411
Journal of Molecular Structure, 142 (1986) 411-415 Elsevier Science Publishers B.V., Amsterdam -Printed
STRUCTURAL
AND CONFORMATIONAL
in The Netherlands
STUDY OF AZABICYCLANONES.
E. GALVEZ? I. ARDID! L.FUENTESj F. FLORENCIO: S. GARCIA 1 Dpto. Qulmica Orgdnica. Univ. Alcald de Henares. 2 Inst. QuImica-Flsica. "Rocasolano". C.S.I.C. Madrid.
BLANCO?
ABSTRACT 3-Phenethyl-3-azabicyclo(3.2.l.)octan-8-one (I), 3-Phenethyl-3-azabicyclo (3.3.l)nonan-g-one (II), and 8-Phenethyl-8-azabicyclo(4.3.l)decan-lo-one (III) have been studied by k, uC NMR and IR spectroscopy and the crystal structure of compound II has been determined by X-ray diffraction. The ketones studied adopt. in CDCl solution a flattened chair conformation in the piperidine ring. This flattentng increases from I to III. This fact is due to the increasing steric ef feet exerted by the polimethylene chain. X-ray data for compound II have revealed that the compound II has crystallized in a flattened chair-chair conformation.
INTRODUCTION In a previous
paper
(ref.1) we reported
study of diazabicyclanones
and diazabicyclanols.
this paper the structural.and conformational
sis of I-III
(ref. 2)
cycloalkanone clanone
Scheme
the structural
is shown in Scheme
with formaldehyde
and
and conformational
In the same line,
study of compounds
1. From the reaction
a-phenethylamine,
I-III.
we report in The synthe
of the suitable
the corresponding
azabicy
is obtained.
1
+
HCHO
+
PhCH2CH2NH2
n= 2, I n= 3, II n= 4, III EXPERIMENTAL IR spectra were recorded were compressed a Bruker_WM360 Varian
on a Perkin Elmer 599 spectrophotometer. All canpeunds 1 H NMR spectra were obtained at 360 MHz with 13 spectrometer. C NMR spectra were determined at 20 MHz with the into KBr
pellets.
FT 80 in the Fourier transform
CDC13 using TMS as internal
0022-2S60/36/$03.50
mode. All
of the spectra were obtained
reference.
0 1986 Elsevier Science Publishers B.V.
in
412 A prismatic crystal of 0.10 x 0.15 x 0.30 mm was used to determine the cell parameters in a Philips PN 1100 four circle diffractometer.Lattice parameters were refined by a least-squaresfit of 25 reflections. Intensity data were collected from the same crystal in the same diffractometer with graphite-monochromatedCut& radiation for 2te<65 h2a
, Max hkl 12 15 14. The
scan technique was used. Of the 2422 reflections measured, 1670 was consid o being determined from counting statistics.
ered as observed with I >20 (I), The crystal data are given
in Table 1.
RESULTS AND DISCUSSION Description and discussion of the structure Figure 1 shows a view of the molecule and the numberings for the crystallographic study. Bond lengths, valence and torsion angles are given
in Table 2.
TABLE 1 Crystal dataa :'%27(l)A = Ii 451(1)A ,b= 11:939(1)A s= 103.13(1)Q Space group
C16H21No
P21lc
aStandard deviations, given
V = 1422.6(8) i3 2=4 -3 D = l.l36(2)Mg m F'(OO0) = 528 !J=5.115 hMoKa = 1.5418
in parentheses, refer to the least significant
digits.
Fig. 1 Perspective view and numbering of compound II.
413 TABLE 2 Bond distances
( h )
Cl -c2 Cl - c9 N3 - c4
Cl - C8 C2 - N3 N3 - Cl1
l-522(6) 1.490(5) 1.452(5)
;; : ;;
;;
C7 - C8 Cl1 - Cl2 Cl3 - Cl4 Cl4 - Cl5 Cl6 - Cl7
::2--'::3 Cl3 - Cl8 Cl5 - Cl6 Cl7 - Cl8
1.381(6)
c2 - Cl - c9
107-l(3)
1.352(7)
Bond angles
C8 - Cl ;; : ;; C4 - N3 - c5 :: - c5 C6 - C7 ;; I ;; Cl1 - Cl2 Cl2 - Cl3 Cl3 - Cl4 Cl5 - Cl6 Cl3 - Cl8
(')
C9 C8 Cl1 Cl1 c9 c9 C8 c5 010 - Cl3 - Cl4 - Cl5 - Cl7 - Cl7
;: : ;; : ;; N3 C4 C5 Cl c5
-
c4 C5 C6 C8 c9
c5 C6 C7 C7 010 - Cl2 !:2--?;3 - Cl8 Cl4 - Cl3 - Cl8 Cl4 - Cl5 - Cl6 Cl6 - Cl7 - Cl8
112.4(4)
The N3 . ..C7 distance (2.62 1
: ;;
(2.905(5) A
) (ref. 3) between the 3 and 7 positions.
0.715(4)
8, so that the piperidine In the cyclohexane
square plane through the cyclohexane phenethyl
the molecules
The displacements
ring adopts a slightly
ring, the displacements
ring adopts also a slightly the equatorial
in the crystal
takes place through
and
chair confor-
of C7 and C9 from the least and 0.710(4)
flattened
position.
flattened
distance
of N3 and
Cl, C2, C4, C5, are -O-633(3)
Cl, C5, C6, C8 are -O-543(5)
group occupies
125.2(3) 113.1(3) 120.6(4) 116.9(3) 120.3(4) 120.0(4)
) is largest than the theoretical
C9 from the least square plane through
mation.
