproportionation of pIutonium(1V) in 0.950 M hydrochloric acid a t 25". "F" is the value of the left side of equation 15, 16 or 17, multiplied by 0.01 times the total plutonium concentration. The symbols 0 , 0 and 0 refer to Pu(III), Pu(1Y) and Pu(VI), respectively.

I

2.00 1.00 1.00" 0.46) 1.00"

-10

--I

0.009 zk 0.002 .I3 i .03

.23 f .03 40 i 10

0.091 0 . 0 3 .9 .3 , 7 5 zk .12 150 zt 80

*

In the experiment a t 0,1019 M perchloric acid the change in concentration of Pu(1II) was small compared to that of Pu(IV), Pu(V) and Pu(V1). Therefore equation (11) was combined with equations (8), (9) and (10) to yield three equations similar to (15), (16) and (17) except that eachcontained the rate of change of Pu(II1) concentration. In the first, second and fourth experiments of Table I the concentration of Pu(V) and the d(V)/ dt term were negligible. In the third experiment Kasha reported no Pu,(V) concentrations but significant amounts should have been present. Its concentration was calculated using a value of 10 for KL, and slopes were read from the plot versus time. The correction was large only near the start of the experiment. The uncertainties in K,and kl indicated by i in Table I (and the other tables) are based on the niaxiinum spread in the plots of equations (l5), (16) and (17). To this error must be added any systematic errors in the analyses. In Fig. 4 the logarithm of K , is plotted versus the logarithm of the perchloric acid concentration for the experiments at unit ionic strength (symbol @). The straight line, which fits the points within the estimated uncertainty (denoted by the vertical lines), is drawn with a slope of -4.00. This is the power dependence on hydrogen ion expected from equation (1). The data uncorrected for the a-particle induced reaction gave a third power depende n ~ e . For ~ reaction (1) a t 1.1 = 1 and 25' the cquilibriuni quotient becomes A'

I

I

I

I

I

4 G S 10 ( I I I ) ~ ( V I ) / ( I V )x~ 10. Fig. 3.-Equilibrium and rate of reproportionation of plutonium(1V) in 0.950 M hydrochloric acid a t 25'. "F" is the value of the left side of equation 15, 16 or 17, multiplied by 0.01 times the total plutonium concentration. The symbols e, 0 and 0 refer to Pu(III), Pu(1V) and Pu(VI), respectively. (1

1.55 1.50 1.73 1.30

ki,

moles - 1 liters br.-l -10-1

K,

P

Sodium perchlorate added.

0

-141

Total PII, moles/l. 1.72 X 10-3

2

ment where equilibrium was approached through reproportionation of Pu(1V). The original, unsmoothed cnncentration data (unpublished) were

=

(Pu +3)2(Puo:! ++)(I3+I4 (Pu +4)3

=

o,oo9

i",",

The correctness of the assumed rate law was dificult to check by the linearity of the plots, because of the scattering of the points. Within the accuracy of the data straight lines were observed in all cases. The 0.516 M perchloric acid experiment was the only one in which a severe test could be made. When plotted according to the one other rate law which seems plausible on theoretical grounds,6 it failed to give a straight line. In the logarithmic plot of kl versus the acid coli(10) K . .%. Kraus, I, p. 241. (11) S. W. Kahideatr sn