rotational isomerism of methyldichlorothiophosphate

4
ROTATIONAL ISOMERISM OF METHYLDICHLOR OTHIOPHOSPHA TE R. R. Shagidullin, O. A. Raevskii, and I. I. Vandyukova UDC 541.63:541.62:547.1'118 The structure of methyldichlorothiophosphate (MCP) has already been discussed in the literature [1- 7]. The author of [2] suggests the presence of a plane of symmetry in both the conformers participating in the equilibrium. At the same time, in [6] considerations were advanced in support of an equilibrium of forms with shielding of the methyl group by sulfur and chlorine atoms. In this communication, data on the dipole moments (DM) [8] are enlisted for the characterization of the structure of MCP, together with sup- plemcntary spectroscopic information. The spectrograms that we obtained, in accordance with the already cited studies, clearly indicate thepresence of a conformational equilibrium. Moreover, it was found that in nonpolar medium (solution in CC14) at 298~ the conformer responsible for the absorption band in the IR spectra with maxima 474, 554, 702, and 827 cm -I (isomer (H) [2]) predominates quantitatively (70%). With increasing dielectric permeability of the medium, the position of the equilibrium is somewhat shifted in the direction of another conformer, responsible for the absorption band with maxima 452, 534, 720, and 820 cm -1 [isomer (I)]. Thus, in CH3CN solution a predominance of the latter conformer is already observed. This gives a basis for believing, in accord with [6], that the conformer (I) possesses a relatively large DM. It should be noted that in the gas phase an equilibrium of two isomers is observed, with a clear predominance of isomer (II), while in the IR and R aman spectra of the solid state, only the bands of the isomer (I) are present. The thermo- dynamic parameters of the conformational equilibrium in n-hexane, which we found, were: AHII- I = -- 650 50 cal/mole, ASII-I = --3.6 • 0.3 cal/mole deg, which is in quantitative agreement with the results of [6]. A comparison of the molecular DM of the compounds PC13 (0.8 D), PSC1 s (1.4 D), CHa--C--CH2--O--p / (4.15 D), CH3--C--CH2--O--P = S (6.77 D) shows that gP=S depends substantially on the substituent. Since there are two chlorine atoms and one ester oxygen at the phosphorus atom in MCP, we assumed pp = S = 2.3 D. For the remaining bonds we used the values: PlJ--CI = 0.56, PP=O = --0.6 and gOCH~ = --1.13D [9]. The calculations gave the following values of the DM for four possible steric forms: S CHs CI CI 2.43 D S Cl l-is CL 2,88 D" S i? .CHs :/ !! b Cl'~'~Ct 2,73D S v d ci~dl ! CHa :~,.46 A. E. Arbuzov Institute of Organic and Physical Chemistry, Kazan' Branch of the Academy of Sciences of the USSR. Translated from Izvestiya Akademii Nauk SSSR, Seriya Khimicheskaya, No. 1, pp. 80-84, January, 1975. Original article submitted March 18, 1974. 1975 Plenum Publishing Corporction, 227 West 1 7th Street, New York,'N. Y. 100ll. No part of this publication may be reproduced, stored in a retrieval system, or transmitted, in any form or by any means, electronic, mechanical, photocopying, microfilming, recording or otherwise, without written permission of the publisher. A copy of this article is available from the publisher for $15.00. 71

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Page 1: Rotational isomerism of methyldichlorothiophosphate

R O T A T I O N A L I S O M E R I S M O F

M E T H Y L D I C H L O R O T H I O P H O S P H A T E

R . R . S h a g i d u l l i n , O. A . R a e v s k i i , a n d I . I . V a n d y u k o v a

UDC 541.63:541.62:547.1'118

The s t r u c t u r e of methyld ichloro th iophosphate (MCP) has a l r eady been d i scussed in the l i t e r a t u r e [1- 7]. The author of [2] sugges t s the p r e s e n c e of a plane of s y m m e t r y in both the c o n f o r m e r s par t i c ipa t ing in the equi l ibr ium. At the s a m e t ime, in [6] cons idera t ions were advanced in suppor t of an equi l ibr ium of f o r m s with shielding of the methyl group by sulfur and chlor ine a toms . In this communica t ion , data on the dipole momen t s (DM) [8] a r e enl is ted for the cha r ac t e r i z a t i on of the s t r u c t u r e of MCP, toge the r with sup- p l e m c n t a r y s p e c t r o s c o p i c informat ion .

