Reaction Product Identification from O(3P) + Benzene, Toluene, and 1

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Reaction Product Identification from O( P) + Benzene, Toluene, and 1,3,5-Trimethylbenzene Collisions THOMPSON M. SLOANE

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Physical Chemistry Department, General Motors Research Laboratories, Warren, MI 48090

Reactions of oxygen atoms with aromatic hydrocarbons have received a great deal of attention in recent years because of their potential importance in combustion processes and in atmos­ pheric chemistry. (1) This paper presents the results of product analysis of single reactive c o l l i s i o n s at room temperature between O( P) atoms and benzene, toluene, and 1, 3, 5 - trimethyl­ benzene. The apparatus used in these experiments consisted of a quadrupole mass spectrometer housed inside a two-chamber, d i f f u ­ sion-pumped, stainless steel vacuum system. The major features of the design were similar to the apparatus employed by Foner and Hudson. (2) The beam intersection angle was 60°. Products were observed at m/e = 94 and 66 for the reaction of O( P) with benzene. The product at m/e= 94 i s a long-lived C H O complex which, if stable, i s probably phenol. The product at m/e = 66 corresponds to the complex minus a molecule whose mass i s 28. a.m.u., undoubtedly carbon monoxide. The ionization efficiency measurement for this C H hydrocarbon product i s shown in Figure 1. There appears to be a small amount of product with an ionization threshold near 9.0 eV, and a much larger amount with a threshold near 9.6 eV. Cyclopentadiene has an ionization potential of about 9 eV. Molecules similar to 3-penten-1-yne have ionization potentials in the range 9.8 to 10.2 eV. (4) Assuming that 3-penten-1-yne has an ionization potential close to those compounds, the major product at m/e = 66 i s l i k e l y to be this open-chain C H hydrocarbon. The less intense product is probably cyclopentadiene. The hydrocarbon product must be in its ground electronic state for two reasons. F i r s t , the reaction would be too endothermic (ΔΗ = 20 kJ/mol) to take place at these low kinetic energies if the product were e l e c t r o n i c a l l y excited. Second, the measured ionization potential would be about 3 eV smaller for the excited product. Products were observed at m/e = 108, 106, and 80 for the reaction of oxygen atoms with toluene. These three product 3

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• M A S S 66

Ο

Δ

Ο

Δ 9.0

8.0

Δ

10.0 E l e c t r o n Energy ( e V ) 3

Figure 1. Ionization efficiency measurement for the 0( P) + benzene reaction product at m/e = 66. Ο—measured intensity; Δ—intensity corrected for thefiniteenergy width of the ionizing electrons using the procedure in Ref. 3.

masses correspond t o the three products observed f o r 0 ( P ) + 1, 3, 5 - trimethylbenzene. Since more extensive data were obtained f o r t h i s l a t t e r r e a c t i o n , the r e s u l t s f o r 0( P) + toluene w i l l not be discussed f u r t h e r . The r e a c t i o n o f 0( P) with 1, 3 , 5 - trimethylbenzene y i e l d e d products a t m/e = 136, 134, and 108. Figure 2 shows the i o n i z a t i o n e f f i c i e n c y measurement f o r the product a t m/e = 136. The i o n i z a t i o n t h r e s h o l d i s about 8.2 eV. This product could be 2, 4 , 6 - t r i m e t h y l p h e n o l , 3 , 5 - d i m e t h y l a n i s o l e , or 3 , 5 dimethyl benzyl a l c o h o l . Since i t i s unclear how the i n t e r n a l energy o f the C H , 0 adduct (^400 kJ/mol i f i t i s the ground e l e c t r o n i c s t a t e ) might a f f e c t an i o n i z a t i o n p o t e n t i a l measure­ ment, no c o n c l u s i o n can be drawn about t h i s product's s t r u c t u r e . The i o n i z a t i o n e f f i c i e n c y measurement f o r the product a t m/e J

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Brooks and Hayes; State-to-State Chemistry ACS Symposium Series; American Chemical Society: Washington, DC, 1977.

