The tricyclo[2.1.0.02,5]pentan-3-one system: A new probe for the study of π-facial selectivity in nucleophilic additions

Article abstract of DOI:10.1016/S0040-4039(03)00515-X

Monosubstituted tricyclo[2.1.0.0^2,5]pentan-3-one derivatives have been synthesised and subjected to hydride reduction. Quite unexpectedly and in contrast to earlier observations in related systems, anti-selectivity has been encountered in these substrates. Computational studies employing various models reproduce the observed facial preference and indicate that the causative factor for the anti-preference could be the polarization of the C1-C5 strained σ bond.

Full text of DOI:10.1016/S0040-4039(03)00515-X

TETRAHEDRON
LETTERS
Pergamon
Tetrahedron Letters 44 (2003) 3101–3104
The tricyclo[2.1.0.02,5]pentan-3-one system: a new probe for the
study of p-facial selectivity in nucleophilic additions
Goverdhan Mehta,a,* S. Robindro Singh,a U. Deva Priyakumarb and G. Narahari Sastryb,*
aDepartment of Organic Chemistry, Indian Institute of Science, Bangalore 560 012, India
bMolecular Modelling Group, Organic Chemical Sciences, Indian Institute of Chemical Technology, Hyderabad 500 007, India
Received 14 January 2003; revised 12 February 2003; accepted 21 February 2003
Abstract—Monosubstituted tricyclo[2.1.0.02,5]pentan-3-one derivatives have been synthesised and subjected to hydride reduction.
Quite unexpectedly and in contrast to earlier observations in related systems, anti-selectivity has been encountered in these
substrates. Computational studies employing various models reproduce the observed facial preference and indicate that the
causative factor for the anti-preference could be the polarization of the C1ꢀC5 strained s bond. © 2003 Elsevier Science Ltd. All
rights reserved.
Control of diastereoselectivity during nucleophilic addi-
tions to carbonyl groups is a key issue in stereogenesis.
It is now well recognised that both steric and long
range electronic effects can profoundly influence p-face
selection during addition to the carbonyl group.1 While
the role of steric effects in determining face-selectivity is
quite predictable, the precise nature, effectiveness and
predictability of remote electronic effects in determining
p-face selectivity is still a matter of ongoing scrutiny
and debate.1,2 Efforts from our group and of others
over the past decade have focussed on studying systems
where the two faces of the carbonyl group are virtually
in an isosteric environment but are amenable to long
range electronic perturbation.3 These approaches have
enabled the segregation of steric effects from electronic
effects and firmly established the role of the latter in
influencing p-face selection.3,4 For example, 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-substi-
tuted-9-nor snoutanone 33d and 5-exo-substituted-
bicyclo[2.1.1] hexan-2-ones 4,4 where the carbonyl
group is in a sterically neutral disposition, distal sub-
stituents (R) can significantly influence the stereochemi-
cal outcome (syn- versus anti-addition). The issue of
concern now is the delineation of the precise nature of
the electronic effects operating in these systems. Several
explanations based on hyperconjugative interactions at
the transition state (Cieplak effect), electrostatic effects,
various orbital mixing/tilting effects and cation com-
plexation, among others have been proffered to explain
the various experimental data.1–5 A scrutiny of the
available experimental and computational data reveals
that many of these electronic effects operate simulta-
neously, within a narrow energy range, either co-opera-
tively or in opposition and their cumulative effect
determines the observed p-face selectivities. Thus, eluci-
dation and quantification of the subtle role of the
various electronic factors that determine facial selectiv-
ity is still a challenge that mandates continued search
and study of newer probe systems. As part of our
continuing efforts in the area, we introduce tricy-
clo[2.1.0.02,5]pentan-3-one 5 as a new probe system
wherein p-facial discrimination is introduced through
the remote C-1 substituent (R).
Besides having an isosteric environment around the
carbonyl group as revealed by high level calculations
and crystal structure data (vide infra), the overlay
diagram (6) of 5 (R=CN, red) with the parent bicy-
clo[1.1.1]pentan-2-one (black) and its endo-4-cyanobicy-
clo[1.1.1]pentan-2-one derivative (blue) indicates that
the skeleton of 5 is much more strained (cf. 1–4) and
the C1 substituent does not come in the way of the
trajectory of the approaching nucleophile. Interestingly,
* Corresponding authors. E-mail: gm@orgchem.iisc.ernet.in
0040-4039/03/$ - see front matter © 2003 Elsevier Science Ltd. All rights reserved.
doi:10.1016/S0040-4039(03)00515-X

3102
G. Mehta et al. / Tetrahedron Letters 44 (2003) 3101–3104
the electronic effects of the C1 substituent in 5 are
transmitted through the connecting cyclopropane
bonds. Further, the stereo-differentiating C1 and C5
carbons in 5 are connected through a unique bond
which is the central bond of the bicyclo[1.1.0]butane
moiety embedded in it (see bold). Thus, a study of face
selection in derivatives of 5 was of intrinsic interest and
we wish to report here the results of experimental and
computational studies on this system.