-
A
consequently,
chair conformation.
In compound
The
II the packing of
Van der Waals forces.
JR spectra According bands
to the crystal
in the infrared
the axially
oriented
compound
(2850-2600
C - H bonds
(ref. l).The spectroscopy compound
structure,
spectra
in a positions
behavioyr
of compounds
II in the 2850-2600 cm region. -1 1760, 1740, 1730 cm respectively.
II show characteristic
Bohlmann
cm-'). These bands are originated
The
in relation I and III
by
to the nitrogen atuns
are similar to that of
u(C=O) bands of I-III are at
chemical
61.82
45.35
48.75 47.95
I
ka
20.91
C 7
I-III
for compound
reasons, the numbering
aFor homogeneity
34.79
C 6(8)
at 20 MHz. Solvent CDC13.
22.65
C 6(7)
Spectra recorded
59.80 60.42
C 2(4)
C l(5)
(ppm) for compounds
Compound
shifts
chemical
Carbon-13
TABLE 4
H 6(Veq 1.9 m
1.8 m
H Wax
C 6(9)
III
26.54
C 7(8)
is altered.
31.94
1.38 dtt
H 7eq
‘J 13 ‘J 3
2m
H 7ax
CHP
217.94 213.29 58.71 59.20
219.64 57.1
C=O
1.30 m
33.99 33.95
34.0
CH26
2.8 t 3J 7.5
7.81-t )J 7.5
<;7; ;
CH2a
128.61 128.57
128.60
ortho
7.15-7.3
7.18-7.32m
para
C-ipso
t, triplet
2.61 t U 7.7
2.56 t
128.28 125.98 128.29 125.96 140.37 140.25
m
7.18-7.30m
Ph
128.26 125.96 140.34
meta
CH26 2.70 t
m, multiplet;
H 7Weq
1.79 m
H 7(8jax
of doublets;
1.79 m
H 6(9jeq
1.54 m
H 6(9)ax
br, broad; dd, doublet
2.11 dd
H 6Weq
2.0 m ‘J 13.29 ‘J 2.2
H 6(8J,,
(J, Hz) for compounds I-ITT
CDC13. Abbreviations:
2.87 d ‘J 11.31
3t.23 d J 10.88
3.03 d
Solvent
2.43 dd ‘J 11.62 ‘J 2.4
at 360 MHz.
WI/2 17
2.59 brs
Spectra recorded
:IIa
I
111a
II
dd ;J 10 52
2.6
WI/2 10 2.35 brs
WI/2 9
2.56 dd
2.15 brs
I
H 2(41eq
( 6, ppm) and multiplicities
H 2(41ax
shifts
H l(5)
Compound
'H NMR
TABLE 3
415 NMR Spectra The 'H and l3C NMR data of I-III are summarized in Tables 3 and 4 respectively. 13 From the 'H and C NMR data of I-III, the following general features were deduced:
(a) In CDC13 solution
formation; exerted
(b) This flattening
by the polimethylene
atom adopts
an equatorial
The above statements compounds electron
attributed coplanar
to
In compound
pounds
are substantiated signals
o-electron
attached
as follows.
correspond
to the nitrogen
delocalization
In the 'H NMR spectra
of
to protons gauche to the nitrogen
appears
at higher field which
of the nitrogen
is
lone pair in trans-
In II and III, J H2 4 ax is greater than J H2 4 eq;co"sequefltlY
,
angle H2,4 eq- C - C - H,_5 is greater II theAsH
effect exerted
chair con-
from I to III due to the steric effect
(c) the radical
(ref. 1); H 2(4) ax signals
C-H bonds.
the dihedraL
increases
chain;
ring adopts a flattened
position.
I-III, H 2(4)eq pairs
the piperidine
than H2,4 ax- 'C - C - H, 5.
(7)ax -6H (7),; 0.6 ppm is attributed
by the nitrogen
to the deshieldini
lone pair (ref. 1). It is also observed
in com-
I and III.
The sequence increased
SC (2,4) (I)>sC (2,4) (II)> SC (2,4) (III) is consistent
eclipsing
flattening
between
the H 2(4)ax-
from I to III in the piperidine
The N-CH2- aI3 C chemical equatorial
position
H l(5) as a consequence
to the
of the increased
ring.
shifts are consistent
with a phenethyl
group
in an
(ref. 1).
CONCLUSIONS From X-ray diffraction, concluded mational
IR, 'H and l3C data of compounds
that these compounds
occupy
space in both solutions
approximately
and the crystalline
I-III it can be
the same region of conforstate.
ACKNOWLEDGEMENTS We thank the Comisi6n for partial
Asesora
de Investigacidn
Cientifica
y Tecnica
(Grant1750)
support of this research.
REFERENCES
1 E. Galvez, M.S. Arias, J. Bellanato, J.V. Garcia-Ramos, Verdier, S. Garcia-Blanco, J. Mol. Str., 127 (1985) 185. 2 I. Ardid, unpublished results. 3 N. C. Webb, M. R. Becker, J. Chem. Sot. B (1976) 1317.
F. Florencio,
P. Smith