The Dissociation Constants of Some Phosphorus(V) Acids

The Dissociation Constants of Some Phosphorus(V) Acids

THE DISSOCIATION CONSTANTS OF SOME PHOSPHORUS (V) ACIDS 245 The Dissociation Constants of some Phosphorus(V) Acids C. J. P e a c o c k * and G. N ic k l e s s Department of Inorganic Chemistry, University of Bristol, England (Z. Naturforsch. 24 a, 245— 247 [1969] ; received 25 September 1968) The dissociation constants of ortho-, monothio-, monoamido- and diamido-phosphoric acids have been measured at a series of temperatures using a potentiometric titration method involving com­ puter fitting of the theoretical titration curve to the experimental one. the constants being used as adjustable parameters. Less accurate values for diamidothio- and tetrathio-phosphoric acids were also obtained. The results are discussed with respect to the site of protonation. For the monothio acid only the first dissociation (ATt) appears to involve the sulphur atom. The monoamido compound may be protonated first on nitrogen (£2) • The diamido- and diamidothio-phosphoric acids show a remark­ able effect in that, although monoanionic, two p K a values may be measured, the first protonation (Ko) being probably onto nitrogen, the second (£j) involving the oxygen atom more. For measuring dissociation constants of acids This differential equation may be integrated and the with no measurable U.V. or visible spectra, as the curve shape calculated. This was done automatically phosphorus ( V) acids, it is necessary to use con­ by the computer program. ductivity or potentiometric titration methods. If the The various data affected the calculated curve compounds are relatively unstable as acids one thus: dissociation constants only in the region of wishes to work as far as possible with the salts, so ± 2 p K units around their value; Ky,- between pn 7 conductivity methods are not available. The normal and 9, A around p Kx and pn 7, B\y around p Kx procedure for potentiometric titrations is to titrate and p Ko but if B\y was calculated from the titration the salt with acid until it is half ionized, whence as curve using the value of A small errors in A had p Ka = ph + l°g ([acid] / [salt]) and the acid and salt little affect on the curve; changes in V displaced the activities are equal, the p Ka is given, after some whole curve slightly. corrections, by the pn at this point. However the Thus the titration was performed using a solution method is wasteful on data, effectively only one of the salt of the weak acid containing a few7 drops point on the whole curve being used. It is possible of strong base so that both inflection points appear however to calculate the shape of the titration curve, on the titration curve, and Bw could be calculated and using the dissociation constants as adjustable from the volume added between them. The data were parameters fit this to the experimental data. This taken from the region where the curve shape was also allows for the corrections needing to be made sensitive to variation of the dissociation constants. for the volume of acid added, proton transfer etc. Initial values of these constants were calculated from If the volume of acid of normality A added to a the midpoint of the two inflections. mixture of B mmoles of strong base and B\\ mmoles The quantity calculated is the hydrogen ion con­ of a weakly dibasic salt is v mis, then: centration, but that measured by a pn meter is the a _b_ jtw lK + a +H(V+r) activity. Thus a parameter linking the two was intro­ duced. Attempts were made to calculate it from Debye-Hiickel theory; treat it as a variable of the where the initial volume of solution was V mis, the form given by this theory; or just considering it a hydrogen ion concentration is H, and Kx, K2 and constant over the whole titration. The last gave just K\\ are the dissociation constants of the weak base as consistent results and involved the least calculation and ionic product of water respectively. so was always used. The value of this mean activity The change of hydrogen ion concentration with coefficient always fell between 0.8 and 0.95. volume is hence given by The calculations were performed using a com­ dH = (A+Kw -H \ / puter program which integrated the differential equa- dv { H } / l(Kw+H2)(V + v) , BwK^HZ+M iK^ + K^KJ * Present address: Dept, of Chemistry, The University, Sout­ V H //-’ f / / K1 + Kl K, hampton, S09 5NH, England. Dieses Werk wurde im Jahr 2013 vom Verlag Zeitschrift für Naturforschung This work has been digitalized and published in 2013 by Verlag Zeitschrift in Zusammenarbeit mit der Max-Planck-Gesellschaft zur Förderung der für Naturforschung in cooperation with the Max Planck Society for the Wissenschaften e.V. digitalisiert und unter folgender Lizenz veröffentlicht: Advancement of Science under a Creative Commons Attribution Creative Commons Namensnennung 4.0 Lizenz. 