13C NMR investigation of rhodium PI-complexes

13C NMR investigation of rhodium PI-complexes

INORG. NUCL. CHEM. LETTERS Vol. 9, pp. 885-889, 1973. Pergamon Press. Printed in Great Britain. 13C NMR INVESTIGATION OF R H O D I U M P I - ...

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INORG.

NUCL.

CHEM. LETTERS

Vol. 9,

pp. 885-889,

1973. Pergamon Press.

Printed

in

Great Britain.

13C NMR INVESTIGATION OF R H O D I U M P I - C O M P L E X E S D.E. Axelson, Dept. of Chemistry,

C.E. Holloway and A.J. Oliver

York University,

Downsview

(Toronto) Ontario,

Canada

(ReceiuedSAprill~3) Carbon nuclear

rhodium-olefin

magnetic

complexes

(1,2,3).

carbon atoms is not large is zero.

resonance

has

been

used

It was reported

for

several

studies

(i) that iJRh C for olefinic

(i0 ~ 14 Hz), and for the cyclopentadlenyl

This was a t t r i b u t e d

to the predominance

classification

group it

of T-type interactions

metal-ring bonding scheme, although with molecules of low symmetry, ~-C5H5RhL2,

of

in the

such as

of o-and T-bonding loses much of its significance.

An estimate of 15% s-character was made for the olefin-carbon AO used in bonding to the rhodium,

on the basis of an equation

the dominance of the Fermi Contact contribution.

(i) (p = 0.96 JRhC ) , assuming However,

this transfer of

s-character

into the metal-olefin bond does not seem to be countered by a de1 crease in s-character of the olefin C-H bonds as measured by JCH" Indeed an increase in IJcH seems to occur on coordination, noted in other ~-eomplexes s-character

of metals

in these complexes,

(4).

and similar effects have been

Insofar as JCH can be related to

which is not altogether

unlikely that the ligands are undergoing appreciable been pointed out (5) for Pt-olefin

complexes

certain,

it seems

internal change.

It has

that the spin coupling via a

Fermi Contact mechanism must occur through the ligand - metal o-bond in order to involve the metal s-orbital.

An MO calculation has suggested

(6) that the

Pt 6s-orbital does not contribute at all to the bonding in these complexes because of the relatively donor orbital.

large energy separation between it and the ligand

At the very least this does suggest that metal s-orbital

participation may be quite small.

If so, then relatively small changes of the

885

886

RHODIUM PI-COMPLEXES

Vol. 9, N o . 8

metal s-orbital participation in the ligand -- metal o-bond would have a marked effect on JMC'

At the same time other o-bonding contributions could be un-

changed or even enhanced via increased participation of other metal orbitals. The Table lists the 13C data obtained on some rhodium olefin and carbonyl derivatives in this study.

In these cases, splitting of the cyclopentadienyl

carbons by rhodium was clearly resolved.

Coupling to the olefinic carbon

atoms was in agreement with the previously reported data (i).

The magnitude of

JRhC for the cyclopentadienyl ligand is much smaller than for the olefinic case, the largest variations being observed for the rhodium(III) derivatives. The coupling also appears more sensitive to the other ligands on the metal, tending to decrease with increasing trans effect. (7) in JRhP"

A similar trend is observed

It is interesting to compare the reduced coupling constants of

platinum (8) and rhodium olefin derivatives.

In [(COD)RhCI] 2 the reduced

carbon-rhodium coupling is 14.8 x 1021 cm -3, and in (CODPt(CH3)~and (CODPt(CF3) 2 the reduced coupling is 8 x 1021 cm -3, which increases to 18.1 x 1021cm -3 for (COD)PtI 2.

Comparison of the ethylene derivatives (1,8) yields

KRh C = 10.5 to 14.8 x 1021 cm -3 and ~ t C

= 7.3 x 1021 cm -3 ~rans-[PtCH3(C2H4)-

~ ( C H 3 ) 2 ~ 2 ] P F 6 ) , and 28.5 x 1021 cm -3 ((C2H4)Pt(CI3)2).

