The bicyclo[2.1.1]hexan-2-one system: A new probe for the experimental and computational study of electronic effects in π-facial selectivity in nucleophilic additions

Article abstract of DOI:10.1016/S0040-4039(01)01818-4

The remotely substituted 5-exo-bicyclo[2.1.1]hexan-2-one system is introduced as a new probe to study long range electronic effects on π-face selectivity during hydride reduction and a systematic computational study demonstrates good predictability at the

Full text of DOI:10.1016/S0040-4039(01)01818-4

TETRAHEDRON
LETTERS
Pergamon
Tetrahedron Letters 42 (2001) 8527–8530
The bicyclo[2.1.1]hexan-2-one system: a new probe for the
experimental and computational study of electronic effects in
p-facial selectivity in nucleophilic additions
Goverdhan Mehta,a,* S. Robindro Singh,a Vanessa Gagliardini,a U. Deva Priyakumarb and
G. Narahari Sastryb,*
aDepartment of Organic Chemistry, Indian Institute of Science, Bangalore 560 012, India
bDepartment of Chemistry, Pondicherry University, Pondicherry 605 014, India
Received 7 August 2001; revised 18 September 2001; accepted 27 September 2001
Abstract—The remotely substituted 5-exo-bicyclo[2.1.1]hexan-2-one system is introduced as a new probe to study long range
electronic effects on p-face selectivity during hydride reduction and a systematic computational study demonstrates good
predictability at the semi-empirical level. © 2001 Elsevier Science Ltd. All rights reserved.
Prediction and control of stereoselectivities during
nucleophilic additions to the carbonyl group is a funda-
mental issue in stereogenesis. While the role of steric
effects in controlling p-face selection during addition to
the carbonyl group is well recognized and predictable,
the precise nature and effectiveness of long range elec-
tronic effects in determining p-face selectivity is a mat-
ter of ongoing inquiry and debate.1 Examples are now
known where remote electronic effects can overwhelm
steric effects and there is the possibility of such effects
finding applications in stereoselective syntheses.2 In
order to separate steric and electronic effects, several
probe systems, wherein the two faces of the carbonyl
group are in an isosteric environment, have been intro-
duced.3 We have reported that in endo substituted
bicyclo[2.2.1]heptan-7-ones 13a,b and bicyclo[2.2.2]-
octan-2-ones 2,3c 4-substituted-9-norsnoutanone 33d
and related systems, where the carbonyl group is in a
sterically neutral disposition, distal substituents can
influence stereochemical outcome (syn- versus anti-
addition) in a profound way. Continuing our investiga-
tions in the area,1b,3a–e we now introduce 5-exo-
substituted-bicyclo[2.1.1]hexan-2-ones 4 as a new probe
system to explore further the role of distal electronic
modifications on p-face selectivity. We have also
employed the experimental results on 4 to test the
predictability of various computational models at dif-
ferent levels of theory.
In light of our interesting observations during the
hydride reduction of 1–3, p-face selection studies with 4
were a natural impulse. Besides the broad structural
resemblance to 1 and 2 and isosteric environment
around the carbonyl group as revealed by high level
calculations, the skeleton of 4 has some distinctive
features. The substituent in 4 is farther removed from
the stereoinduction center compared to 1 and the elec-
tronic effects are transmitted through the connecting
cyclobutane bonds. Further, the carbonyl group is in
the ‘off’ position from the vertical plane in which the
substituent resides. Thus, a study of face selection in a
range of derivatives of 4 was of intrinsic interest. How-
O
O
O
O
R1
R1
R
R
R
R
1
3
2
4
* Corresponding authors.
0040-4039/01/$ - see front matter © 2001 Elsevier Science Ltd. All rights reserved.
PII: S0040-4039(01)01818-4