Figure 1. ORTEP diagram of 5b.
Our initial task was to access derivatives of 5. However,
a literature search revealed that C1 monosubstituted
derivatives of tricyclo[2.1.0.02,5]pentan-3-one 5 are not
Scheme 3.
known.6 Therefore, a new synthesis of the C1 monosub-
stituted tricyclo[2.1.0.02,5]pentan-3-ones was developed
as shown in Scheme 1 and was based on earlier
approaches to this ring system.7 We selected three
monosubstituted derivatives 5a–c for the present study.
Careful addition of tert-butyl diazoacetate to an excess
of TMS-protected 2-propynyl acetate 7 in the presence
of dirhodium(II) tetraacetate catalyst resulted in con-
trolled nitrogen evolution and formation of cyclo-
propene 8.8 Protodesilylation and hydrolysis of the
ester group in 8 led to cyclopropene carboxylic acid 9
(Scheme 1). Carboxylic acid 9 was elaborated to the
a-diazoketone 10 for an intramolecular [2+1]-
cycloaddition. Decomposition of 10 in the presence of
the Rh2(OAc)4 catalyst furnished the tricyclic ketone 11
which was further hydrolysed to the hydroxymethyl
derivative 128 (Scheme 1). The hydroxymethyl bearing
tricyclic ketone was elaborated to the desired deriva-
tives 5a–c as shown in Scheme 2. These transformations
were devised to avoid any carbonyl group protecting
manoeuvres in view of the extreme sensitivity and
volatility of the substrates. At this stage an X-ray
crystal structure determination of 5b was carried out
(Fig. 1)9 to secure the structures and confirm that the
two faces of the carbonyl group were in a near iso-steric
environment. Tricyclic ketones 5a–c were subjected to
sodium borohydride reduction to furnish (E)-13a–c and
(Z)-14a–c alcohols in nearly quantitative yields
(Scheme 3). The observed diastereoselectivities (E:Z
ratio) are displayed in the Scheme and were determined
Scheme 1. Reagents and conditions: (a) N2CHCOOtBu,
Rh2(OAc)4, rt 50–60%; (b) TBAF, THF, 0°C, 2 h, 75%; (c)
TFA, 0°C, 1.5 h, 80%; (d) i. (COBr)2, ether, 0°C, 4 h; ii.
CH2N2, ether, −78°C, 24 h, 50% (two steps); (e) Rh2(OAc)4,
CHCl3, 60°C, 1 h, 30%; (f) K2CO3, MeOH, rt, 4 h, 85%.
Scheme 2. Reagents and conditions: (a) PDC, CH2Cl2, 4 h,
90%; (b) i. NH2OH·HCl, py, CH2Cl2, 1 h; ii. TsCl, py, 0°C–rt,
36 h, 50% (two steps); (c) i. RuO2–NaIO4, acetone–H2O (1:1),
2 days; ii. CH2N2, 0°C, 15 min 50% (two steps); (d) CH3I,
Ag2O, CH2Cl2, 2 days, 85%.
1
through H NMR analyses.

G. Mehta et al. / Tetrahedron Letters 44 (2003) 3101–3104
3103
the B3LYP/6-31G* level of theory.12 Interestingly, all
five models employed in the present study (see Tables 1
and 2) predict addition from the anti-face in agreement
with the experimental results.
The stereostructures of 13a–c and 14a–c were unam-
biguously determined on the basis of the relative
deshielding (ca. 0.2 ppm) of the H(5) protons in the
(E)-alcohols 13a–c compared to the (Z)-alcohols 14a–c.
Additionally, the H(5) proton in (E)-13a–c appeared as
a diagnostic doublet (J=ꢀ7.5 Hz) due to long range (4
bond) coupling with the syn-H(3) proton and could be
readily recognised.
The unexpected and seemingly contra-intuitive
diastereoselection observed in the case of 5a–c may be
attributed to charge polarization induced by an elec-
tron-withdrawing substituent on the central s bond of
the bicyclobutane moiety (see bold in 5). Thus, the
polarized C1ꢀC5 bond renders a l+ on C-5 to facilitate
the anti attack of the nucleophile.