4.0 International License. 24 6 C. J. PEACOCK AND G. NICKLESS tion by a Runga Kutta method for each combination paratus was brought up to temperature containing of parameters and performed a least squares fit on distilled water and the electrodes were equilibrated the data by adjusting the parameters. The final fit at this temperature for at least 12 hours. Tempera­ resulted in the calculated and theoretical curves be­ ture control was obtained by immersing the appara­ ing always within 0.02 pu units of each other. tus in a waterbath controlled to within 0.1 cC by a Measurements were performed at a series of tem­ Tecam “Tempunit’. The water was then carefully peratures and the final values smoothed using the poured out leaving any condensed on the vessel and function T p Ka = a + b T + c T2. Both smoothed and condenser sides as far as possible untouched, for at unsmoothed values are given in Table 1. It is seen higher temperatures this could be 2 — 3 ml, enough that the r.m.s. variation of the two for any one set to introduce an error of 0.01 pn units. The pre­ is at most 0.05 units. Taking into account the error warmed salt solution was then poured in and the as­ due to using mean activity coefficients, the uncer­ sembly left to come to equilibrium again. A stream tainty on the ionic strength, and the error on the of nitrogen served to stir the solution and remove data constants it is thought that the error on the any contaminating carbon dioxide. smoothed p Ka values will not exceed 0.05 units. All Immediately before titration the electrodes were values are relative to a pn scale taking that of an standardized against 0.05 m potassium hydrogen 0.05 m aqueous solution of potassium hydrogen phthalate solution. phthalate as being 4.000 at 15 °C. For titrations of thio-phosphates the nitrogen stream passed through a solution of silver nitrate Experimental after leaving the titration vessel, so that any decom­ Measurements were made in a 250 ml five-necked position could be monitored. For monothiophosphate reaction vessel fitted with the two pn meter electro­ at 35 °C only 2/S decomposition had occurred by des (E.I.L. GHS 33 screened glass above 15 °C, the end of the measurements. E.I.L. GHC 33 screened glass below 20 cC; calomel The salt solution was made up of 200 ml of 0.05 m /saturated KC1 reference); thermometer; burette; phosphorus anion, plus potassium chloride and a coldwater condenser and nitrogen bleed. The record­ few drops of potassium hydroxide to bring the initial ing was done on a Vibron 39 A pn-meter. The ap­ PH up to 11 or so, and the initial ionic strength to P Ki P k 2 PK 3 Ion Temp. °C Measured Smoothed Measured Smoothed Measured Smoothed P 0 43" 0.2 1.610 1.713 6.781 6.730 10.0 1.781 1.742 6.725 6.712 22.0 1.859 1.860 6.704 6.690 22.1 1.803 1.861 6.691 6.694 Not measured 30.0 1.983 1.937 6.724 6.715 40.0 1.998 2.008 6.704 6.718 50.0 2.104 2.108 6.725 6.726 p o 3s 3~ 10.0 1.265 1.265 5.254 5.280 10.294 10.29 16.0 1.517 1.517 5.382 5.390 10.175 10.19 19.0 —— 5.378 5.401 10.154 10.13 25.0 1.788 1.788 5.413 5.427 10.092 10.08 32.2 —— 5.400 5.428 10.009 10.00 POjjNHo2- 6.0 2.735 2.610 8.403 8.422 9.2 2.707 2.708 8.345 8.320 19.0 2.734 2.738 8.198 8.184 26.5 2.738 2.739 8.050 8.102 33.0 2.758 2.731 7.978 7.950 40.0 2.708 2.716 7.865 7.896 46.3 2.696 2.696 7.808 7.821 P 0 2(NH2)2- 0.0 1.118 1.051 5.279 5.299 8.0 1.140 1.098 5.182 5.103 21.4 1.148 1.194 4.978 4.998 30.0 1.221 1.279 4.870 4.889 40.0 1.451 1.400 4.803 4.780 Table 1. p Ka values for ortho-, monothio-, monoamido- and diamidophosphoric acids over a range of temperatures. Measured values from individual experiments; smoothed ones from best fit to curve T ■ p K a = a + b T + c T2.

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