8528
G. Mehta et al. / Tetrahedron Letters 42 (2001) 8527–8530
ever, 5-exo-substituted derivatives like 4 are syntheti-
cally quite inaccessible.4 In this context, a recent report5
on the synthesis of 4 (R=COOCH3), although involving
an arduous and long synthetic sequence, provided an
opening. Employing this route, emanating from readily
available bicyclo[2.2.1]hept-5-en-2-one, we have synthe-
sized several 5-exo-bicyclo[2.1.1]hexan-2-one derivatives
4a–f6 and subjected them to hydride addition.7
system 1. The anti-face selectivity in the case of 4d,f is
contrary to the prediction based on the Cieplak model.9
In the case of the alkyl substituted derivative 4e, there
is a marginal preference for the anti-face addition, see
Scheme 1.
The experimental probe 4a–f provided an opportunity to
test the validity and predictability of the proposed
computational models3b,8 at different levels of theory.
The reduced selectivities observed in the case of 4 (cf.
1–3)3a–e were indicative of the involvement of more
subtle factors and thereby this system was expected to
provide a stringent test for the performance of computa-
tional techniques. While ab initio and DFT level calcu-
lations were performed using the Gaussian 94 suite
of programs,10 the MNDO11a and AM111b calculations
used the MOPAC program package. First, the eco-
nomically attractive semi-empirical, MNDO and AM1
methods were employed to discern the orbital and
electrostatic effects using the hydride and charge models
as well as the LiH transition states (Table 1). The charge
and hydride model calculations were carried out by
placing a point charge and hydride ion, respectively, 1.4
Bicyclic ketones 4a–f on reduction with sodium borohy-
dride furnished (E)-5a–f and (Z)-6a–f alcohols in near
quantitative yield (Scheme 1).7 The observed diastereo-
selectivities (E:Z ratio) are displayed in Scheme 1 and
1
were determined through GLC and H NMR analyses.
The stereostructures of 5a–f and 6a–f were unambigu-
ously determined on the basis of: (i) the relative
deshielding (ca. 0.45 ppm) of the H(6) endo protons in
the (E)-alcohols 5a–f compared to the (Z)-alcohols 6a–f.
The H(6) endo proton in 5a–f and 6a–f appeared as a
diagnostic triplet (J=ꢀ7 Hz) due to long range (4
bond) coupling with the H(5) endo proton and could be
readily recognized; (ii) shielding (ca. 3–5 ppm) of the
C(6) carbon resonance in the (E)-series compared to the
(Z)-series.
,
A away from the carbonyl carbon on both sides along
the trajectory perpendicular to the carbonyl face, as
described earlier.3b The LiH transition states are located
on the potential energy surface and characterized as
saddle points by the frequency calculations. Charge
models overestimate the preference for the anti attack,
especially at MNDO level (Table 1). However, the
results of hydride and LiH transition state models
The stereoselectivities during hydride reduction of 4a–f
are generally consistent with the trend observed earlier
with related systems.1–3 However, the syn-face prefer-
ence of the remote electron withdrawing substituents
like cyano and ester is diminished in the bicy-
clo[2.1.1]hexane system 4 compared to the norbornyl
O
OH
H
HO
H
2
3
1
NaBH4
(endo)H
6
6
+
(endo)H
H
MeOH, 0-5oC
H
6
5
4
H(exo)
(E)-5a
H(exo)
(Z)-6a
R
R
R
4a
75%
66%
25%
R = CN
b
c
34%
40%
52%
b
c
d
R = COOMe
R =
b
c
60%
48%
C
CH
R = CH2OH
R = CH2CH3
d
e
f
d
e
f
e
f
47%
44%
53%
56%
CH=CH
R =
2
Scheme 1.
Table 1. The relative energy for anti-face addition with respect to the syn-face addition calculated using the hydride model,
charge model and for the LiH addition transition states at MNDO and AM1 levels.a All values are given in kcal/mol
4. R=
Charge model
AM1
Hydride model
AM1
Transition states
AM1
0.58
MNDO
MNDO
MNDO
CN
COOMe
CCH
CH2OH
CH2CH3
CHCH2
−0.26
−1.65
−2.00
−3.95
−4.29
−3.06
1.85
0.56
−0.37
−3.27
−3.02
−3.50
0.67
0.47
−0.04
−0.63
−0.78
−0.38
1.19
1.02
0.38
−0.23
−0.41
−0.68
0.26
−0.05
−0.14
−0.35
−0.32
−0.24
0.11
0.17
−0.56
−0.24
−0.24
a A positive value denotes syn preference and a negative value denotes anti preference.