The stereoselectivities observed during hydride reduc-
tion of 5a–c exhibit a small preference for the anti-face
addition but this result is in contrast with the trend
observed earlier with related systems.1–4 We have con-
sistently encountered syn face preference of the remote
electron withdrawing substituents such as cyano and
ester in the systems 1–4, among others, studied so far.3
To understand the underlying reasons for this unex-
pected deviation, tricyclic ketones 5a–c were studied
computationally employing five different models.
Orbital and electrostatic effects were assessed employ-
ing the hydride and charge models as described earlier,
i.e. by placing an H− ion and a negative point charge,
The high preference for anti-selectivity in the charge
model (Table 1) may be directly traced to the overrid-
ing electrostatic influence, effectively countering the
opposing orbital interactions. The LiHTS model and
hydride models (Table 1) also reproduce the observed
anti-selectivity but the small magnitude of such prefer-
ence is perhaps more realistic. The NBO analysis
(except in 5c) and cation complexation model calcula-
tions summarized in Table 2 also support the anti-pref-
erence observed in 5a–c.
,
respectively, at a distance of 1.4 A away from the
carbonyl carbon along the trajectory perpendicular to
the p-plane.3b The LiH transition states (Table 1) were
characterized as saddle points through geometry opti-
mizations followed by frequency calculations.5b
Semiempirical calculations were performed using the
AM1 Hamiltonian.10 The NBO analysis11 and cation
complexation models (Table 2)5c were investigated at
If the contention that the anti-selectivity observed in
5a–c is due to the polarization of the central cyclobu-
tane bond C1ꢀC5 is valid, then the removal of this
bond should restore the commonly observed syn-prefer-
ence. Indeed, we tested all the above computational
models with the model compound endo-4-cyanobicy-
clo[1.1.1]pentan-2-one and found complete reversal and
prediction of the expected syn-selectivity. Efforts are
underway to experimentally validate this prediction.13
Table 1. The relative energy for syn and anti face addi-
tions calculated using the charge, hydride and LiHTS
models at AM1 level of theory.a All values are given in
kcal/mol
In summary, we have devised a synthesis of 1-substi-
tuted tricyclo[2.1.0.02,5]pentan-3-ones 5a–c, with the
carbonyl group positioned in a near iso-steric environ-
ment, and introduced these substrates as a new probe
system for studying p-face selectivity during nucle-
ophilic additions. The small anti-preference observed
for the hydride addition to 5a–c is quite unexpected and
a departure from earlier observations in related sys-
tems. Computational studies reproduce the observed
selectivities and indicate that polarization of the C1ꢀC5
bond and the resulting electrostatic interaction as the
possible causative factor.
Structure
Charge
anti
Hydride
LiHTS
anti
syn
syn
anti
syn
5a
5b
5c
12.21
9.13
4.73
0.00
0.00
0.00
0.61
0.76
0.06
0.0
0.00
0.00
1.18
1.72
0.40
0.00
0.00
0.00
a A value of 0.0 denotes the preference of the corresponding face
addition.
Table 2. The principal dihedral angles (in degrees) in the
proton complexed reactanta,b and interaction energy (kcal/
mol) of the s bond antiperiplanar to the incipient CꢀH
bond in the syn and anti sides of 5 and the p*CꢁO of the
reactant obtained at the B3LYP/6-31G* level
Acknowledgements
R.S. and U.D.P. thank CSIR and UGC, respectively,
for the award of research fellowships.
Comp.
syn
D2
anti
D4
NBO
anti
9.90
D1
D3
syn
References
5a
5b
5c
123.5
119.8
119.8
121.2
116.6
116.0
177.9
173.7
173.1
175.7
171.2
170.8
13.80
13.32
12.11
10.66
12.74
1. For recent reviews on diastereoselection, see a thematic
issue: (a) 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.;
a D1, D2, D3 and D4 are the dihedral angles Ú6-3-4-1, Ú6-3-2-1,
Ú6-3-4-5 and Ú6-3-2-5, respectively.
b If D1>D3 and D2>D4, syn attack is preferred; if D3>D1 and
D4>D2, anti attack is preferred.

3104
G. Mehta et al. / Tetrahedron Letters 44 (2003) 3101–3104
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; (k) Mehta,
G.; Gagliardini, V.; Priyakumar, U. D.; Sastry, G. N.
Tetrahedron Lett. 2002, 43, 2487.