The s p e c t r o g r a m s that we obtained, in acco rdance with the a l r e ady ci ted s tudies , c l e a r l y indicate t h e p r e s e n c e of a conformat iona l equi l ibr ium. Moreover , it was found that in nonpolar med ium (solution in CC14) at 298~ the c o n f o r m e r r e spons ib l e for the absorp t ion band in the IR s p e c t r a with m a x i m a 474, 554, 702, and 827 cm - I ( i somer (H) [2]) p r edomina te s quant i ta t ively (70%). With inc reas ing d ie l ec t r i c p e r m e a b i l i t y of the medium, the pos i t ion of the equi l ibr ium is somewhat shif ted in the d i rec t ion of ano ther c o n f o r m e r , r e spons ib l e for the absorp t ion band with m a x i m a 452, 534, 720, and 820 c m -1 [ i somer (I)]. Thus, in CH3CN solution a p redominance of the l a t t e r c o n f o r m e r is a l r e ady obse rved . This gives a bas i s for bel ieving, in acco rd with [6], that the c o n f o r m e r (I) p o s s e s s e s a r e l a t i ve ly l a rge DM. It should be noted that in the gas phase an equi l ibr ium of two i s o m e r s is obse rved , with a c l ea r p r edominance of i s o m e r (II), while in the IR and R aman s p e c t r a of the sol id s ta te , only the bands of the i s o m e r (I) a r e p r e s e n t . The t h e r m o - dynamic p a r a m e t e r s of the conformat iona l equi l ibr ium in n-hexane , which we found, were : AHII- I = -- 650 �9 50 c a l / m o l e , ASII- I = - -3 .6 • 0.3 c a l / m o l e �9 deg, which is in quant i ta t ive a g r e e m e n t with the r e su l t s of [6].

A compar i son of the mo lecu l a r DM of the compounds PC13 (0.8 D), PSC1 s (1.4 D), CHa- -C- -CH2--O--p

/ (4.15 D), CH3--C--CH2--O--P = S (6.77 D) shows that g P = S depends subs tan t ia l ly on the subst i tuent . Since

t he r e a r e two chlor ine a toms and one e s t e r oxygen at the phosphorus a tom in MCP, we a s s u m e d p p = S = 2.3 D. For the r ema in ing bonds we used the va lues : PlJ--CI = 0.56, P P = O = --0 .6 and gOCH~ = --1.13D [9]. The calcula t ions gave the following values of the DM for four poss ib le s t e r i c f o r m s :

S CHs

CI CI

2.43 D

S

Cl l-is CL

2,88 D"

S i? .CHs :/ !!

b C l ' ~ ' ~ C t

2,73D

S v

d c i ~ d l ! CHa

:~,.46

A. E. Arbuzov Inst i tu te of Organic and Phys ica l Chemis t ry , Kazan ' Branch of the Academy of Sciences of the USSR. T r a n s l a t e d f rom Izves t iya Akademi i Nauk SSSR, Ser iya Khimicheskaya , No. 1, pp. 80-84, January , 1975. Original a r t i c l e submi t ted March 18, 1974.

�9 1975 Plenum Publishing Corporction, 227 West 1 7th Street, New York,'N. Y. 100ll. No part of this publication may be reproduced, stored in a retrieval system, or transmitted, in any form or by any means, electronic, mechanical, photocopying, microfilming, recording or otherwise, without written permission of the publisher. A copy of this article is available from the publisher for $15.00.

71

Page 2: Rotational isomerism of methyldichlorothiophosphate

TABLE 1. Energies of van der Waals Interact ions with Methyldichlorothiophosphate

Confor- ZE,kcal ]Confor- I~:E, kcal mation /mole lmation i/mole

a %o7 t ] 2,77 b --0,t2 ~ 0,00

The experimental value of the DM in a solution of CC14 at 298~ proved equal to 2.82 • 0.05 D, i . e . , in termediate between a and d. Since we know f rom the IR spec t ra that under conditions of de te rmina- tion of the experimental dipole moment an equilibrium of the composi- tion 7 : 3 is real ized, with predominance of the less polar form, we should consider the following var ia t ions : 0~ a with 0.3 b, c, d; 0.7 b, with 0.3 c, d; and 0.7 c with 0.3 d. According to the equation

~ x p = ~z 2x + ~rI" (t - - z)

the experimental value is best approached by the variat ion of equilibrium a ~- d or b ~ d. For the subse- quent select ion it is important that during the var ia t ion of the t empera tu re a large energy stabili ty of the i s o m e r (I) is detected; at the same t ime, there is only 30% at 298~ For the var ia t ion a ~= d this leads to a contradict ion to the Bol tzmann distr ibution law. F rom the standpoint of the equilibrium b ~ d the experimental data can be explained by the different s ta t is t ical probabil i ty of s t e r i c forms part icipating in the equilibrium. Actually, as a resu l t of t hep re sence of two identical substituents at the phosphorus atom, in the case of complete rotat ion re la t ive to the P- -O bond, conformation b is encountered twice:

r C]-13 CH

L " CI / ~ "CI C I / ~ \CI

Consequently, the formation of this fo rm is preferent ia l with respec t to entropy. On the basis of this, of the two var ia t ions remaining we selected the equilibrium b ~ d. Let us note that it agrees with the shape of the potential energy curve of the van der Waals interact ions of the nonbonded atoms [10] (Table 1).

Thus, an analysis of the mater ia l that we obtained permi t s us to support the fact that MPC is char - ac te r i zed by an equil ibrium of gauche- and t r a n s - e o n f o r m e r s (we have in mind the orientation of the P = S and O--CH 3 bonds). Since we know that the i s o m e r (I), s tabil ized in the solid phase, posses ses a r e l a - t ively la rge DM, we should a s sume that this is a symmet r i ca l t r a n s - f o r m .