G. Mehta et al. / Tetrahedron Letters 42 (2001) 8527–8530
8529
are in good agreement with the experimental
observations.
level of theory. All methods correctly reproduce the
higher syn selectivity for the cyano substituent, and anti
selectivity of ethyl and hydroxymethyl groups. The
success of the hydride model over the charge model in
correctly reproducing the observed selectivities high-
lights the subtle interplay of electrostatic and orbital
effects in the nucleophilic additions to the carbonyl
group.
The hydride and LiH transition state models were
modelled also at ab initio and density functional theory
level. Transition states are optimized (transition states
for syn and anti attack in 4a are given in Fig. 1) and
characterized by frequency calculations at the B3LYP/
6-31G* level, followed by single point calculations at
HF and MP2 levels. Table 2 clearly indicates that the
relative barrier heights are virtually insensitive to the
The Cieplak type hyperconjugative effects and the per-
turbations in carbonyl pyramidalization upon metal ion
complexation8b are estimated by NBO analysis12 and
proton complexation models, respectively, at B3LYP/6-
31G* level of theory (Table 3). The interaction energies
between the s 1,5- and s 1,6-donors and p*CO accep-
tors, as obtained from the NBO second-order perturba-
tive analysis, predict uniform preference for an anti
attack in all cases. The metal ion complexation model
predicts the preferential syn attack for 4a and anti for
4b–f. Also, the differences in the pyramidalization,
gauged by the difference in the dihedral angles D1 and
D2, do not correlate very well with the observed selec-
tivities. Thus, the simplistic approximations in the NBO
analysis and cation complexation models have rather
limited predictability. In contrast, the hydride model,
which takes into account electrostatic and orbital
effects, seems to provide reliable and quick answers
even at semi-empirical level (Table 1).
syn
anti
In summary, a systematic experimental and computa-
tional study on the new system 4, ranging from semi-
empirical to ab initio and DFT, indicates that the
Figure 1. The B3LYP/6-31G* optimized LiH addition transi-
tion state structures.
Table 2. The relative energy for anti-face addition with respect to the syn-face addition calculated using the hydride model
and for the LiH addition transition states at HF, B3LYP and MP2 levels.a All values are given in kcal/mol
4. R=
Hydride model
Transition state
B3LYP/6-31G*
HF/6-31G*b
MP2/6-31G*b
B3LYP/6-31G*
HF/6-31G*b
MP2/6-31G*b
CN
COOMe
CCH
CH2OH
CH2CH3
CHCH2
1.28
−1.95
−0.15
−1.03
−1.89
−1.46
1.36
−0.57
−0.67
−1.17
−2.72
−2.37
1.52
−0.72
−0.03
−0.78
−1.82
−1.48
1.16
0.46
0.41
−0.14
−0.09
0.34
0.76
0.40
0.33
−0.07
−0.07
0.13
1.13
0.52
0.45
−0.14
−0.11
0.27
a A positive value denotes syn preference and a negative value denotes anti preference.
b Single point energy calculations on B3LYP/6-31G* optimized structures.
Table 3. The NBO s–p* interaction energy (in kcal/mol), which estimates the Cieplack-type hyperconjugative effect, and the
dihedral angles which gauges carbonyl pyramidalization for the proton complex. Values in parentheses correspond to the
neutral reactant. All values are at B3LYP/6-31G* on geometries optimized at the same level
4. R=
s
1–5–p2*–7
s
1–6–p2*–7
Da
D1b
D2b
CN
COOMe
CCH
CH2OH
CH2CH3
CHCH2
10.50 (4.73)
11.93 (4.94)
14.53 (5.01)
11.40 (4.74)
14.24 (4.88)
16.01 (5.17)
9.51 (4.41)
8.81 (4.46)
7.77 (4.51)
9.82 (4.80)
8.37 (4.78)
7.60 (4.60)
0.99 (0.32)
3.12 (0.48)
6.76 (0.50)
1.58 (−0.06)
5.87 (0.10)
8.41 (0.57)
138.0 (135.9)
133.4 (135.9)
132.1 (135.5)
135.0 (135.8)
130.4 (135.1)
130.7 (135.3)
136.7 (136.3)
141.5 (136.3)
143.3 (136.8)
139.4 (136.1)
144.4 (136.8)
144.8 (137.0)
a D is the difference between s1–5–p*2–7 and s1–6–p* .
2–7
b D1 and D2 are dihedral angles C7ꢀC2ꢀC1ꢀC5 and C7ꢀC2ꢀC1ꢀC6, respectively.