CDCl3): l 183, 63.7, 58.4, 39.5 (2C), 10.5, 2.9; Mass: m/z
1
147 (M++Na). 14a: IR (cm−1) 3397, 2226; H NMR (300
MHz, CDCl3): l 4.22 (d, J=10.2 Hz, 1H), 4.0 (s, 1H),
2.76 (d, J=10.2 Hz, 1H), 2.64 (s, 2H); 13C (75 MHz,
CDCl3): l 116.1, 86.4, 40.1 (2C), 13.19, 8.77; Mass: m/z
1
130 (M++Na). 14b: IR (cm−1) 1714, 3415; H NMR (300
MHz, CDCl3): l 4.11 (s, 1H), 3.75 (s, 3H), 3.69 (s, 1H),
2.69 (s, 2H); 13C (75 MHz, CDCl3): l 170.9, 84.3, 51.9,
40.1 (2C), 24.4, 16.3; Mass: m/z 141 (M++1). 13a: IR
1
(cm−1) 3394, 2226; H NMR (300 MHz, CDCl3): l 4.48
(t, J=7.5 Hz, 1H), 4.17 (d, J=6.6 Hz, 1H), 2.61 (s, 2H),
2.44 (d, J=9.3 Hz, 1H); 13C (75 MHz, CDCl3): l 115.6,
86.9, 39.2 (2C), 25.5, −2.78; Mass: m/z 130 (M++Na).
1
13b: IR (cm−1) 1714, 3414; H NMR (300 MHz, CDCl3):
l 4.3 (m, 1H), 3.85 (d, J=7.5 Hz, 1H), 3.76 (s, 3H), 2.63
(s, 2H), 2.32 (s, 1H); 13C (75 MHz, CDCl3): l 169.6, 86.0,
52.0, 39.2 (2C), 28.0, 12.8; Mass: m/z 141 (M++1). 14c:
IR (cm−1) 3398; 1H NMR (300 MHz, CDCl3), l 4.1 (s,
3H), 3.5 (s, 3H), 3.2 (s, 1H), 2.0 (s, 2H); 13C (75 MHz,
CDCl3) l 85.2, 68.1, 58.17, 32.9 (2C), 27.2, 4.5.
4. Mehta, G.; Singh, S. R.; Gagliardini, V.; Priyakumar, U.
D.; Sastry, G. N. Tetrahedron Lett. 2001, 42, 8527.
5. (a) Cieplak, A. S. J. Am. Chem. Soc. 1981, 103, 4540; (b)
Paddow-Row, M. N.; Wu, Y.-D.; Houk, K. N. J. Am.
Chem. Soc. 1992, 114, 10638; (c) Jeyaraj, D.; Yadav, A.
A.; Yadav, V. K. Tetrahedron Lett. 1997, 38, 4483.
6. Levin, M. D.; Kaszynski, P.; Michl, J. Chem. Rev. 2000,
100, 169.
9. Crystal data for 5b: Structure was solved by direct meth-
ods (SIR92). Refinement was by full-matrix least-squares
procedures on F2 using SHELXL-97. Crystal system:
triclinic, space group: P-1, cell parameters: a=5.6956(22),
7. (a) Doering, W.v. E.; Pomerantz, M. Tetrahedron Lett.
1964, 5, 961; (b) Maier, G.; Resinauer, H. P.; Freitag, H.
A. Tetrahedron Lett. 1978, 19, 121; (c) Dowd, P.; Garner,
P.; Schappert, R.; Irngartinger, H.; Goldman, A. J. Org.
Chem. 1982, 47, 4240; (d) Irngartinger, H.; Reimann, W.;
Garner, P.; Dowd, P. J. Org. Chem. 1988, 53, 3046.
8. All new compounds reported here were fully character-
,
b=7628(30), c=7.8045(30) A, h=70.62(0), i=88.50(1),
3
,
k=87.93(1)°, V=325.27(22) A , Z=2, z(calcd)=1.4103
g cm−3, F(000)=144, v=1.117 mm−1, u=0.71073 A.
,
Total number of l.s. parameters=115. R1=0.0371 for
Fo>4|(Fo) and 0.0427 for all 1286 data. wR2=0.1016,
GoF=1.052, Restrained GoF=1.052 for all data. An
ORTEP drawing of compound 5b with 50% ellipsoidal
probability has been displayed. Crystallographic data has
been deposited with the Cambridge Crystallographic
Data Centre (Reference number 203637).