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= 134 i s shown i n Figure 3 . A l i k e l y product a t t h i s mass i s 3 , 5 - dimethylbenzaldehyde because the i o n i z a t i o n p o t e n t i a l o f methylbenzaldehyde i s 9.33 eV. (4j_ The i o n i z a t i o n e f f i c i e n c y measurement f o r the product a t m/e = 108 i s shown i n Figure 4. As i n the case of 0( P) + benzene, when CO leaves the adduct the r i n g may c l o s e to form trimethylcyclopentadiene ( I . P . = 7.96 eV ) or remain open to given an open-chain o l e f i n s i m i l a r to hydrocarbons having i o n i z a ­ t i o n p o t e n t i a l s ranging from 8 . 6 to 9.1 eV. Although the measur­ ed data were too noisy f o r c o r r e c t i o n , they i n d i c a t e that a t l e a s t a major f r a c t i o n o f the products a t m/e = 108 i s an openchain o l e f i n r a t h e r than t r i m e t h y l c y c l o p e n t a d i e n e . A r e a c t i o n path which was not observed f o r these r e a c t i o n s i s the hydrogen atom a b s t r a c t i o n path to produce OH and an aromatic r a d i c a l . Even i f the aromatic r a d i c a l i s s c a t t e r e d "backward," i t should s t i l l be observed due t o poor beam collimation. -, 1 Tests f o r the p a r t i c i p a t i o n o f r e a c t i o n s o f 0( D) o r 0p( Δ ) i n the 0 atom beam and f o r r e a c t i o n s i n the i o n i z e r showed t h a t these p o s s i b l e i n t e r f e r i n g processes were n e g l i g i b l e . g The c o r r e l a t i o n diagram of Figure 5 shows f o r 0( P) + benzene that ground s t a t e r e a c t a n t s should c o r r e l a t e with e x c i t e d products. The observed products must then be produced by a s p i n -

ο ( P ) Io}j-*3

+ /

Ο

Measured

Δ

Corrected

Mass 1 3 6

. 1.0

-

.5

Ο

Δ Δ

Ο

ο Δ

Δ Δ 7.0

Δ

Δ 8.0

9.0

Electron Energy (eV)

10.0

Figure 2. Ionization efficiency measure­ ment for the 0( P) + 1,3,5-trimethylbenzene reaction product at m/e = 136 3

Brooks and Hayes; State-to-State Chemistry ACS Symposium Series; American Chemical Society: Washington, DC, 1977.

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0 ( P) +J^)_^ I 3

/

30

r

^ ^

• Mass 1 3 4

\—

Δ

Δ

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20 \ —

Δ 10

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Δ Δ & 7.0

Δ

ι

Δ

Δ

Δ

Δ

Δ

I

Δβ.Ο

9.0 Electron Energy

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Figure 3. Ionization efficiency measurement for the 0( P) + 1,3,5-trimethylbenzene reaction product at m/e = 134. Only the corrected measurement is shown. 3

forbidden process. T u l l y has s u c c e s s f u l l y explained the r a p i d r a t e s of a number of s p i n - f o r b i d d e n r e a c t i o n s . (5) To determine whether h i s theory may e x p l a i n the s p i n - f o r b i d d e n nature of the 0 + benzene r e a c t i o n , the f o l l o w i n g two questions must be answered: (1) i s the lowest t r i p l e t s t a t e of phenol (T,) l o n g l i v e d enough? (2) Is the c r o s s i n g region between T, and S e a s i l y a c c e s s i b l e during the l i f e t i m e of the complex? To answer the f i r s t q u e s t i o n , the RRKM l i f e t i m e of T was e s t i m a t e d . For a r e l a t i v e k i n e t i c energy of 2.7 kJ/mol, the estimated l i f e t i m e was 10" seconds. A c r o s s i n g pointed l o c a t e d near the,-minimum of a 1300 cm v i b r a t i o n could be t r a v e r s e d 3.5 χ 10 times during t h i s l i f e t i m e . In order to answer the second q u e s t i o n , t h a t of the a c c e s s n

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Brooks and Hayes; State-to-State Chemistry ACS Symposium Series; American Chemical Society: Washington, DC, 1977.