The much larger varia-

tion in the platinum ethylene derivatives is reflected by a much larger variation in 13C coordination shift (8), although there is no clear relationship between the two.

This is not unexpected if coupling changes are due mainly to

changes in metal s-orbital participation. Coupling between rhodium and a carbonyl carbon has been reported for two derivatives, a cluster (2) RhN(CO) I2 and a dimer (3) [(C5H5)RhCO]2CO.

In the

monomeric derivative (C5H5)Rh(CO) 2 a value (Table) of 83.5 Hz is observed for IJRh C.

The correlation of s-characters and JRhC suggested by a previous study

(i) does not fit this compound, assuming the carbon s-character is 50%.

The

large value of the coupling suggests a greater involvement of rhodium s-orbital in this metal-carbon bond.

It has been noted elsewhere (9) that the reduced

~

62.1

All

downfie]d relative to TMS.

5.2

88.6

C5H5Rh[(CH3)2CHNC]I 2

*

0

93.3

CsHsRhP#3(COCH3)I

80.3

3.8

ppm

(COD)Rh(2.4.Leutidine)Cl

86.2

CsH5Rh(COD)

2.4

6

78.5

82.5

C5H5Rh(CO)P~ 3

3.0~0.2

JHz

Olefln

12.5

13.9

13.9

JHz

Isonitrile

P~3

Acetate

2.4 Leut:

It

"

It

(PC) " "

(RHC)

JHz

23.0 n4ogtSsee~

CH 3

not seen 133.8 (PC) 127.7 " 130.1 "

55.7

30.9 148.0 133.9 138.4 18.2

30.9

32.3

132.2 127.0 128.9

CH N~C

C:O ortho meta para

CH 3

CH3

ortho meta para

"

ppm

Carbons

19.9

Other

ortho meta para

(COD) aliphatie

P$3

CO

13C Data for Rhodium Com p lexes

[(COD)RhCI] 2

87.6

ppm

Cyclopentadlenyl

C5HsRh(CO) 2

Compound

Table

10.3 10.4 0

12.7 10.5 1.7

83.5

.o

888

RltODIUM P I - C O M P L E X E S

Vol. 9, No. 8

coupling KMC in the first row transition metal carbonyls increases left to right.

The reduced coupling for the rhodium complex (88.5 x 1021cm -3)

is intermediate between those of the first row carbonyls (14 to 40 x i0 21cm-3) and that of a third row derivative (durene)W(CO)3 (168 x i021cm-3).

The same

coupling has been observed for the dimer (3), the values of 2JRh C and IJRh. R h being near zero, the latter suggesting very little s-character in this bond. Only an averaged coupling is obtained for the cluster (2), however, similar values of

JRhC can fit the observed spectrum on taking into account that the

averaged spectrum is made up of nine iJRh C (terminal) plus three iJRh C (bridging) and thirty-three 2JRh C.

If values of 83 and 45 respectively are taken for

the iJRh C parameters and zero for 2JRh C an average of 19 Hz is obtained, compared to the experimental value of 17.1 Hz.

If 2JRh C is small but of opposite

sign to 1JRhc, which is consistent with the sign alternation observed in other couplings, then a closer fit could be obtained with only minor changes in the iJRh C parameters.

On the other hand, substituent effects can be quite large,

as the value of 68.8 Hz for JRhC in dicarbonyl rhodium chloride dimer (2) indicates.

This resonance, along with the carbonyl resonances of C5H5Rh(CO)P~3

and C5H5Rh(P~3)(COCH3)I ,

could not be observed in natural abundance in this

study.

Acknowledgements The authors thank Varian Associates for loan o£ an NV-14 FT NMR spectrometer.

Vol. 9, No. 8

RHODIUM P I - C O M P L E X E S

889

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2.

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