1
ized on the basis of complementary spectroscopic (IR, H
and 13C NMR and MS) and analytical data. Except in
the case of the 13c, all the diastereomers were separated
and individually characterized. Selected spectral data. 8:
IR (cm−1) 1751, 1722; 1H NMR (300 MHz, CDCl3): l
5.10 (1/2ABq, J=16 Hz, 1H), 5.02 (1/2ABq, J=16 Hz,
1H), 2.10 (s, 4H), 1.37 (s, 9H), 0.20 (s, 9H); 13C (75 MHz,
CDCl3): l 175.0, 170.3, 122.1, 108.2, 79.5, 59.4, 28.0,
22.5, 20.7, −1.7; Mass: m/z 241 (M+−Ac), 211 (M+−
SiMe3). 9: IR (cm−1) 3148, 1784, 1743, 1698; 1H NMR
(300 MHz, CDCl3): l 6.71 (s, 1H), 5.06 (brs, 2H), 2.33 (s,
1H), 2.12 (s, 3H); 13C (75 MHz, CDCl3): l 181.5, 170.3,
110.3, 97.8, 57.5, 20.5, 20.0; Mass: m/z 111 (M+−CO2H),
10. Dewar, M. J. S.; Zoebisch, Z.; Healy, E. F.; Stewart, J. J.
P. J. Am. Chem. Soc. 1985, 107, 3902.
11. NBO Version 3.1: Glendening, E. D.; Reed, A.; Carpen-
ter, J. E.; Weinhold, F.
12. Gaussian 98, Revision A.11.2, Frisch, M. J.; Trucks, G.
W.; Schlegel, H. B.; Scuseria, G. E.; Robb, M. A.;
Cheeseman, J. R.; Zakrzewski, V. G.; Montgomery, Jr.,
J. A.; Stratmann, R. E.; Burant, J. C.; Dapprich, S.;
Millam, J. M.; Daniels, A. D.; Kudin, K. N.; Strain, M.
C.; Farkas, O.; Tomasi, J.; Barone, V.; Cossi, M.;
Cammi, R.; Mennucci, B.; Pomelli, C.; Adamo, C.; Clif-
ford, S.; Ochterski, J.; Petersson, G. A.; Ayala, P. Y.;
Cui, Q.; Morokuma, K.; Rega, N.; Salvador, P.; Dannen-
berg, J. J.; Malick, D. K.; Rabuck, A. D.; Raghavachari,
K.; Foresman, J. B.; Cioslowski, J.; Ortiz, J. V.; Baboul,
A. G.; Stefanov, B. B.; Liu, G.; Liashenko, A.; Piskorz,
P.; Komaromi, I.; Gomperts, R.; Martin, R. L.; Fox, D.
J.; Keith, T.; Al-Laham, M. A.; Peng, C. Y.; Nanayak-
kara, A.; Challacombe, M.; Gill, P. M. W.; Johnson, B.;
Chen, W.; Wong, M. W.; Andres, J. L.; Gonzalez, C.;
Head-Gordon, M.; Replogle, E. S.; Pople, J. A. Gaus-
sian, Inc., Pittsburgh PA, 2001.
1
114 (M++1−Ac). 11: IR (cm−1) 1782, 1744; H NMR (300
MHz, CDCl3): l 5.04 (s, 2H), 4.17 (s, 1H), 2.22 (s, 2H),
2.11 (s, 3H); 13C (75 MHz, CDCl3): l 182.5, 170.7, 56.2,
40.1 (2C), 20.7, 11.0, 3.4; Mass: m/z 153 (M++1). 12: IR
1
(cm−1) 3401, 1763; H NMR (300 MHz, CDCl3): l 4.65
(s, 2H), 4.15 (s, 1H), 2.20 (s, 2H); 13C (75 MHz, CDCl3):
l 183.5, 54.7, 39.2 (2C), 13.6, 3.6; Mass: m/z 111 (M++1).
1
5a: IR (cm−1) 2241, 1805; H NMR (300 MHz, CDCl3):
l 4.74 (s, 1H), 2.8 (s, 2H); 13C (75 MHz, CDCl3): l 177.3,
1
111.7, 46.6 (2C), 29.6, 7.6. 5b: IR (cm−1) 1794, 1729; H
NMR (300 MHz, CDCl3): l 4.53 (s, 1H), 3.85 (s, 3H),
2.68 (s, 2H); 13C (75 MHz, CDCl3): l 179.7, 166.1, 52.8,
44.0 (2C), 10.6, 8.6; Mass: m/z 107 (M+−OMe). 5c: IR
(cm−1) 1778; 1H NMR (300 MHz, CDCl3): l 4.43 (s, 2H),
4.14 (s, 1H), 3.45 (s, 3H), 2.2 (s, 2H); 13C (75 MHz,
13. Unpublished results.