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Reaction Product Identification

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SLOANE

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Figure 4. Ionization efficiency measurement for the 0( P) + 1,3,5-trimethylbenzene reaction product at m/e = 108. Only the uncorrected measurement is shown. 3

8.0

9.0

E l e c t r o n Energy

10.0 (eV)

+50

0( D) + CgHg^A! 1

CO + H C = C C H = C H C H ( A ' 3

J

CO( l )+HC^CCH=CHCH ( A') 1

w

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-50

-100 I CO + C H 5

6

OH

)po Figure 5.

c

6v

-OH C

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O

+

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5 6 H

s

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Electronic state correlation diagram for the 0( P) + benzene system

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-301.40

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-301.50 h-

z -301.60

-301.70 T -

DISPLACEMENT

(Λ)

Figure 6. Energy of the T, and S states of phenol as a func­ tion of displacement from the T, minimum along a ring stretch­ ing vibrational mode 0

i b i l i t y of the c r o s s i n g r e g i o n , c a l c u l a t i o n s were c a r r i e d out with the ab i n i t i o SCF-M0 program Gaussian 70 using the ST0-3G b a s i s s e t . (7) The T-. and S p o t e n t i a l energy surfaces along e i g h t v i b r a t i o n a l modei of phenol were e x p l o r e d . For one mode, a c r o s s i n g was located about 160 kJ/mol above the minimum energy c o n f i g u r a t i o n of T,. The r e s u l t s f o r t h i s mode are shown in Figure 6. Due to the p r i m i t i v e nature of these l i m i t e d basis set s i n g l e - c o n f i g u r a t i o n c a l c u l a t i o n s , the r e l a t i v e p o s i t i o n s of the two surfaces are u n c e r t a i n . The two surfaces probably cross but where the c r o s s i n g i s l o c a t e d w i t h respect to the minimum i n the Τ , surface cannot be determined with chemical accuracy from these c a l c u l a t i o n s . These RRKM and molecular o r b i t a l c a l c u l a t i o n s i n d i c a t e t h a t T u l l y ' s theory of s p i n - f o r b i d d e n r e a c t i o n s i s a p l a u s i b l e explana­ t i o n f o r the s p i n - f o r b i d d e n nature of the 0( P) + benzene and Q

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methylbenzene r e a c t i o n s . More accurate c a l c u l a t i o n s would be h e l p f u l i n e x p l a i n i n g more clearly the details of these r e a c t i o n s .

Literature Cited 1.

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J.

See Colussi, A. J., Singleton, D. L., Irwin, R. S., and Cvetanovic, R. J., J. Phys. Chem., 79, 1900-3 (1975), and references cited therein. 2. Foner, S. Ν . , and Hudson, R. L., J. Chem. Phys., 53, 4377-86 (1970). 3. Winters, R. E., Collins, J. H., and Courchene, W. L., J. Chem. Phys., 45, 1931-37 (1966). 4. Franklin, J. L., Dillard, J. C., Rosenstock, H. M., Herron, T., Draxl, K . , and F i e l d , F. H., "Ionization Potentials, Appearance Potentials, and Heats of Formation of Gaseous Positive Ions," NSRDS-NBS 26, U. S. Government Printing Office, Washington, D.C., 1969. 5. T u l l y , J. C., J. Chem. Phys., 62, 1893-8 (1975). 6. Hehre, W. J., Lathan, W. Α., D i t c h f i e l d , R., Newton, M. D., and Pople, J. Α., GAUSSIAN 70, Program #136, Quantum Chemistry Program Exchange, Indiana University, Bloomington, Indiana. 7. Hehre, W. J. and Pople, J. Α., J. Amer. Chem. Soc., 92, 2191-7 (1970).

Brooks and Hayes; State-to-State Chemistry ACS Symposium Series; American Chemical Society: Washington, DC, 1977.