We were in teres ted in calculating the frequencies and fo rms of normal vibrations of the MPC mole- cule, considering our identification of the i s o m e r s . A t r ans -eonformat ion posses ses s y m m e t r y Cs, and of 21 normal vibrat ions, 15 belong to type A' , six to type A". The tors ional vibrations around the 1)--O and C--O bonds were neglected. All the angles were assumed to be te t rahedra l . The calculation was pe r - formed according to the method of [11, 12]. The force constants cited in [7] were taken as the null approxi- mation. For be t te r ag reement of the calculated and experimenta! ly obse rved frequencies of the t r a n s - i somer , chiefly the diagonal force constants were varied. The best ag reemen t with the experiment was obtained at the following values of the force constants: Kii/[Q1] = 7.65; [Q2] = 7.39; [qi] = 7.8; [61] = 1.8; [62] = [53] = 1.7; [71] = [~/2] = 1.65; [T3] = 0.95; [~/4] = 1.1; [~i] = 1.3; [c~ i] = 0.6; Aij/[Q2t/i] = 0.4. The remaining coefficients were unchanged. The vibrational coordinates of MCP a re given in Fig. 1.

On the assumpt ion of constancy of the selected force field, we calculated the frequencies of the gauche - i somer , possess ing s y m m e t r y C1. The theore t ica l difference in the frequencies of the two i somers obtained is r a the r close to the experimental value (Table 2). Our calculated data confirmed and refined the ass ignments in the spec t rum of the compounds studied accepted in the l i te ra ture [2, 7]. From Table 2 it is evident that the P = S bond p r imar i ly par t ic ipates in the vibrations 8 and 8', and the P--C1 bond in

6

U

Q~

{11

~ H z q t ~ x 2 / a 3

Fig. 1. Vibrational coordinates of methyldichlorothiophosphate.

72

Page 3: Rotational isomerism of methyldichlorothiophosphate

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Page 4: Rotational isomerism of methyldichlorothiophosphate

vibrations 9 and 9', 17, and 17'. Moreover, the angles adjoining the phosphorus atom participate in these vibrations.

E X P E R I M E N T A L M E T H O D

Methyldichlorothiophosphate was synthesized according to the method of [13]. The II~ spectra were taken on a UR-10 instrument, slit program 4, ra te of development of the pr ism 32 cm-1/min; the Raman spectra were taken on a Coderg instrument in the interval 298-103~ The measurement of the capaci- tances of the solutions was performed on an IDM instrument [14]. The indices of refract ion were deter- mined on an IRF-23 re f rac tometer . The position of conformational equilibrium and the thermodynamic parameters were determined just as in [6].

The authors would like to express their gratitude to V. K. Khairullin for synthesizing the investi- gated compound.

CONCLUSIONS

1. An equilibrium of conformers with gauche- and trams-orientation of the P = S and OCH 3 groups in the gas and liquid phases follows from the vibrational spectra and dipole moments of methyldichloro- thiophosphate. A trans-conformer is realized in the crystalline state.

2. The IR and Raman spectra of methyldichlorothiophosphate were interpreted on the basis of a calculation of the frequencies and forms of the normal vibrations considering possible rotational isomers .

L I T E R A T U R E C I T E D

1. R . A . Nyquist and W. W. Muelder, Spectroehim. Acta, 22, 1563 (1966). 2. R . A . Nyquist, Spectrochim. Acta, 23A, 1499 (1967). 3. F. Feher and A. Blumcke, Chem. Ber . , 90, 1934 (1957). 4. Von V. Hornung, O. A. Wafa, A. Lentz, andY. Goubeau, Z. Anorgan. undAllgem. Chem., 380,

137 (1971). 5. R . A . McIvor, G. A. Grant, and G. E. Hubly, Canad. J. Chem., 34, 1611 (1956). 6. A. F. Vasil 'ev, Zh. Prikl . Spektroskopii, 6, 485 (1967). 7. A. F. Vasil 'ev, Zh. Prikl . Spektroskopii, 5, 524 (1966). 8. O . A . Raevsky, J. Molec. Structure, 19A, 275 (1974). 9. O . A . Raevskii, F. G. Khalitov, and T. A. Zyablikova, Izv. Akad. Nauk SSSR, Ser. Khim., 348

(1972). 10. E. Elliel, N. Allinger, S. Angyal, and G. Morrison, Conformational Analysis [Russian translation],

Mir (1969). 11. M . V . Vol'kenshtein, L. A. Gribov, M. A. El'yashevich, and B. L Stepanov, Molecular Vibrations

[in Russian], Nauka (1972). 12. L . S . Mayants, Theory and Calculation of Molecular Vibrations [in Russian], Izd-vo AN SSSR (1960). 13. I. Houben-Weyl, Organische Phosphor Verbindung, Stuttgart, Vol. 2 (1964), p. 590. 14. R. Sh. Nignmtullin and M. R. Vyaselev, Zavod. Lab., 30, 500 (1964).

74