8530
G. Mehta et al. / Tetrahedron Letters 42 (2001) 8527–8530
simple hydride model (as well as LiH transition state
model) at semi-empirical level constitutes an economi-
cal predictive tool for facial selectivities in nucleophilic
additions to sterically unbiased ketones and reinforces
our earlier3b proposals in this regard.
6. Substrates 4a and 4c–f were prepared from carbonyl
protected 4b5 through routine but non-trivial functional
group transformations and overall access to 4a–f was
certainly a very demanding endeavor.
7. All new compounds reported here were fully character-
1
ized on the basis of complementary spectroscopic (IR, H
and 13C NMR and MS) and analytical data. Except in
the case of 5c/6c and 5e/6e, the diastereomers 5a,b,d,f and
6a,b,d,f were separated and individually characterized.
Selected spectral data: 13C NMR l (75 MHz, CDCl3); 5a:
120.5, 70.1, 50.1, 43.7, 38.3, 37.3, 33.7. 6a: 121.7, 70.8,
51.0, 43.7, 37.8, 37.4, 35.4. 5b: 173.0, 71.4, 54.0, 51.7,
49.3, 42.2, 38.7, 33.3. 6b: 174.3, 72.0, 51.7, 50.7, 49.8,
42.4, 38.6, 37.7. 5c/6c: 100.6, 84.8, 71.8, 71.1, 68.7, 52.1,
51.6, 44.7, 44.6, 40.9, 38.2, 37.5, 37.3, 33.1, 29.7. 5d: 72.3,
61.0, 54.3, 46.9, 39.6, 39.4, 32.0. 6d: 72.4, 61.4, 50.1, 47.0,
39.5, 39.4, 36.4. 5e/6e: 72.9, 72.5, 54.3, 49.7, 48.8, 48.7,
41.0, 40.9, 39.9, 39.8, 36.4, 31.8, 20.1, 19.9, 13.5, 13.2. 5f:
136.9, 115.8, 72.1, 55.6, 50.1, 42.6, 39.3, 31.8. 6f: 137.4,
116.1, 72.7, 51.5, 50.3, 42.8, 39.3, 36.4.
Acknowledgements
R.S., U.D.P. and V.G. thank CSIR, UGC and
JNCASR, respectively, for research fellowships.
References
1. For recent reviews on diastereoselection, see a thematic
issue: Chem. Rev. 1999, 99, 1069–1480; (b) Mehta, G.;
Chandrasekhar, J. Chem. Rev. 1999, 99, 1437.
2. Mehta, G.; Khan, F. A. Tetrahedron Lett. 1992, 33, 3065.
3. (a) Mehta, G.; Khan, F. A. J. Am. Chem. Soc. 1990, 112,
6140; (b) Ganguly, B.; Chandrasekhar, J.; Khan, F. A.;
Mehta, G. J. Org. Chem. 1993, 58, 1734; (c) Mehta, G.;
Khan, F. A.; Ganguly, B.; Chandrasekhar, J. J. Chem.
Soc., Chem. Commun. 1992, 1711; (d) Mehta, G.; Ravikr-
ishna, C.; Ganguly, B.; Chandrasekhar, J. J. Chem. Soc.,
Chem. Commun. 1997, 75; (e) Mehta, G.; Ravikrishna,
C.; Kalyanraman, P.; Chandrasekhar, J. J. Chem. Soc.,
Perkin Trans. 1 1998, 1895; (f) Halterman, R. L.;
McEvoy, M. A. J. Am. Chem. Soc. 1990, 112, 6690; (g)
Ohwada, T. J. Am. Chem. Soc. 1992, 114, 8818; (h) Wipf,
P.; Kim, Y. J. Am. Chem. Soc. 1994, 116, 117678; (i)
Fraser, R. R.; Faibish, N. C.; Kong, F.; Bednarski, F. J.
Org. Chem. 1997, 62, 6164; (j) Li, H.; le Noble, W. J.
Recl. Trav. Chim. Pays-Bas 1992, 111, 199.
8. (a) Paddow-Row, M. N.; Wu, Y.-D.; Houk, K. N. J. Am.
Chem. Soc. 1992, 114, 10638; (b) Jeyaraj, D.; Yadav, A.
A.; Yadav, V. K. Tetrahedron Lett. 1997, 38, 4483.
9. Cieplack, A. S. J. Am. Chem. Soc. 1981, 103, 4540.
10. Frisch, M. J.; Trucks, G. W.; Schlegel, H. B.; Jones,
P. M. W.; Johnson, B. G.; Robb, M. A.; Cheeseman, J.
R.; Kheith, T.; Petersson, G. A.; Montgomery, J. A.;
Gaghavachari, M. A.; Al-Laham, M. A.; Zakrzewski, V.
G.; Ortiz, J. V.; Foresman, J. B.; Cioslowski, J.; Stefanov,
B. B.; Nanayakkara, A.; Challacombe, M.; Peng, C. Y.;
Ayala, P. Y.; Chen, W.; Wong, M. W.; Andres, J. L.;
Replogle, E. S.; Gomperts, R.; Martin, R. L.; Fox, D. J.;
Binkley, J. S.; Defrees, D. J.; Baker, J.; Stewart, J. P.;
Head-Gordon, M.; Gonzalez, C.; Pople, J. A. Gaussian
94: Gaussian, Inc., Pittsburgh, PA, 1995.
4. (a) Meinwald, J.; Crandall, J. K. J. Am. Chem. Soc. 1966,
88, 1292; (b) Wiberg, K. B.; Ubersax, R. W. J. Org.
Chem. 1972, 37, 3827.
5. Conti, P.; Kozikowski, A. P. Tetrahedron Lett. 2000, 41,
4053.
11. (a) Dewar, M. J. S.; Theil, W. J. Am. Chem. Soc. 1977,
99, 4899; (b) Dewar, M. J. S.; Zoebisch, Z.; Healy, E. F.;
Stewart, J. J. P. J. Am. Chem. Soc. 1985, 107, 3902.
12. NBO Version 3.1. Glendening, E. D.; Reed, A.; Carpen-
ter, E J. E.; Weinhold, F.